{"title":"High Power Cylindrical Lens Array","description":null,"products":[{"product_id":"high-power-cylindrical-lens-array-mlar22-075-p10-b","title":"High Power Cylindrical Lens Array MLAR22-075-P10-B","description":"\u003ch3\u003eOverview\u003c\/h3\u003e\n\u003cp\u003eThis High Power Cylindrical Lens Array is a refractive microlens array for one-dimensional beam shaping and homogenization. Cylindrical lenslets are figured directly into a S-TIH53 substrate in a single-sided cylindrical lens array, giving a 1 mm array period and an f-number of 0.571. The 22×10.9×2 mm element offers a 20×8.9 mm clear aperture and spreads the incident beam over a 75 ° divergence angle across the 770-1070 nm operating range. Microlens focal length: 0.56 mm @808 nm; 0.571 mm @1064 nm. The element is a solid single-material S-TIH53 component with no polymer or adhesive layer in the beam path, consistent with its high-power designation.\u003c\/p\u003e\n\u003ch3\u003eApplications\u003c\/h3\u003e\n\u003cul\u003e\n  \u003cli\u003eHigh-power laser beam homogenization and flat-top profile generation\u003c\/li\u003e\n  \u003cli\u003eOne-dimensional line generation and structured illumination\u003c\/li\u003e\n  \u003cli\u003eDiode-bar and fiber-laser beam shaping\u003c\/li\u003e\n  \u003cli\u003eLaser materials processing and line-beam illumination\u003c\/li\u003e\n  \u003cli\u003eUniform illumination in lithography and imaging systems\u003c\/li\u003e\n\u003c\/ul\u003e\n\u003ch3\u003eConstruction \u0026amp; Performance\u003c\/h3\u003e\n\u003cp\u003eThe lenslets are arranged in a single-sided cylindrical lens array on a S-TIH53 blank of 22×10.9×2 mm outer dimensions, with a 0.46 mm radius of curvature per lenslet. The surfaces carry AR coating Ravg \u0026lt;1% @770 nm-1070 nm. Transmittance is \u0026gt;99%. Key specifications for this model:\u003c\/p\u003e\n\u003cul\u003e\n  \u003cli\u003e\n\u003cstrong\u003eOptical Component Size:\u003c\/strong\u003e 22×10.9×2 mm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eOperating Wavelength:\u003c\/strong\u003e 770-1070 nm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eClear Aperture:\u003c\/strong\u003e 20×8.9 mm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eDivergence Angle:\u003c\/strong\u003e 75 °\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eMaterial:\u003c\/strong\u003e S-TIH53\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eStructural Type:\u003c\/strong\u003e Single-sided cylindrical lens array\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eTransmittance:\u003c\/strong\u003e \u0026gt;99%\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eArray Period:\u003c\/strong\u003e 1 mm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eMicrolens Focal Length:\u003c\/strong\u003e 0.56 mm @808 nm; 0.571 mm @1064 nm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eF-number:\u003c\/strong\u003e 0.571\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eRadius of Curvature:\u003c\/strong\u003e 0.46 mm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eAR Coating:\u003c\/strong\u003e AR coating Ravg \u0026lt;1% @770 nm-1070 nm\u003c\/li\u003e\n\u003c\/ul\u003e\n\u003ch3\u003eStorage \u0026amp; Handling\u003c\/h3\u003e\n\u003cp\u003eHandle the array by its edges and avoid contact with the clear aperture. Keep the microlens surfaces free of dust and fingerprints; when cleaning is required, use clean optical-grade solvents and lens tissue, wiping along the lenslet axis. Note the orientation of the lenslet axis when mounting so the shaped beam lies in the intended plane. Store in the original container in a clean, dry environment, away from direct sunlight, condensation and corrosive vapors.