{"title":"Polymer Vortex Retarders","description":"\u003cp\u003eBrowse 66+ retarders from WaveQuanta's catalog. Detailed specifications, datasheets, and 3D models available for each product. Request a quote today.\u003c\/p\u003e","products":[{"product_id":"polymer-vortex-retarders-vr1-405","title":"Polymer Vortex Retarders VR1-405","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=1 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=1 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm, achieving a conversion efficiency of ≥99.5%. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±1; under linearly polarized light, it produces vector polarization beams, including radially polarized beams and azimuthally polarized beams.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.05 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±1\u003c\/li\u003e\n\u003cli\u003eCapable of generating vector polarized beams, including radially and azimuthally polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481760252058,"sku":"VR1-405","price":849.82,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/126a90e596ded05e856ab37ab3f4d4a6.jpg?v=1771995652"},{"product_id":"polymer-vortex-retarders-vr1-442","title":"Polymer Vortex Retarders VR1-442","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=1 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=1 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm, achieving a conversion efficiency of ≥99.5%. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±1; under linearly polarized light, it produces vector polarization beams, including radially polarized beams and azimuthally polarized beams.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.05 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±1\u003c\/li\u003e\n\u003cli\u003eCapable of generating vector polarized beams, including radially and azimuthally polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481760481434,"sku":"VR1-442","price":849.82,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/126a90e596ded05e856ab37ab3f4d4a6_f3ffc64a-655d-4858-ab6f-f150a136752d.jpg?v=1771995657"},{"product_id":"polymer-vortex-retarders-vr1-488","title":"Polymer Vortex Retarders VR1-488","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=1 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=1 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm, achieving a conversion efficiency of ≥99.5%. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±1; under linearly polarized light, it produces vector polarization beams, including radially polarized beams and azimuthally polarized beams.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.05 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±1\u003c\/li\u003e\n\u003cli\u003eCapable of generating vector polarized beams, including radially and azimuthally polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481760612506,"sku":"VR1-488","price":849.82,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/126a90e596ded05e856ab37ab3f4d4a6_02500057-57f5-464f-bc72-a396e5250b46.jpg?v=1771995660"},{"product_id":"polymer-vortex-retarders-vr1-520","title":"Polymer Vortex Retarders VR1-520","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=1 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=1 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm, achieving a conversion efficiency of ≥99.5%. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±1; under linearly polarized light, it produces vector polarization beams, including radially polarized beams and azimuthally polarized beams.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.05 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±1\u003c\/li\u003e\n\u003cli\u003eCapable of generating vector polarized beams, including radially and azimuthally polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481760743578,"sku":"VR1-520","price":849.82,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/126a90e596ded05e856ab37ab3f4d4a6_a4ce2688-d100-4dbf-87ee-d4ba20f695ff.jpg?v=1771995663"},{"product_id":"polymer-vortex-retarders-vr1-532","title":"Polymer Vortex Retarders VR1-532","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=1 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=1 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm, achieving a conversion efficiency of ≥99.5%. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±1; under linearly polarized light, it produces vector polarization beams, including radially polarized beams and azimuthally polarized beams.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.05 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±1\u003c\/li\u003e\n\u003cli\u003eCapable of generating vector polarized beams, including radially and azimuthally polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481760907418,"sku":"VR1-532","price":879.63,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/126a90e596ded05e856ab37ab3f4d4a6_6009e95c-11fe-4902-831a-7cfd460eba00.jpg?v=1771995666"},{"product_id":"polymer-vortex-retarders-vr1-633","title":"Polymer Vortex Retarders VR1-633","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=1 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=1 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm, achieving a conversion efficiency of ≥99.5%. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±1; under linearly polarized light, it produces vector polarization beams, including radially polarized beams and azimuthally polarized beams.