{"title":"Vortex retarder and phase plate","description":"\u003cp\u003eBrowse 77+ 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":"spiral-phase-plates-vp1-355","title":"Spiral Phase Plates VP1-355","description":"\u003cp\u003eThe LBTEK Spiral Phase Plate is a diffractive optical element that achieves phase modulation of light beams by varying the material height along the azimuthal direction, thereby generating vortex beams. When an incident plane wave passes through the spiral phase plate, it produces a vortex beam with a helical phase front, causing mutual cancellation at the optical axis and forming a central dark ring.\u003c\/p\u003e\n\n\u003cp\u003eSpiral phase plates offer advantages such as high efficiency, stability, ease of operation, and a high damage threshold, making them widely applicable in optical tweezers, high-resolution microscopy, information processing, and surface topography measurement. Compared to liquid crystal polymers, UV-grade fused silica features lower absorption, making it more compatible with ultraviolet applications.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eUV fused silica material, spiral staircase structure\u003c\/li\u003e\n\u003cli\u003eApplicable for generating vortex beams with spiral phase wavefronts\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, high damage threshold\u003c\/li\u003e\n\u003cli\u003eWorking wavelength: 355 nm, 532 nm, and 1064 nm; order m: 1, 2\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003eSpiral Phase Plate Series\u003c\/h3\u003e\n\u003cp\u003eThe LBTEK spiral phase plate is fabricated from UV-grade fused silica using surface relief technology, featuring a spiral staircase structure. The standard spiral phase plate has a clear aperture of 9×9 mm and is mounted in a compatible 1-inch mechanical housing. The housing surface is engraved with the product model number.\u003c\/p\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481755533466,"sku":"VP1-355","price":1061.49,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/1-FvaBTWeyHpS8QA8K3rYJmh6yWvNt.jpg?v=1771995566"},{"product_id":"spiral-phase-plates-vp1-532","title":"Spiral Phase Plates VP1-532","description":"\u003cp\u003eThe LBTEK Spiral Phase Plate is a diffractive optical element that achieves phase modulation of light beams by varying the material height along the azimuthal direction, thereby generating vortex beams. When an incident plane wave passes through the spiral phase plate, it produces a vortex beam with a helical phase front, causing mutual cancellation at the optical axis and forming a central dark ring.\u003c\/p\u003e\n\n\u003cp\u003eSpiral phase plates offer advantages such as high efficiency, stability, ease of operation, and a high damage threshold, making them widely applicable in optical tweezers, high-resolution microscopy, information processing, and surface topography measurement. Compared to liquid crystal polymers, UV-grade fused silica features lower absorption, making it more compatible with ultraviolet applications.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eUV fused silica material, spiral staircase structure\u003c\/li\u003e\n\u003cli\u003eApplicable for generating vortex beams with spiral phase wavefronts\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, high damage threshold\u003c\/li\u003e\n\u003cli\u003eWorking wavelength: 355 nm, 532 nm, and 1064 nm; order m: 1, 2\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003eSpiral Phase Plate Series\u003c\/h3\u003e\n\u003cp\u003eThe LBTEK spiral phase plate is fabricated from UV-grade fused silica using surface relief technology, featuring a spiral staircase structure. The standard spiral phase plate has a clear aperture of 9×9 mm and is mounted in a compatible 1-inch mechanical housing. The housing surface is engraved with the product model number.\u003c\/p\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481755893914,"sku":"VP1-532","price":1061.49,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/1-FvaBTWeyHpS8QA8K3rYJmh6yWvNt_f8dc8a41-adf4-4c7d-8446-00c8377ef811.jpg?v=1771995569"},{"product_id":"spiral-phase-plates-vp1-1064","title":"Spiral Phase Plates VP1-1064","description":"\u003cp\u003eThe LBTEK Spiral Phase Plate is a diffractive optical element that achieves phase modulation of light beams by varying the material height along the azimuthal direction, thereby generating vortex beams. When an incident plane wave passes through the spiral phase plate, it produces a vortex beam with a helical phase front, causing mutual cancellation at the optical axis and forming a central dark ring.