{"title":"Micro \/ Nano Optics","description":null,"products":[{"product_id":"vrf1-355","title":"VRF1-355 Quartz Vortex Retarder 355nm UVFS","description":"\u003cp\u003eThe Quartz Vortex Retarder is fabricated on a UVFS substrate by utilizing internally induced birefringent micro?nano structures within quartz. It comes as a 1?inch single?substrate bare chip without housing.\u003c\/p\u003e\u003cp\u003eInside the substrate, the fast?axis orientation of the birefringent microstructure features continuous azimuthal rotation. A uniform ¦Ë\/2 retardance is maintained across the full aperture of the device, making it a single?wavelength component.\u003c\/p\u003e\u003cp\u003eThe Quartz Vortex Retarder features polarization?dependent optical properties. Subject to the polarization state of the incident beam, it generates vortex beams with helical wavefronts for circularly polarized incidence (with reversed handedness of output circular polarization); vector?polarized beams will be produced when illuminated by linearly polarized light.\u003c\/p\u003e\u003cp\u003eCompared with conventional spiral phase plates, the quartz vortex retarder generates vortex beams efficiently via delicate polarization manipulation with greater flexibility. Its flat?plate configuration has no physical relief profiles and facilitates easy integration. Unlike liquid?crystal?based vortex retarders, it works for ultraviolet spectral range. Thanks to the substrate material, it delivers a high damage threshold under ultraviolet irradiation.\u003c\/p\u003e\u003cp\u003eoffers standard Quartz Vortex Retarders with operating wavelength ¦Ë of 355?nm and topological charge m of 1. Flexible specification customization is available to satisfy diverse requirements across various application scenarios.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eFused Silica\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾92 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e355 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e10¡Á10 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼5 arcsec\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657155465402,"sku":"VRF1-355","price":29630.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/66aa1630ae50480a92055bd7e1d91997.jpg?v=1789617630"},{"product_id":"vr1-405","title":"VR1-405 True Zero Order Polymer Vortex Half Wave Retarder 405nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003eRavg£¼0.5 %@400-700 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾85 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e405 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657155793082,"sku":"VR1-405","price":6500.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/4482562b0f6e45a1871b2c502436df64.jpg?v=1789617630"},{"product_id":"vr1-442","title":"VR1-442 True Zero Order Polymer Vortex Half Wave Retarder 442nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003eRavg£¼0.5 %@400-700 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾93 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e442 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657156153530,"sku":"VR1-442","price":6500.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/2e5ac907eb8f4bc28daa29c69e0ae1e5.jpg?v=1789617632"},{"product_id":"vr1-488","title":"VR1-488 True Zero Order Polymer Vortex Half Wave Retarder 488nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003eRavg£¼0.5 %@400-700 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾96 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e488 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657156251834,"sku":"VR1-488","price":6500.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/6557ed72944446efb4683920805ffd43.jpg?v=1789617632"},{"product_id":"vr1-520","title":"VR1-520 True Zero Order Polymer Vortex Half Wave Retarder 520nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003eRavg£¼0.5 %@400-700 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾97 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e520 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657156710586,"sku":"VR1-520","price":6500.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/b00082561ac249dda936d905b52cb4ce.jpg?v=1789617634"},{"product_id":"vr1-532","title":"VR1-532 True Zero Order Polymer Vortex Half Wave Retarder 532nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003eRavg£¼0.5 %@400-700 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾97 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e532 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657157038266,"sku":"VR1-532","price":6728.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/8052014c38ac46c0beb6015a723eab68.jpg?v=1789617635"},{"product_id":"vr1-633","title":"VR1-633 True Zero Order Polymer Vortex Half Wave Retarder 633nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003eRavg£¼0.5 %@400-700 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾98 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e633 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657157136570,"sku":"VR1-633","price":6728.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/9478909225e148f297b57ee74518dcf0.jpg?v=1789617634"},{"product_id":"vr1-670","title":"VR1-670 True Zero Order Polymer Vortex Half Wave Retarder 670nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003eRavg£¼0.5 %@400-700 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾98 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e670 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657157398714,"sku":"VR1-670","price":6500.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/24ccd229342f45958e4a91de924360d2.jpg?v=1789617636"},{"product_id":"vr1-780","title":"VR1-780 True Zero Order Polymer Vortex Half Wave Retarder 780nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003eRavg£¼0.5 %@700-1100 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾98 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e780 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657157693626,"sku":"VR1-780","price":6728.