\u003c\/p\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47717830852762,"sku":"MLAR22-075-P10-B","price":1209.39,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/high-power-cylindrical-lens-array-product.jpg?v=1785983607"},{"product_id":"high-power-cylindrical-lens-array-mlas12-110-p10-b","title":"High Power Cylindrical Lens Array MLAS12-110-P10-B","description":"\u003ch3\u003eOverview\u003c\/h3\u003e\n\u003cp\u003eThis High Power Cylindrical Lens Array is a refractive microlens array for one-dimensional beam shaping and homogenization. Cylindrical lenslets are figured directly into a S-TIH53 substrate in a single-sided cylindrical lens array, giving a 1 mm array period and an f-number of 0.305. The 12×12×2 mm element offers a 10×10 mm clear aperture and spreads the incident beam over a 110 ° divergence angle across the 790-950 nm operating range. Microlens focal length: 0.30 mm. The element is a solid single-material S-TIH53 component with no polymer or adhesive layer in the beam path, consistent with its high-power designation.\u003c\/p\u003e\n\u003ch3\u003eApplications\u003c\/h3\u003e\n\u003cul\u003e\n  \u003cli\u003eHigh-power laser beam homogenization and flat-top profile generation\u003c\/li\u003e\n  \u003cli\u003eOne-dimensional line generation and structured illumination\u003c\/li\u003e\n  \u003cli\u003eDiode-bar and fiber-laser beam shaping\u003c\/li\u003e\n  \u003cli\u003eLaser materials processing and line-beam illumination\u003c\/li\u003e\n  \u003cli\u003eUniform illumination in lithography and imaging systems\u003c\/li\u003e\n\u003c\/ul\u003e\n\u003ch3\u003eConstruction \u0026amp; Performance\u003c\/h3\u003e\n\u003cp\u003eThe lenslets are arranged in a single-sided cylindrical lens array on a S-TIH53 blank of 12×12×2 mm outer dimensions, with a 0.25 mm radius of curvature per lenslet. The surfaces carry AR coating Ravg \u0026lt;1% @790 nm-950 nm. Transmittance is \u0026gt;99%. Key specifications for this model:\u003c\/p\u003e\n\u003cul\u003e\n  \u003cli\u003e\n\u003cstrong\u003eOptical Component Size:\u003c\/strong\u003e 12×12×2 mm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eOperating Wavelength:\u003c\/strong\u003e 790-950 nm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eClear Aperture:\u003c\/strong\u003e 10×10 mm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eDivergence Angle:\u003c\/strong\u003e 110 °\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eMaterial:\u003c\/strong\u003e S-TIH53\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eStructural Type:\u003c\/strong\u003e Single-sided cylindrical lens array\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eTransmittance:\u003c\/strong\u003e \u0026gt;99%\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eArray Period:\u003c\/strong\u003e 1 mm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eMicrolens Focal Length:\u003c\/strong\u003e 0.30 mm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eF-number:\u003c\/strong\u003e 0.305\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eRadius of Curvature:\u003c\/strong\u003e 0.25 mm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eAR Coating:\u003c\/strong\u003e AR coating Ravg \u0026lt;1% @790 nm-950 nm\u003c\/li\u003e\n\u003c\/ul\u003e\n\u003ch3\u003eStorage \u0026amp; Handling\u003c\/h3\u003e\n\u003cp\u003eHandle the array by its edges and avoid contact with the clear aperture. Keep the microlens surfaces free of dust and fingerprints; when cleaning is required, use clean optical-grade solvents and lens tissue, wiping along the lenslet axis. Note the orientation of the lenslet axis when mounting so the shaped beam lies in the intended plane. Store in the original container in a clean, dry environment, away from direct sunlight, condensation and corrosive vapors.