\u003c\/p\u003e\n\n\u003cp\u003eSpiral phase plates offer advantages such as high efficiency, stability, ease of operation, and a high damage threshold, making them widely applicable in optical tweezers, high-resolution microscopy, information processing, and surface topography measurement. Compared to liquid crystal polymers, UV-grade fused silica features lower absorption, making it more compatible with ultraviolet applications.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eUV fused silica material, spiral staircase structure\u003c\/li\u003e\n\u003cli\u003eApplicable for generating vortex beams with spiral phase wavefronts\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, high damage threshold\u003c\/li\u003e\n\u003cli\u003eWorking wavelength: 355 nm, 532 nm, and 1064 nm; order m: 1, 2\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003eSpiral Phase Plate Series\u003c\/h3\u003e\n\u003cp\u003eThe LBTEK spiral phase plate is fabricated from UV-grade fused silica using surface relief technology, featuring a spiral staircase structure. The standard spiral phase plate has a clear aperture of 9×9 mm and is mounted in a compatible 1-inch mechanical housing. The housing surface is engraved with the product model number.\u003c\/p\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481755959450,"sku":"VP1-1064","price":1061.49,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/1-FvaBTWeyHpS8QA8K3rYJmh6yWvNt_b2f13385-e8b6-46f7-9dba-c8fd923894f7.jpg?v=1771995573"},{"product_id":"spiral-phase-plates-vp2-355","title":"Spiral Phase Plates VP2-355","description":"\u003cp\u003eThe LBTEK Spiral Phase Plate is a diffractive optical element that achieves phase modulation of light beams by varying the material height along the azimuthal direction, thereby generating vortex beams. When an incident plane wave passes through the spiral phase plate, it produces a vortex beam with a helical phase front, causing mutual cancellation at the optical axis and forming a central dark ring.\u003c\/p\u003e\n\n\u003cp\u003eSpiral phase plates offer advantages such as high efficiency, stability, ease of operation, and a high damage threshold, making them widely applicable in optical tweezers, high-resolution microscopy, information processing, and surface topography measurement. Compared to liquid crystal polymers, UV-grade fused silica features lower absorption, making it more compatible with ultraviolet applications.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eUV fused silica material, spiral staircase structure\u003c\/li\u003e\n\u003cli\u003eApplicable for generating vortex beams with spiral phase wavefronts\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, high damage threshold\u003c\/li\u003e\n\u003cli\u003eWorking wavelength: 355 nm, 532 nm, and 1064 nm; order m: 1, 2\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003eSpiral Phase Plate Series\u003c\/h3\u003e\n\u003cp\u003eThe LBTEK spiral phase plate is fabricated from UV-grade fused silica using surface relief technology, featuring a spiral staircase structure. The standard spiral phase plate has a clear aperture of 9×9 mm and is mounted in a compatible 1-inch mechanical housing. The housing surface is engraved with the product model number.\u003c\/p\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481758843034,"sku":"VP2-355","price":1061.49,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/5-Fm2rI5Z5BbImYUGq0mEYVAYNM346.jpg?v=1771995631"},{"product_id":"spiral-phase-plates-vp2-532","title":"Spiral Phase Plates VP2-532","description":"\u003cp\u003eThe LBTEK Spiral Phase Plate is a diffractive optical element that achieves phase modulation of light beams by varying the material height along the azimuthal direction, thereby generating vortex beams. When an incident plane wave passes through the spiral phase plate, it produces a vortex beam with a helical phase front, causing mutual cancellation at the optical axis and forming a central dark ring.\u003c\/p\u003e\n\n\u003cp\u003eSpiral phase plates offer advantages such as high efficiency, stability, ease of operation, and a high damage threshold, making them widely applicable in optical tweezers, high-resolution microscopy, information processing, and surface topography measurement. Compared to liquid crystal polymers, UV-grade fused silica features lower absorption, making it more compatible with ultraviolet applications.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eUV fused silica material, spiral staircase structure\u003c\/li\u003e\n\u003cli\u003eApplicable for generating vortex beams with spiral phase wavefronts\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, high damage threshold\u003c\/li\u003e\n\u003cli\u003eWorking wavelength: 355 nm, 532 nm, and 1064 nm; order m: 1, 2\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003eSpiral Phase Plate Series\u003c\/h3\u003e\n\u003cp\u003eThe LBTEK spiral phase plate is fabricated from UV-grade fused silica using surface relief technology, featuring a spiral staircase structure. The standard spiral phase plate has a clear aperture of 9×9 mm and is mounted in a compatible 1-inch mechanical housing. The housing surface is engraved with the product model number.