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/b78682ed158f400ca809e4f467b98361.jpg?v=1789617639"},{"product_id":"vr1-795","title":"VR1-795 True Zero Order Polymer Vortex Half Wave Retarder 795nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003eRavg£¼0.5 %@700-1100 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾98 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e795 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657157759162,"sku":"VR1-795","price":6500.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/f51a8e45265b4e0c8b64f48e6a7eca95.jpg?v=1789617637"},{"product_id":"vr1-808","title":"VR1-808 True Zero Order Polymer Vortex Half Wave Retarder 808nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003eRavg£¼0.5 %@700-1100 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾98 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e808 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657158480058,"sku":"VR1-808","price":6500.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/06e8218b0b8b40c88976534c5a52b227.jpg?v=1789617637"},{"product_id":"vr1-850","title":"VR1-850 True Zero Order Polymer Vortex Half Wave Retarder 850nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003eRavg£¼0.5 %@700-1100 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾98 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e850 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657158807738,"sku":"VR1-850","price":6500.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/0cc8b818365744508104c80d591de375.jpg?v=1789617639"},{"product_id":"vr1-980","title":"VR1-980 True Zero Order Polymer Vortex Half Wave Retarder 980nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003eRavg£¼0.5 %@700-1100 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾98 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e980 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657158873274,"sku":"VR1-980","price":6728.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/024b001bcfe04d458516267e172f35f4.png?v=1789617640"},{"product_id":"vr1-1030","title":"VR1-1030 True Zero Order Polymer Vortex Half Wave Retarder 1030nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003eRavg£¼0.5 %@700-1100 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾98 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e1030 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657158938810,"sku":"VR1-1030","price":6500.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/0c280c726b284499a3cfba656bfbccb6.jpg?v=1789617641"},{"product_id":"vr1-1064","title":"VR1-1064 True Zero Order Polymer Vortex Half Wave Retarder 1064nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003eRavg£¼0.5 %@700-1100 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾98 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e1064 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657159037114,"sku":"VR1-1064","price":6728.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/40512cba09bd425abe3cf616c1555dd6.jpg?v=1789617643"},{"product_id":"vr1-1310","title":"VR1-1310 True Zero Order Polymer Vortex Half Wave Retarder 1310nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003eRavg£¼0.5 %@1100-1700 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾98 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e1310 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657159102650,"sku":"VR1-1310","price":6728.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/22bebb9e4c604ddbbc7c3cb67c9eb6bb.jpg?v=1789617645"},{"product_id":"vr1-1550","title":"VR1-1550 True Zero Order Polymer Vortex Half Wave Retarder 1550nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003eRavg£¼0.5 %@1100-1700 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾98 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e1550 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657159495866,"sku":"VR1-1550","price":6728.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/034635d1fd424ca6a559abb5bc9b5f27.jpg?v=1789617644"},{"product_id":"vr2-405","title":"VR2-405 True Zero Order Polymer Vortex Half Wave Retarder 405nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003eRavg£¼0.5 %@400-700 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾85 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e405 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657161134266,"sku":"VR2-405","price":6500.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/054764c1d22d45d6894646020138b101.jpg?v=1789617646"},{"product_id":"vr2-442","title":"VR2-442 True Zero Order Polymer Vortex Half Wave Retarder 442nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003eRavg£¼0.5 %@400-700 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾93 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e442 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657161461946,"sku":"VR2-442","price":6500.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/2d93e8b2422344d793afe6c2ebc313db.jpg?v=1789617647"},{"product_id":"vr2-488","title":"VR2-488 True Zero Order Polymer Vortex Half Wave Retarder 488nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003eRavg£¼0.5 %@400-700 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾96 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e488 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657161789626,"sku":"VR2-488","price":6500.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/05c49af43c1e478ab7cf2415e387eba0.jpg?v=1789617648"},{"product_id":"vr2-520","title":"VR2-520 True Zero Order Polymer Vortex Half Wave Retarder 520nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003eRavg£¼0.5 %@400-700 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾97 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e520 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657162051770,"sku":"VR2-520","price":6500.