\u003c\/p\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47717833801882,"sku":"MLAS12-110-P10-B","price":1028.92,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/high-power-cylindrical-lens-array-product_650856c4-6907-43a3-a925-27a4c0badb97.jpg?v=1785983624"},{"product_id":"high-power-cylindrical-lens-array-mlas20-011-op13-b","title":"High Power Cylindrical Lens Array MLAS20-011-OP13-B","description":"\u003ch3\u003eOverview\u003c\/h3\u003e\n\u003cp\u003eThis High Power Cylindrical Lens Array is a refractive microlens array for one-dimensional beam shaping and homogenization. Cylindrical lenslets are figured directly into a UV fused silica substrate in a double-sided orthogonal cylindrical lens array, giving a 1.3 mm array period and an f-number of 5.12. The 20×20×2 mm element offers a 17.5×17.5 mm clear aperture and spreads the incident beam over a 11.21 ° divergence angle across the 790-990 nm operating range. Microlens focal length: 5.88 mm @248 nm; 6.49 mm @532 nm; 6.65 mm @1064 nm. The element is a solid single-material UV fused silica component with no polymer or adhesive layer in the beam path, consistent with its high-power designation.\u003c\/p\u003e\n\u003ch3\u003eApplications\u003c\/h3\u003e\n\u003cul\u003e\n  \u003cli\u003eHigh-power laser beam homogenization and flat-top profile generation\u003c\/li\u003e\n  \u003cli\u003eTwo-axis (orthogonal) beam spreading in a single element\u003c\/li\u003e\n  \u003cli\u003eDiode-bar and fiber-laser beam shaping\u003c\/li\u003e\n  \u003cli\u003eLaser materials processing and line-beam illumination\u003c\/li\u003e\n  \u003cli\u003eUniform illumination in lithography and imaging systems\u003c\/li\u003e\n\u003c\/ul\u003e\n\u003ch3\u003eConstruction \u0026amp; Performance\u003c\/h3\u003e\n\u003cp\u003eThe lenslets are arranged in a double-sided orthogonal cylindrical lens array on a UV fused silica blank of 20×20×2 mm outer dimensions, with a 2.99 mm radius of curvature per lenslet. The surfaces carry AR coating Ravg \u0026lt;1% @790 nm-990 nm. Transmittance is \u0026gt;99%. Key specifications for this model:\u003c\/p\u003e\n\u003cul\u003e\n  \u003cli\u003e\n\u003cstrong\u003eOptical Component Size:\u003c\/strong\u003e 20×20×2 mm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eOperating Wavelength:\u003c\/strong\u003e 790-990 nm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eClear Aperture:\u003c\/strong\u003e 17.5×17.5 mm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eDivergence Angle:\u003c\/strong\u003e 11.21 °\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eMaterial:\u003c\/strong\u003e UV fused silica\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eStructural Type:\u003c\/strong\u003e Double-sided orthogonal cylindrical lens array\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eTransmittance:\u003c\/strong\u003e \u0026gt;99%\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eArray Period:\u003c\/strong\u003e 1.3 mm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eMicrolens Focal Length:\u003c\/strong\u003e 5.88 mm @248 nm; 6.49 mm @532 nm; 6.65 mm @1064 nm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eF-number:\u003c\/strong\u003e 5.12\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eRadius of Curvature:\u003c\/strong\u003e 2.99 mm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eAR Coating:\u003c\/strong\u003e AR coating Ravg \u0026lt;1% @790 nm-990 nm\u003c\/li\u003e\n\u003c\/ul\u003e\n\u003ch3\u003eStorage \u0026amp; Handling\u003c\/h3\u003e\n\u003cp\u003eHandle the array by its edges and avoid contact with the clear aperture. Keep the microlens surfaces free of dust and fingerprints; when cleaning is required, use clean optical-grade solvents and lens tissue, wiping along the lenslet axis. Note the orientation of the lenslet axis when mounting so the shaped beam lies in the intended plane. Store in the original container in a clean, dry environment, away from direct sunlight, condensation and corrosive vapors.