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.05 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±1\u003c\/li\u003e\n\u003cli\u003eCapable of generating vector polarized beams, including radially and azimuthally polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481761038490,"sku":"VR1-633","price":879.63,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/126a90e596ded05e856ab37ab3f4d4a6_154aee2f-ef04-4ec2-a240-bb1eba6038f1.jpg?v=1771995670"},{"product_id":"polymer-vortex-retarders-vr1-670","title":"Polymer Vortex Retarders VR1-670","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=1 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=1 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm, achieving a conversion efficiency of ≥99.5%. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±1; under linearly polarized light, it produces vector polarization beams, including radially polarized beams and azimuthally polarized beams.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.05 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±1\u003c\/li\u003e\n\u003cli\u003eCapable of generating vector polarized beams, including radially and azimuthally polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481761169562,"sku":"VR1-670","price":849.82,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/126a90e596ded05e856ab37ab3f4d4a6_16e6008f-20c8-4924-8307-2b022359b340.jpg?v=1771995673"},{"product_id":"polymer-vortex-retarders-vr1-780","title":"Polymer Vortex Retarders VR1-780","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=1 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=1 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm, achieving a conversion efficiency of ≥99.5%. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±1; under linearly polarized light, it produces vector polarization beams, including radially polarized beams and azimuthally polarized beams.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.05 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±1\u003c\/li\u003e\n\u003cli\u003eCapable of generating vector polarized beams, including radially and azimuthally polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481761300634,"sku":"VR1-780","price":879.63,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/126a90e596ded05e856ab37ab3f4d4a6_6bf72793-249c-401f-a8b9-32a43f7b4cbd.jpg?v=1771995677"},{"product_id":"polymer-vortex-retarders-vr1-795","title":"Polymer Vortex Retarders VR1-795","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=1 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=1 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm, achieving a conversion efficiency of ≥99.5%. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±1; under linearly polarized light, it produces vector polarization beams, including radially polarized beams and azimuthally polarized beams.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.05 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±1\u003c\/li\u003e\n\u003cli\u003eCapable of generating vector polarized beams, including radially and azimuthally polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481761530010,"sku":"VR1-795","price":849.82,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/126a90e596ded05e856ab37ab3f4d4a6_56d31ed9-2337-4317-b451-e5317b3dd7b4.jpg?v=1771995680"},{"product_id":"polymer-vortex-retarders-vr1-808","title":"Polymer Vortex Retarders VR1-808","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=1 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=1 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm, achieving a conversion efficiency of ≥99.5%. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±1; under linearly polarized light, it produces vector polarization beams, including radially polarized beams and azimuthally polarized beams.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.05 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±1\u003c\/li\u003e\n\u003cli\u003eCapable of generating vector polarized beams, including radially and azimuthally polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481761726618,"sku":"VR1-808","price":849.82,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/126a90e596ded05e856ab37ab3f4d4a6_0c3d7036-de09-4070-a350-74dd15665007.jpg?v=1771995684"},{"product_id":"polymer-vortex-retarders-vr1-850","title":"Polymer Vortex Retarders VR1-850","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=1 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=1 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm, achieving a conversion efficiency of ≥99.5%. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±1; under linearly polarized light, it produces vector polarization beams, including radially polarized beams and azimuthally polarized beams.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.05 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±1\u003c\/li\u003e\n\u003cli\u003eCapable of generating vector polarized beams, including radially and azimuthally polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481761857690,"sku":"VR1-850","price":849.82,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/126a90e596ded05e856ab37ab3f4d4a6_4d9bc1d8-e959-4315-90ff-5e14644b0024.jpg?v=1771995687"},{"product_id":"polymer-vortex-retarders-vr1-980","title":"Polymer Vortex Retarders VR1-980","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=1 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=1 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm, achieving a conversion efficiency of ≥99.5%. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±1; under linearly polarized light, it produces vector polarization beams, including radially polarized beams and azimuthally polarized beams.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.05 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±1\u003c\/li\u003e\n\u003cli\u003eCapable of generating vector polarized beams, including radially and azimuthally polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481761988762,"sku":"VR1-980","price":879.63,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/126a90e596ded05e856ab37ab3f4d4a6_5ca1a305-11d0-4b3a-902b-5c025c4e1e6e.jpg?v=1771995691"},{"product_id":"polymer-vortex-retarders-vr1-1030","title":"Polymer Vortex Retarders VR1-1030","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=1 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=1 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm, achieving a conversion efficiency of ≥99.5%. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±1; under linearly polarized light, it produces vector polarization beams, including radially polarized beams and azimuthally polarized beams.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.05 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±1\u003c\/li\u003e\n\u003cli\u003eCapable of generating vector polarized beams, including radially and azimuthally polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481762185370,"sku":"VR1-1030","price":849.82,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/126a90e596ded05e856ab37ab3f4d4a6_746ea354-ce5f-4f14-91be-aa74b80dfe0e.jpg?v=1771995695"},{"product_id":"polymer-vortex-retarders-vr1-1064","title":"Polymer Vortex Retarders VR1-1064","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=1 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=1 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm, achieving a conversion efficiency of ≥99.5%. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±1; under linearly polarized light, it produces vector polarization beams, including radially polarized beams and azimuthally polarized beams.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.05 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±1\u003c\/li\u003e\n\u003cli\u003eCapable of generating vector polarized beams, including radially and azimuthally polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481762316442,"sku":"VR1-1064","price":879.63,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/126a90e596ded05e856ab37ab3f4d4a6_d85d23ef-b76d-4366-bee3-afcbb08f8171.jpg?v=1771995698"},{"product_id":"polymer-vortex-retarders-vr1-1310","title":"Polymer Vortex Retarders VR1-1310","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=1 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=1 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm, achieving a conversion efficiency of ≥99.5%. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±1; under linearly polarized light, it produces vector polarization beams, including radially polarized beams and azimuthally polarized beams.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.05 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±1\u003c\/li\u003e\n\u003cli\u003eCapable of generating vector polarized beams, including radially and azimuthally polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481762447514,"sku":"VR1-1310","price":879.63,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/126a90e596ded05e856ab37ab3f4d4a6_10ef2cdc-de4b-46b1-b255-f8a88474c9ae.jpg?v=1771995702"},{"product_id":"polymer-vortex-retarders-vr1-1550","title":"Polymer Vortex Retarders VR1-1550","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=1 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=1 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm, achieving a conversion efficiency of ≥99.5%. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±1; under linearly polarized light, it produces vector polarization beams, including radially polarized beams and azimuthally polarized beams.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.05 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±1\u003c\/li\u003e\n\u003cli\u003eCapable of generating vector polarized beams, including radially and azimuthally polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481762611354,"sku":"VR1-1550","price":879.63,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/126a90e596ded05e856ab37ab3f4d4a6_ea544e56-9451-43eb-9136-f426d18da178.jpg?v=1771995705"},{"product_id":"polymer-vortex-retarders-vr2-405","title":"Polymer Vortex Retarders VR2-405","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=2 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=2 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm, with a conversion efficiency of ≥99.5%. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±2; under linearly polarized light, it produces higher-order vector polarized beams.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.05 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±2\u003c\/li\u003e\n\u003cli\u003eCapable of generating higher-order vector polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481762709658,"sku":"VR2-405","price":849.82,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/6e6ec8a4ae83099bcb0e4505159edeec.jpg?v=1771995709"},{"product_id":"polymer-vortex-retarders-vr2-442","title":"Polymer Vortex Retarders VR2-442","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=2 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=2 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm, with a conversion efficiency of ≥99.5%. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±2; under linearly polarized light, it produces higher-order vector polarized beams.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.05 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±2\u003c\/li\u003e\n\u003cli\u003eCapable of generating higher-order vector polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481762840730,"sku":"VR2-442","price":849.82,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/6e6ec8a4ae83099bcb0e4505159edeec_1801430e-ea7b-4959-8c74-0027b9d4181b.jpg?v=1771995712"},{"product_id":"polymer-vortex-retarders-vr2-488","title":"Polymer Vortex Retarders VR2-488","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=2 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=2 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm, with a conversion efficiency of ≥99.5%. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±2; under linearly polarized light, it produces higher-order vector polarized beams.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.05 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±2\u003c\/li\u003e\n\u003cli\u003eCapable of generating higher-order vector polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481762971802,"sku":"VR2-488","price":849.82,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/6e6ec8a4ae83099bcb0e4505159edeec_abaa4770-a466-4566-9c61-812990d34416.jpg?v=1771995716"},{"product_id":"polymer-vortex-retarders-vr2-520","title":"Polymer Vortex Retarders VR2-520","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=2 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=2 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm, with a conversion efficiency of ≥99.5%. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±2; under linearly polarized light, it produces higher-order vector polarized beams.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.05 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±2\u003c\/li\u003e\n\u003cli\u003eCapable of generating higher-order vector polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481763332250,"sku":"VR2-520","price":849.82,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/6e6ec8a4ae83099bcb0e4505159edeec_2517ed04-2b8c-4f10-9cf2-7f82e13ab8a7.jpg?v=1771995719"},{"product_id":"polymer-vortex-retarders-vr2-532","title":"Polymer Vortex Retarders VR2-532","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=2 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=2 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm, with a conversion efficiency of ≥99.5%. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±2; under linearly polarized light, it produces higher-order vector polarized beams.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.05 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±2\u003c\/li\u003e\n\u003cli\u003eCapable of generating higher-order vector polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481763430554,"sku":"VR2-532","price":879.63,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/6e6ec8a4ae83099bcb0e4505159edeec_292b7ce3-313a-46ae-a4cb-f01cf2d84692.jpg?v=1771995723"},{"product_id":"polymer-vortex-retarders-vr2-633","title":"Polymer Vortex Retarders VR2-633","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=2 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=2 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm, with a conversion efficiency of ≥99.5%. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±2; under linearly polarized light, it produces higher-order vector polarized beams.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.05 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±2\u003c\/li\u003e\n\u003cli\u003eCapable of generating higher-order vector polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481764544666,"sku":"VR2-633","price":879.63,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/6e6ec8a4ae83099bcb0e4505159edeec_0de8b4d7-fcc1-445e-9382-e019e4d1828b.jpg?v=1771995727"},{"product_id":"polymer-vortex-retarders-vr2-670","title":"Polymer Vortex Retarders VR2-670","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=2 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=2 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm, with a conversion efficiency of ≥99.5%. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±2; under linearly polarized light, it produces higher-order vector polarized beams.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.05 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±2\u003c\/li\u003e\n\u003cli\u003eCapable of generating higher-order vector polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481764937882,"sku":"VR2-670","price":849.82,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/6e6ec8a4ae83099bcb0e4505159edeec_3e609104-0dcc-4eb9-9125-faf5bfcf11a7.jpg?v=1771995731"},{"product_id":"polymer-vortex-retarders-vr2-780","title":"Polymer Vortex Retarders VR2-780","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=2 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=2 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm, with a conversion efficiency of ≥99.5%. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±2; under linearly polarized light, it produces higher-order vector polarized beams.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.05 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±2\u003c\/li\u003e\n\u003cli\u003eCapable of generating higher-order vector polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481765101722,"sku":"VR2-780","price":879.63,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/6e6ec8a4ae83099bcb0e4505159edeec_84829b57-ebf5-41f7-8307-c7e23952bda6.jpg?v=1771995734"},{"product_id":"polymer-vortex-retarders-vr2-795","title":"Polymer Vortex Retarders VR2-795","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=2 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=2 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm, with a conversion efficiency of ≥99.5%. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±2; under linearly polarized light, it produces higher-order vector polarized beams.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.05 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±2\u003c\/li\u003e\n\u003cli\u003eCapable of generating higher-order vector polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481765232794,"sku":"VR2-795","price":849.82,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/6e6ec8a4ae83099bcb0e4505159edeec_77ba0bf7-cbc6-4986-8d4a-de39adc2f161.jpg?v=1771995738"},{"product_id":"polymer-vortex-retarders-vr2-808","title":"Polymer Vortex Retarders VR2-808","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=2 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=2 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm, with a conversion efficiency of ≥99.5%. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±2; under linearly polarized light, it produces higher-order vector polarized beams.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.05 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±2\u003c\/li\u003e\n\u003cli\u003eCapable of generating higher-order vector polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481765363866,"sku":"VR2-808","price":849.82,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/6e6ec8a4ae83099bcb0e4505159edeec_4bdfa011-037e-4298-94ee-2b4bb2d573bc.jpg?v=1771995741"},{"product_id":"polymer-vortex-retarders-vr2-850","title":"Polymer Vortex Retarders VR2-850","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=2 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=2 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm, with a conversion efficiency of ≥99.5%. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±2; under linearly polarized light, it produces higher-order vector polarized beams.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.05 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±2\u003c\/li\u003e\n\u003cli\u003eCapable of generating higher-order vector polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481765757082,"sku":"VR2-850","price":849.82,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/6e6ec8a4ae83099bcb0e4505159edeec_b275f3be-8931-46fc-8625-a0dd08fb11ff.jpg?v=1771995745"},{"product_id":"polymer-vortex-retarders-vr2-980","title":"Polymer Vortex Retarders VR2-980","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=2 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=2 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm, with a conversion efficiency of ≥99.5%. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±2; under linearly polarized light, it produces higher-order vector polarized beams.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.05 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±2\u003c\/li\u003e\n\u003cli\u003eCapable of generating higher-order vector polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481765920922,"sku":"VR2-980","price":879.63,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/6e6ec8a4ae83099bcb0e4505159edeec_5cd29d3a-e7a5-43bd-b15b-b1ffe8745ce2.jpg?v=1771995748"},{"product_id":"polymer-vortex-retarders-vr2-1030","title":"Polymer Vortex Retarders VR2-1030","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=2 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=2 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm, with a conversion efficiency of ≥99.5%. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±2; under linearly polarized light, it produces higher-order vector polarized beams.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.05 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±2\u003c\/li\u003e\n\u003cli\u003eCapable of generating higher-order vector polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481766019226,"sku":"VR2-1030","price":849.82,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/6e6ec8a4ae83099bcb0e4505159edeec_3d87165b-d7cd-4d63-949a-21a3c47445bc.jpg?v=1771995751"},{"product_id":"polymer-vortex-retarders-vr2-1064","title":"Polymer Vortex Retarders VR2-1064","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=2 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=2 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm, with a conversion efficiency of ≥99.5%. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±2; under linearly polarized light, it produces higher-order vector polarized beams.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.05 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±2\u003c\/li\u003e\n\u003cli\u003eCapable of generating higher-order vector polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481766117530,"sku":"VR2-1064","price":879.63,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/6e6ec8a4ae83099bcb0e4505159edeec_3108b87c-cb84-445c-ac05-1e8b501b66a7.jpg?v=1771995756"},{"product_id":"polymer-vortex-retarders-vr2-1310","title":"Polymer Vortex Retarders VR2-1310","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=2 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=2 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm, with a conversion efficiency of ≥99.5%. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±2; under linearly polarized light, it produces higher-order vector polarized beams.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.05 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±2\u003c\/li\u003e\n\u003cli\u003eCapable of generating higher-order vector polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481766248602,"sku":"VR2-1310","price":879.63,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/6e6ec8a4ae83099bcb0e4505159edeec_3ed358d6-1ea5-4b8b-8ffc-9dce6f024d19.jpg?v=1771995760"},{"product_id":"polymer-vortex-retarders-vr2-1550","title":"Polymer Vortex Retarders VR2-1550","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=2 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=2 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm, with a conversion efficiency of ≥99.5%. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±2; under linearly polarized light, it produces higher-order vector polarized beams.