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/04145bb5e2d545029fa146c40d5cafa0.png?v=1789617652"},{"product_id":"vr2-532","title":"VR2-532 True Zero Order Polymer Vortex Half Wave Retarder 532nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003eRavg£¼0.5 %@400-700 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾98 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e532 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657162150074,"sku":"VR2-532","price":6728.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/1efe68d7f555463e81d3dcdc0249f6a2.jpg?v=1789617651"},{"product_id":"vr2-633","title":"VR2-633 True Zero Order Polymer Vortex Half Wave Retarder 633nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003eRavg£¼0.5 %@400-700 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾98 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e633 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657162870970,"sku":"VR2-633","price":6728.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/1418e76c301047b281edcbd979cca51f.jpg?v=1789617652"},{"product_id":"vr2-670","title":"VR2-670 True Zero Order Polymer Vortex Half Wave Retarder 670nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003eRavg£¼0.5 %@400-700 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾98 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e670 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657163133114,"sku":"VR2-670","price":6500.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/07c1b3f8a5a3486e8af5449df26d83c1.jpg?v=1789617653"},{"product_id":"vr2-780","title":"VR2-780 True Zero Order Polymer Vortex Half Wave Retarder 780nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003eRavg£¼0.5 %@700-1100 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾98 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e780 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657163165882,"sku":"VR2-780","price":6728.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/06c67e5097b745629d6db0c36d9a36bb.png?v=1789617656"},{"product_id":"vr2-795","title":"VR2-795 True Zero Order Polymer Vortex Half Wave Retarder 795nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003eRavg£¼0.5 %@700-1100 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾98 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e795 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657163886778,"sku":"VR2-795","price":6500.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/2286f2437e3d4da9a42c30fc0b83d239.jpg?v=1789617656"},{"product_id":"vr2-808","title":"VR2-808 True Zero Order Polymer Vortex Half Wave Retarder 808nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003eRavg£¼0.5 %@700-1100 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾98 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e808 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657164411066,"sku":"VR2-808","price":6500.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/071d20324c6f4e0296fdbc93710997a3.png?v=1789617658"},{"product_id":"vr2-850","title":"VR2-850 True Zero Order Polymer Vortex Half Wave Retarder 850nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003eRavg£¼0.5 %@700-1100 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾98 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e850 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657164476602,"sku":"VR2-850","price":6500.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/25f9c2353f6b4c59ae9f01f4670b48db.jpg?v=1789617659"},{"product_id":"vr2-980","title":"VR2-980 True Zero Order Polymer Vortex Half Wave Retarder 980nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003eRavg£¼0.5 %@700-1100 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾98 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e980 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657165361338,"sku":"VR2-980","price":6728.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/14456a956f0b4c6ab06dd4891b272258.jpg?v=1789617659"},{"product_id":"vr2-1030","title":"VR2-1030 True Zero Order Polymer Vortex Half Wave Retarder 1030nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003eRavg£¼0.5 %@700-1100 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾98 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e1030 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657165623482,"sku":"VR2-1030","price":6500.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/28c637e0926544e480f3515dd4169186.jpg?v=1789617661"},{"product_id":"vr2-1064","title":"VR2-1064 True Zero Order Polymer Vortex Half Wave Retarder 1064nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003eRavg£¼0.5 %@700-1100 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾98 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e1064 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657166082234,"sku":"VR2-1064","price":6728.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/00c6fceb72334b30a98ed8922cd1d382.jpg?v=1789617662"},{"product_id":"vr2-1310","title":"VR2-1310 True Zero Order Polymer Vortex Half Wave Retarder 1310nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003eRavg£¼0.5 %@1100-1700 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾98 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e1310 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657166180538,"sku":"VR2-1310","price":6728.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/235ac934ee2244b79cb350b855675a3d.jpg?v=1789617662"},{"product_id":"vr2-1550","title":"VR2-1550 True Zero Order Polymer Vortex Half Wave Retarder 1550nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003eRavg£¼0.5 %@1100-1700 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾98 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e1550 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657166508218,"sku":"VR2-1550","price":6728.