\u003c\/p\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47717838192794,"sku":"MLAS20-011-OP13-B","price":2800.48,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/high-power-cylindrical-lens-array-product_c38b567c-1ca4-489c-a5fb-f0b5fcc6a498.jpg?v=1785983646"},{"product_id":"high-power-cylindrical-lens-array-mlas35-005-op13-n","title":"High Power Cylindrical Lens Array MLAS35-005-OP13-N","description":"\u003ch3\u003eOverview\u003c\/h3\u003e\n\u003cp\u003eThis High Power Cylindrical Lens Array is a refractive microlens array for one-dimensional beam shaping and homogenization. Cylindrical lenslets are figured directly into a UV fused silica substrate in a double-sided orthogonal cylindrical lens array, giving a 1.3 mm array period and an f-number of 11.15. The 35×35×2 mm element offers a 32.5×32.5 mm clear aperture and spreads the incident beam over a 5.16 ° divergence angle across the 200-2100 nm operating range. Microlens focal length: 12.8 mm @248 nm; 14.1 mm @532 nm; 14.5 mm @1064 nm. The element is a solid single-material UV fused silica component with no polymer or adhesive layer in the beam path, consistent with its high-power designation.\u003c\/p\u003e\n\u003ch3\u003eApplications\u003c\/h3\u003e\n\u003cul\u003e\n  \u003cli\u003eHigh-power laser beam homogenization and flat-top profile generation\u003c\/li\u003e\n  \u003cli\u003eTwo-axis (orthogonal) beam spreading in a single element\u003c\/li\u003e\n  \u003cli\u003eDiode-bar and fiber-laser beam shaping\u003c\/li\u003e\n  \u003cli\u003eLaser materials processing and line-beam illumination\u003c\/li\u003e\n  \u003cli\u003eUniform illumination in lithography and imaging systems\u003c\/li\u003e\n\u003c\/ul\u003e\n\u003ch3\u003eConstruction \u0026amp; Performance\u003c\/h3\u003e\n\u003cp\u003eThe lenslets are arranged in a double-sided orthogonal cylindrical lens array on a UV fused silica blank of 35×35×2 mm outer dimensions, with a 6.5 mm radius of curvature per lenslet. The surfaces are left uncoated, which keeps the damage threshold as high as the bare substrate allows. Transmittance is \u0026gt;90% @248-1064 nm. Key specifications for this model:\u003c\/p\u003e\n\u003cul\u003e\n  \u003cli\u003e\n\u003cstrong\u003eOptical Component Size:\u003c\/strong\u003e 35×35×2 mm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eOperating Wavelength:\u003c\/strong\u003e 200-2100 nm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eClear Aperture:\u003c\/strong\u003e 32.5×32.5 mm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eDivergence Angle:\u003c\/strong\u003e 5.16 °\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eMaterial:\u003c\/strong\u003e UV fused silica\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eStructural Type:\u003c\/strong\u003e Double-sided orthogonal cylindrical lens array\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eTransmittance:\u003c\/strong\u003e \u0026gt;90% @248-1064 nm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eArray Period:\u003c\/strong\u003e 1.3 mm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eMicrolens Focal Length:\u003c\/strong\u003e 12.8 mm @248 nm; 14.1 mm @532 nm; 14.5 mm @1064 nm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eF-number:\u003c\/strong\u003e 11.15\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eRadius of Curvature:\u003c\/strong\u003e 6.5 mm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eAR Coating:\u003c\/strong\u003e No Coating\u003c\/li\u003e\n\u003c\/ul\u003e\n\u003ch3\u003eStorage \u0026amp; Handling\u003c\/h3\u003e\n\u003cp\u003eHandle the array by its edges and avoid contact with the clear aperture. Keep the microlens surfaces free of dust and fingerprints; when cleaning is required, use clean optical-grade solvents and lens tissue, wiping along the lenslet axis. Note the orientation of the lenslet axis when mounting so the shaped beam lies in the intended plane. Store in the original container in a clean, dry environment, away from direct sunlight, condensation and corrosive vapors.