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.05 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±2\u003c\/li\u003e\n\u003cli\u003eCapable of generating higher-order vector polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481766412442,"sku":"VR2-1550","price":879.63,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/6e6ec8a4ae83099bcb0e4505159edeec_3c1889c4-20da-4cd3-aa69-8dd0f4f3b7c0.jpg?v=1771995763"},{"product_id":"polymer-vortex-retarders-vr4-405","title":"Polymer Vortex Retarders VR4-405","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=4 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=4 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±4; under linearly polarized light, it produces higher-order vector polarized beams. The smaller the selected order m, the smaller the central hole size of the beam.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.15 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±4\u003c\/li\u003e\n\u003cli\u003eCapable of generating higher-order vector polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481766510746,"sku":"VR4-405","price":866.81,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/234ef766043635c4bfc5b2249a8af907.jpg?v=1771995766"},{"product_id":"polymer-vortex-retarders-vr4-488","title":"Polymer Vortex Retarders VR4-488","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=4 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=4 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±4; under linearly polarized light, it produces higher-order vector polarized beams. The smaller the selected order m, the smaller the central hole size of the beam.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.15 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±4\u003c\/li\u003e\n\u003cli\u003eCapable of generating higher-order vector polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481766641818,"sku":"VR4-488","price":866.81,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/234ef766043635c4bfc5b2249a8af907_2dd8c1c4-2654-4da4-bfc4-d1b8a22d2b6b.jpg?v=1771995770"},{"product_id":"polymer-vortex-retarders-vr4-532","title":"Polymer Vortex Retarders VR4-532","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=4 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=4 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±4; under linearly polarized light, it produces higher-order vector polarized beams. The smaller the selected order m, the smaller the central hole size of the beam.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.15 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±4\u003c\/li\u003e\n\u003cli\u003eCapable of generating higher-order vector polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481766707354,"sku":"VR4-532","price":866.81,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/234ef766043635c4bfc5b2249a8af907_d297463f-b504-4dd8-944a-b0bea4295ada.jpg?v=1771995773"},{"product_id":"polymer-vortex-retarders-vr4-633","title":"Polymer Vortex Retarders VR4-633","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=4 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=4 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±4; under linearly polarized light, it produces higher-order vector polarized beams. The smaller the selected order m, the smaller the central hole size of the beam.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.15 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±4\u003c\/li\u003e\n\u003cli\u003eCapable of generating higher-order vector polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481766805658,"sku":"VR4-633","price":866.81,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/234ef766043635c4bfc5b2249a8af907_63a5849a-8906-4317-9ca9-1b783299c0ed.jpg?v=1771995776"},{"product_id":"polymer-vortex-retarders-vr4-780","title":"Polymer Vortex Retarders VR4-780","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=4 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=4 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±4; under linearly polarized light, it produces higher-order vector polarized beams. The smaller the selected order m, the smaller the central hole size of the beam.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.15 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±4\u003c\/li\u003e\n\u003cli\u003eCapable of generating higher-order vector polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481766936730,"sku":"VR4-780","price":866.81,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/234ef766043635c4bfc5b2249a8af907_1cd34db3-9f8d-4c6e-907b-65ae871f261f.jpg?v=1771995780"},{"product_id":"polymer-vortex-retarders-vr4-850","title":"Polymer Vortex Retarders VR4-850","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=4 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=4 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±4; under linearly polarized light, it produces higher-order vector polarized beams. The smaller the selected order m, the smaller the central hole size of the beam.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.15 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±4\u003c\/li\u003e\n\u003cli\u003eCapable of generating higher-order vector polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481767035034,"sku":"VR4-850","price":866.81,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/234ef766043635c4bfc5b2249a8af907_c8eff067-f679-42a7-8edf-7969b5765662.jpg?v=1771995784"},{"product_id":"polymer-vortex-retarders-vr4-980","title":"Polymer Vortex Retarders VR4-980","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=4 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=4 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±4; under linearly polarized light, it produces higher-order vector polarized beams. The smaller the selected order m, the smaller the central hole size of the beam.