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/0be87668998f4c468e7cb6478eeda170.jpg?v=1789617664"},{"product_id":"vr4-405","title":"VR4-405 True Zero Order Polymer Vortex Half Wave Retarder 405nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003e400-700 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾85 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e405 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657166573754,"sku":"VR4-405","price":6630.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/24c06dc0735d4abbbc978c34cdd15df9.jpg?v=1789617665"},{"product_id":"vr4-488","title":"VR4-488 True Zero Order Polymer Vortex Half Wave Retarder 488nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003e400-700 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾96 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e488 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657166868666,"sku":"VR4-488","price":6630.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/055061b25bb845468635aae8c2530b9d.jpg?v=1789617666"},{"product_id":"vr4-532","title":"VR4-532 True Zero Order Polymer Vortex Half Wave Retarder 532nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003e400-700 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾97 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e532 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657167163578,"sku":"VR4-532","price":6630.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/0581e4b537844779985c6c3018c595da.jpg?v=1789617669"},{"product_id":"vr4-633","title":"VR4-633 True Zero Order Polymer Vortex Half Wave Retarder 633nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003e400-700 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾98 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e633 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657167524026,"sku":"VR4-633","price":6630.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/092882347fbf4e21a2393d7cb32aa460.jpg?v=1789617669"},{"product_id":"vr4-780","title":"VR4-780 True Zero Order Polymer Vortex Half Wave Retarder 780nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003e700-1100 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾98 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e780 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657167786170,"sku":"VR4-780","price":6630.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/12d6c8ebfc664dcbbe69437a2515ad7e.jpg?v=1789617671"},{"product_id":"vr4-850","title":"VR4-850 True Zero Order Polymer Vortex Half Wave Retarder 850nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003e700-1100 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾98 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e850 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657167851706,"sku":"VR4-850","price":6630.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/06a8cea76b6c47b38e1c3485dc3cf16e.jpg?v=1789617670"},{"product_id":"vr4-980","title":"VR4-980 True Zero Order Polymer Vortex Half Wave Retarder 980nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003e700-1100 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾98 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e980 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657168146618,"sku":"VR4-980","price":6630.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/04cab8a1ee434c6795396113f66a893e.jpg?v=1789617671"},{"product_id":"vr4-1064","title":"VR4-1064 True Zero Order Polymer Vortex Half Wave Retarder 1064nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003e700-1100 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾98 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e1064 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657168474298,"sku":"VR4-1064","price":6630.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/06b7395e07a5492c8e26b383959781d2.jpg?v=1789617673"},{"product_id":"vr4-1550","title":"VR4-1550 True Zero Order Polymer Vortex Half Wave Retarder 1550nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003e1100-1700 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾98 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e1550 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657168539834,"sku":"VR4-1550","price":6630.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/090e6d0b42a2494c8c5f4c0dc7335829.jpg?v=1789617674"},{"product_id":"vr8-405","title":"VR8-405 True Zero Order Polymer Vortex Half Wave Retarder 405nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003e400-700 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾85 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e405 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657169031354,"sku":"VR8-405","price":6630.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/0355f65b860845e3af9345fbeb2de278.jpg?v=1789617675"},{"product_id":"vr8-488","title":"VR8-488 True Zero Order Polymer Vortex Half Wave Retarder 488nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003e400-700 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾96 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e488 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657169391802,"sku":"VR8-488","price":6630.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/1f505e168ea24a53937d7b6e474db8e5.jpg?v=1789617676"},{"product_id":"vr8-532","title":"VR8-532 True Zero Order Polymer Vortex Half Wave Retarder 532nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003e400-700 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾97 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e532 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657169948858,"sku":"VR8-532","price":6630.