\u003c\/p\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481758974106,"sku":"VP2-532","price":1061.49,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/5-Fm2rI5Z5BbImYUGq0mEYVAYNM346_4dc2c572-d723-4e13-ab9a-8197f3f14066.jpg?v=1771995633"},{"product_id":"spiral-phase-plates-vp2-1064","title":"Spiral Phase Plates VP2-1064","description":"\u003cp\u003eThe LBTEK Spiral Phase Plate is a diffractive optical element that achieves phase modulation of light beams by varying the material height along the azimuthal direction, thereby generating vortex beams. When an incident plane wave passes through the spiral phase plate, it produces a vortex beam with a helical phase front, causing mutual cancellation at the optical axis and forming a central dark ring.\u003c\/p\u003e\n\n\u003cp\u003eSpiral phase plates offer advantages such as high efficiency, stability, ease of operation, and a high damage threshold, making them widely applicable in optical tweezers, high-resolution microscopy, information processing, and surface topography measurement. Compared to liquid crystal polymers, UV-grade fused silica features lower absorption, making it more compatible with ultraviolet applications.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eUV fused silica material, spiral staircase structure\u003c\/li\u003e\n\u003cli\u003eApplicable for generating vortex beams with spiral phase wavefronts\u003c\/li\u003e\n\u003cli\u003eHighly efficient and stable, easy to operate, high damage threshold\u003c\/li\u003e\n\u003cli\u003eWorking wavelength: 355 nm, 532 nm, and 1064 nm; order m: 1, 2\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003eSpiral Phase Plate Series\u003c\/h3\u003e\n\u003cp\u003eThe LBTEK spiral phase plate is fabricated from UV-grade fused silica using surface relief technology, featuring a spiral staircase structure. The standard spiral phase plate has a clear aperture of 9×9 mm and is mounted in a compatible 1-inch mechanical housing. The housing surface is engraved with the product model number.\u003c\/p\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481759236250,"sku":"VP2-1064","price":1061.49,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/5-Fm2rI5Z5BbImYUGq0mEYVAYNM346_0a1df405-a2cc-4b40-b4a4-6df255077a9a.jpg?v=1771995638"},{"product_id":"polymer-achromatic-vortex-retarders-avr1-vis","title":"Polymer Achromatic Vortex Retarders AVR1-VIS","description":"\u003cp\u003eThe LBTEK Achromatic Vortex Retarder utilizes N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, consisting of three layers of LCP vortex retarders designed and combined at specific angles. Each single-layer retarder features uniform radial alignment of the liquid crystal molecules' fast axis with a continuous azimuthal gradient, providing a λ\/2 retardation.\u003c\/p\u003e\n\n\u003cp\u003eThe three-layer design, stacked at designed angles, forms the overall fast axis orientation and λ\/2 retardation, enabling spatial light field modulation. The device can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00 Gaussian beams into hollow-core intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to single-wavelength retarders, the achromatic version is not limited to specific working wavelengths and is suitable for broadband light sources.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid crystal polymer\/N-BK7 window material, 3-layer glass substrate + 3-layer LCP film, with mechanical housing\u003c\/li\u003e\n\u003cli\u003eThree-layer LCP films stacked to form an achromatic vortex retarder for broadband operation\u003c\/li\u003e\n\u003cli\u003eHigh efficiency and stability, broad spectrum applicability, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength: 400-700 nm, 600-800 nm, 700-1100 nm; order m=1\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=1 Achromatic Vortex Waveplate\u003c\/h3\u003e\n\u003cp\u003eApplicable to incident light with diameters Ø0.5 to Ø21.5 mm. When illuminated with circularly polarized light, it can generate vortex beams with l=±1; under linearly polarized light, it produces vector-polarized beams including radially and azimuthally polarized beams. Conversion efficiency ≥98%.