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.15 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±4\u003c\/li\u003e\n\u003cli\u003eCapable of generating higher-order vector polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481767166106,"sku":"VR4-980","price":866.81,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/234ef766043635c4bfc5b2249a8af907_9935d864-af43-4bf6-8ded-b0ddd57bf145.jpg?v=1771995788"},{"product_id":"polymer-vortex-retarders-vr4-1064","title":"Polymer Vortex Retarders VR4-1064","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=4 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=4 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±4; under linearly polarized light, it produces higher-order vector polarized beams. The smaller the selected order m, the smaller the central hole size of the beam.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.15 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±4\u003c\/li\u003e\n\u003cli\u003eCapable of generating higher-order vector polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481767329946,"sku":"VR4-1064","price":866.81,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/234ef766043635c4bfc5b2249a8af907_e3ae5937-21cc-476d-90a7-8ffd98dd8911.jpg?v=1771995791"},{"product_id":"polymer-vortex-retarders-vr4-1550","title":"Polymer Vortex Retarders VR4-1550","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=4 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=4 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±4; under linearly polarized light, it produces higher-order vector polarized beams. The smaller the selected order m, the smaller the central hole size of the beam.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.15 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±4\u003c\/li\u003e\n\u003cli\u003eCapable of generating higher-order vector polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481767461018,"sku":"VR4-1550","price":866.81,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/234ef766043635c4bfc5b2249a8af907_7cf48687-a0a8-4b4d-8054-42ec8419875f.jpg?v=1771995795"},{"product_id":"polymer-vortex-retarders-vr8-405","title":"Polymer Vortex Retarders VR8-405","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=8 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=8 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±8; under linearly polarized light, it produces higher-order vector polarized beams. The smaller the selected order m, the smaller the central hole size of the beam.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.15 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±8\u003c\/li\u003e\n\u003cli\u003eCapable of generating higher-order vector polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481767592090,"sku":"VR8-405","price":866.81,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/f19f1155ce5cf6f5fe99ece9d50d8154.jpg?v=1771995798"},{"product_id":"polymer-vortex-retarders-vr8-488","title":"Polymer Vortex Retarders VR8-488","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=8 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=8 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±8; under linearly polarized light, it produces higher-order vector polarized beams. The smaller the selected order m, the smaller the central hole size of the beam.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.15 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±8\u003c\/li\u003e\n\u003cli\u003eCapable of generating higher-order vector polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481767821466,"sku":"VR8-488","price":866.81,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/f19f1155ce5cf6f5fe99ece9d50d8154_97d73c91-8782-43a4-b65e-16c7a012505f.jpg?v=1771995802"},{"product_id":"polymer-vortex-retarders-vr8-532","title":"Polymer Vortex Retarders VR8-532","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=8 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=8 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±8; under linearly polarized light, it produces higher-order vector polarized beams. The smaller the selected order m, the smaller the central hole size of the beam.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.15 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±8\u003c\/li\u003e\n\u003cli\u003eCapable of generating higher-order vector polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481768181914,"sku":"VR8-532","price":866.81,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/f19f1155ce5cf6f5fe99ece9d50d8154_421d58f0-72fa-4ef2-b916-fac6bcd988ab.jpg?v=1771995806"},{"product_id":"polymer-vortex-retarders-vr8-633","title":"Polymer Vortex Retarders VR8-633","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=8 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=8 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±8; under linearly polarized light, it produces higher-order vector polarized beams. The smaller the selected order m, the smaller the central hole size of the beam.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.15 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±8\u003c\/li\u003e\n\u003cli\u003eCapable of generating higher-order vector polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481768378522,"sku":"VR8-633","price":866.81,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/f19f1155ce5cf6f5fe99ece9d50d8154_8a107229-eec4-4ff2-98c1-d319fe6937a3.jpg?v=1771995813"},{"product_id":"polymer-vortex-retarders-vr8-780","title":"Polymer Vortex Retarders VR8-780","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=8 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=8 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±8; under linearly polarized light, it produces higher-order vector polarized beams. The smaller the selected order m, the smaller the central hole size of the beam.