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/179feb94e3984aefb0d8ee11e33a0bd0.jpg?v=1789617677"},{"product_id":"vr8-633","title":"VR8-633 True Zero Order Polymer Vortex Half Wave Retarder 633nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003e400-700 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾98 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e633 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657170014394,"sku":"VR8-633","price":6630.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/158facafa64d4c2eb164b6dbcea75346.jpg?v=1789617678"},{"product_id":"vr8-780","title":"VR8-780 True Zero Order Polymer Vortex Half Wave Retarder 780nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003e700-1100 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾98 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e780 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657170735290,"sku":"VR8-780","price":6630.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/2b34546fde504f1aa532fe820e18bcf6.jpg?v=1789617679"},{"product_id":"vr8-850","title":"VR8-850 True Zero Order Polymer Vortex Half Wave Retarder 850nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003e700-1100 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾98 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e850 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657170833594,"sku":"VR8-850","price":6630.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/00d59493284a45c2af0053df74814188.jpg?v=1789617680"},{"product_id":"vr8-980","title":"VR8-980 True Zero Order Polymer Vortex Half Wave Retarder 980nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003e700-1100 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾98 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e980 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657171292346,"sku":"VR8-980","price":6630.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/44614c8d3157441fbe9ae7fc9d0c8cd7.jpg?v=1789617681"},{"product_id":"vr8-1064","title":"VR8-1064 True Zero Order Polymer Vortex Half Wave Retarder 1064nm","description":"\u003cp\u003eThe Vortex Retarder (VR) is fabricated with an N?BK7 glass substrate and Liquid Crystal Polymers (LCP). It features a sandwich structure consisting of front?and?rear glass substrates with a functional LCP film layer in?between, and is housed in a standard SM1 lens tube.\u003c\/p\u003e\u003cp\u003eWithin the LCP layer, the fast?axis orientation of liquid?crystal molecules is radially uniform across the substrate and varies continuously in the azimuthal direction.\u003c\/p\u003e\u003cp\u003eThis device delivers a uniform ¦Ë\/2 retardance across the entire aperture and is designed for single?wavelength operation.\u003c\/p\u003e\u003cp\u003eThe vortex retarder exhibits polarization?dependent optical properties. Depending on the polarization state of the incident beam, it can generate vector?polarized beams or vortex beams with helical phase wavefronts. It converts TEM???mode Gaussian beams into a donut?shaped hollow intensity distribution (refer to technical notes for detailed optical performance).\u003c\/p\u003e\u003cp\u003eCompared with conventional light?field modulation methods, vortex retarders offer advantages including high efficiency, reliable stability, easy operation and dedicated functionality. Its true?zero?order characteristic also enables low wavelength sensitivity, superior temperature stability and a large acceptable incident?angle range.\u003c\/p\u003e\u003cp\u003esupplies standard vortex retarders with operating wavelengths ¦Ë ranging from 405?1550?nm and order m from 1?128. Flexible customization of specifications is also available to meet diverse user requirements for various application scenarios. Please contact technical support for further details.\u003c\/p\u003e\u003ch2\u003eSpecifications\u003c\/h2\u003e\u003ctable\u003e\u003ctbody\u003e\n\u003ctr\u003e\n\u003cth\u003eMaterial\u003c\/th\u003e\n\u003ctd\u003eOptical Glass\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eVisible Light Transmittance\u003c\/th\u003e\n\u003ctd\u003e90%\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eCoating\u003c\/th\u003e\n\u003ctd\u003e700-1100 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eTransmission\u003c\/th\u003e\n\u003ctd\u003e£¾98 %\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eFilter Size\u003c\/th\u003e\n\u003ctd\u003e25 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eWavelength\u003c\/th\u003e\n\u003ctd\u003e1064 nm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eOperating Temperature\u003c\/th\u003e\n\u003ctd\u003e-20~60 ¡æ\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eClear Aperture\u003c\/th\u003e\n\u003ctd\u003e?21.5 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Quality (Scratch-Dig)\u003c\/th\u003e\n\u003ctd\u003e40\/20\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eRetardation\u003c\/th\u003e\n\u003ctd\u003e¦Ë\/2\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eInput Beam Size\u003c\/th\u003e\n\u003ctd\u003e?1.0~?12.0 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eSurface Parallelism\u003c\/th\u003e\n\u003ctd\u003e£¼2 arcmin\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003cth\u003eDimensions\u003c\/th\u003e\n\u003ctd\u003e?25.4¡Á3.2 mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\u003c\/table\u003e","brand":"LUMINA Optics","offers":[{"title":"Default Title","offer_id":46657171652794,"sku":"VR8-1064","price":6630.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0780\/1123\/6538\/files\/257e4467d8ac4aafaa2c4ae4ec1b83b9.jpg?v=1789617683"}],"url":"https:\/\/opticssupplypro.com\/collections\/micro-nano-optics.oembed?page=3","provider":"LUMINA Optics","version":"1.0","type":"link"}