\u003c\/p\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481759400090,"sku":"AVR1-VIS","price":2774.33,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/3-FuF4fsCeUugbldLZRwxWEG1eYfDh.jpg?v=1771995641"},{"product_id":"polymer-achromatic-vortex-retarders-avr1-vnir","title":"Polymer Achromatic Vortex Retarders AVR1-VNIR","description":"\u003cp\u003eThe LBTEK Achromatic Vortex Retarder utilizes N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, consisting of three layers of LCP vortex retarders designed and combined at specific angles. Each single-layer retarder features uniform radial alignment of the liquid crystal molecules' fast axis with a continuous azimuthal gradient, providing a λ\/2 retardation.\u003c\/p\u003e\n\n\u003cp\u003eThe three-layer design, stacked at designed angles, forms the overall fast axis orientation and λ\/2 retardation, enabling spatial light field modulation. The device can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00 Gaussian beams into hollow-core intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to single-wavelength retarders, the achromatic version is not limited to specific working wavelengths and is suitable for broadband light sources.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid crystal polymer\/N-BK7 window material, 3-layer glass substrate + 3-layer LCP film, with mechanical housing\u003c\/li\u003e\n\u003cli\u003eThree-layer LCP films stacked to form an achromatic vortex retarder for broadband operation\u003c\/li\u003e\n\u003cli\u003eHigh efficiency and stability, broad spectrum applicability, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength: 400-700 nm, 600-800 nm, 700-1100 nm; order m=1\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=1 Achromatic Vortex Waveplate\u003c\/h3\u003e\n\u003cp\u003eApplicable to incident light with diameters Ø0.5 to Ø21.5 mm. When illuminated with circularly polarized light, it can generate vortex beams with l=±1; under linearly polarized light, it produces vector-polarized beams including radially and azimuthally polarized beams. Conversion efficiency ≥98%.\u003c\/p\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481759596698,"sku":"AVR1-VNIR","price":2774.33,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/3-FuF4fsCeUugbldLZRwxWEG1eYfDh_36ff261b-c687-42f7-8f01-259f8b0b1723.jpg?v=1771995645"},{"product_id":"polymer-achromatic-vortex-retarders-avr1-snir","title":"Polymer Achromatic Vortex Retarders AVR1-SNIR","description":"\u003cp\u003eThe LBTEK Achromatic Vortex Retarder utilizes N-BK7 glass substrates and Liquid Crystal Polymer (LCP) materials, consisting of three layers of LCP vortex retarders designed and combined at specific angles. Each single-layer retarder features uniform radial alignment of the liquid crystal molecules' fast axis with a continuous azimuthal gradient, providing a λ\/2 retardation.\u003c\/p\u003e\n\n\u003cp\u003eThe three-layer design, stacked at designed angles, forms the overall fast axis orientation and λ\/2 retardation, enabling spatial light field modulation. The device can generate vector-polarized beams or vortex beams with spiral phase fronts, converting TEM00 Gaussian beams into hollow-core intensity distributions.\u003c\/p\u003e\n\n\u003cp\u003eCompared to single-wavelength retarders, the achromatic version is not limited to specific working wavelengths and is suitable for broadband light sources.\u003c\/p\u003e\n\n\u003ch3\u003eKey Features\u003c\/h3\u003e\n\u003cul\u003e\n\u003cli\u003eLiquid crystal polymer\/N-BK7 window material, 3-layer glass substrate + 3-layer LCP film, with mechanical housing\u003c\/li\u003e\n\u003cli\u003eThree-layer LCP films stacked to form an achromatic vortex retarder for broadband operation\u003c\/li\u003e\n\u003cli\u003eHigh efficiency and stability, broad spectrum applicability, large incident angle\u003c\/li\u003e\n\u003cli\u003eOperating wavelength: 400-700 nm, 600-800 nm, 700-1100 nm; order m=1\u003c\/li\u003e\n\u003cli\u003eFlexible customization of parameter specifications available\u003c\/li\u003e\n\u003c\/ul\u003e\n\n\u003ch3\u003em=1 Achromatic Vortex Waveplate\u003c\/h3\u003e\n\u003cp\u003eApplicable to incident light with diameters Ø0.5 to Ø21.5 mm. When illuminated with circularly polarized light, it can generate vortex beams with l=±1; under linearly polarized light, it produces vector-polarized beams including radially and azimuthally polarized beams. Conversion efficiency ≥98%.\u003c\/p\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47481759891610,"sku":"AVR1-SNIR","price":2774.33,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/3-FuF4fsCeUugbldLZRwxWEG1eYfDh_73e653eb-6236-44d0-b819-8be1423db8e7.jpg?v=1771995648"},{"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"}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/collections\/3-FuF4fsCeUugbldLZRwxWEG1eYfDh_73e653eb-6236-44d0-b819-8be1423db8e7.jpg?v=1777783747","url":"https:\/\/waveqvanta.com\/collections\/lbtek-micro-nano-optics-vortex-retarders.oembed","provider":"WaveQuanta","version":"1.0","type":"link"}