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.15 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±8\u003c\/li\u003e\n\u003cli\u003eCapable of generating higher-order vector polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481768509594,"sku":"VR8-780","price":866.81,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/f19f1155ce5cf6f5fe99ece9d50d8154_47d9003a-15d3-4a8b-836e-6da62b91a7c1.jpg?v=1771995816"},{"product_id":"polymer-vortex-retarders-vr8-850","title":"Polymer Vortex Retarders VR8-850","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=8 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=8 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±8; under linearly polarized light, it produces higher-order vector polarized beams. The smaller the selected order m, the smaller the central hole size of the beam.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.15 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±8\u003c\/li\u003e\n\u003cli\u003eCapable of generating higher-order vector polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481768607898,"sku":"VR8-850","price":866.81,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/f19f1155ce5cf6f5fe99ece9d50d8154_f6f1ca60-858c-44e2-99fe-d6e9e9e77528.jpg?v=1771995820"},{"product_id":"polymer-vortex-retarders-vr8-980","title":"Polymer Vortex Retarders VR8-980","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=8 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=8 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±8; under linearly polarized light, it produces higher-order vector polarized beams. The smaller the selected order m, the smaller the central hole size of the beam.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.15 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±8\u003c\/li\u003e\n\u003cli\u003eCapable of generating higher-order vector polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481768771738,"sku":"VR8-980","price":866.81,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/f19f1155ce5cf6f5fe99ece9d50d8154_d4ba3341-a7ff-412a-b0f1-030137a4d382.jpg?v=1771995823"},{"product_id":"polymer-vortex-retarders-vr8-1064","title":"Polymer Vortex Retarders VR8-1064","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=8 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=8 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±8; under linearly polarized light, it produces higher-order vector polarized beams. The smaller the selected order m, the smaller the central hole size of the beam.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.15 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±8\u003c\/li\u003e\n\u003cli\u003eCapable of generating higher-order vector polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481768902810,"sku":"VR8-1064","price":866.81,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/f19f1155ce5cf6f5fe99ece9d50d8154_4bea6849-fa0e-4b41-a8e5-99a504ea477f.jpg?v=1771995827"},{"product_id":"polymer-vortex-retarders-vr8-1550","title":"Polymer Vortex Retarders VR8-1550","description":"\u003cp\u003eThe LBTEK Vortex Retarder (VR) is fabricated using N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, featuring a sandwich structure of \"front and rear glass substrates with an intermediate LCP functional layer,\" and is mounted in a standard SM1 lens tube.\u003c\/p\u003e\n\n\u003cp\u003eIn the LCP layer, the fast-axis orientation of the liquid crystal molecules is uniformly aligned along the radial direction of the substrate and continuously varies along the angular direction. The device exhibits a uniform λ\/2 retardation across the entire plane, making it a single-wavelength component.\u003c\/p\u003e\n\n\u003cp\u003eThe vortex retarder possesses polarization-dependent optical characteristics. With different polarization states of the incident beam, it can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00-mode Gaussian beams into hollow \"doughnut-shaped\" intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to traditional methods of optical field modulation, the vortex retarder offers high efficiency, stability, ease of operation, and dedicated functionality. Its true zero-order characteristic also contributes to low wavelength sensitivity, high temperature stability, and a wide range of incident angles.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid Crystal Polymer\/N-BK7 window plate, sandwich flat structure, with mechanical housing\u003c\/li\u003e\n\u003cli\u003ePolarization-dependent, applicable for generating vector polarized beams and vortex beams\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, specialized function, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength λ: 405–1550 nm, order m: 1–128\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=8 Series\u003c\/h3\u003e\n\u003cp\u003eThe m=8 vortex waveplate is suitable for incident light with diameters ranging from Ø1 mm to Ø21.5 mm. When illuminated with circularly polarized light, it can generate Laguerre-Gaussian beams with l=±8; under linearly polarized light, it produces higher-order vector polarized beams. The smaller the selected order m, the smaller the central hole size of the beam.\u003c\/p\u003e\n\u003cul\u003e\n\u003cli\u003eApplicable to incident light with dimensions Ø0.15 to Ø21.5 mm\u003c\/li\u003e\n\u003cli\u003eCapable of generating Laguerre-Gaussian beams with l=±8\u003c\/li\u003e\n\u003cli\u003eCapable of generating higher-order vector polarized beams\u003c\/li\u003e\n\u003c\/ul\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481769001114,"sku":"VR8-1550","price":866.81,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/f19f1155ce5cf6f5fe99ece9d50d8154_3ab751e0-510f-42d9-a097-5a1427148ac3.jpg?v=1771995831"}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/collections\/126a90e596ded05e856ab37ab3f4d4a6_746ea354-ce5f-4f14-91be-aa74b80dfe0e.jpg?v=1777788252","url":"https:\/\/waveqvanta.com\/collections\/lbtek-micro-nano-optics-vortex-retarders-polymer-vortex-retarders.oembed?page=2","provider":"WaveQuanta","version":"1.0","type":"link"}