\u003c\/p\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47717842649242,"sku":"MLAS35-005-OP13-N","price":8766.52,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/high-power-cylindrical-lens-array-product_fc2a08fc-7bf7-4936-9896-e88811ba1d77.jpg?v=1785983670"},{"product_id":"high-power-cylindrical-lens-array-mlas35-005-p13-b","title":"High Power Cylindrical Lens Array MLAS35-005-P13-B","description":"\u003ch3\u003eOverview\u003c\/h3\u003e\n\u003cp\u003eThis High Power Cylindrical Lens Array is a refractive microlens array for one-dimensional beam shaping and homogenization. Cylindrical lenslets are figured directly into a UV fused silica substrate in a single-sided cylindrical lens array, giving a 1.3 mm array period and an f-number of 14.38. The 35×35×2 mm element offers a 32.5×32.5 mm clear aperture and spreads the incident beam over a 4.99 ° divergence angle across the 900-1100 nm operating range. Microlens focal length: 16.5 mm @248 nm; 18.2 mm @532 nm; 18.7 mm @1064 nm. The element is a solid single-material UV fused silica component with no polymer or adhesive layer in the beam path, consistent with its high-power designation.\u003c\/p\u003e\n\u003ch3\u003eApplications\u003c\/h3\u003e\n\u003cul\u003e\n  \u003cli\u003eHigh-power laser beam homogenization and flat-top profile generation\u003c\/li\u003e\n  \u003cli\u003eOne-dimensional line generation and structured illumination\u003c\/li\u003e\n  \u003cli\u003eDiode-bar and fiber-laser beam shaping\u003c\/li\u003e\n  \u003cli\u003eLaser materials processing and line-beam illumination\u003c\/li\u003e\n  \u003cli\u003eUniform illumination in lithography and imaging systems\u003c\/li\u003e\n\u003c\/ul\u003e\n\u003ch3\u003eConstruction \u0026amp; Performance\u003c\/h3\u003e\n\u003cp\u003eThe lenslets are arranged in a single-sided cylindrical lens array on a UV fused silica blank of 35×35×2 mm outer dimensions, with a 8.4 mm radius of curvature per lenslet. The surfaces carry AR coating Ravg \u0026lt;1% @900 nm-1100 nm. Transmittance is \u0026gt;99%. Key specifications for this model:\u003c\/p\u003e\n\u003cul\u003e\n  \u003cli\u003e\n\u003cstrong\u003eOptical Component Size:\u003c\/strong\u003e 35×35×2 mm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eOperating Wavelength:\u003c\/strong\u003e 900-1100 nm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eClear Aperture:\u003c\/strong\u003e 32.5×32.5 mm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eDivergence Angle:\u003c\/strong\u003e 4.99 °\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eMaterial:\u003c\/strong\u003e UV fused silica\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eStructural Type:\u003c\/strong\u003e Single-sided cylindrical lens array\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eTransmittance:\u003c\/strong\u003e \u0026gt;99%\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eArray Period:\u003c\/strong\u003e 1.3 mm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eMicrolens Focal Length:\u003c\/strong\u003e 16.5 mm @248 nm; 18.2 mm @532 nm; 18.7 mm @1064 nm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eF-number:\u003c\/strong\u003e 14.38\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eRadius of Curvature:\u003c\/strong\u003e 8.4 mm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eAR Coating:\u003c\/strong\u003e AR coating Ravg \u0026lt;1% @900 nm-1100 nm\u003c\/li\u003e\n\u003c\/ul\u003e\n\u003ch3\u003eStorage \u0026amp; Handling\u003c\/h3\u003e\n\u003cp\u003eHandle the array by its edges and avoid contact with the clear aperture. Keep the microlens surfaces free of dust and fingerprints; when cleaning is required, use clean optical-grade solvents and lens tissue, wiping along the lenslet axis. Note the orientation of the lenslet axis when mounting so the shaped beam lies in the intended plane. Store in the original container in a clean, dry environment, away from direct sunlight, condensation and corrosive vapors.\u003c\/p\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47717845729434,"sku":"MLAS35-005-P13-B","price":6862.21,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/high-power-cylindrical-lens-array-product_ce778504-d42e-481d-89b6-9af641a99db4.jpg?v=1785983687"},{"product_id":"high-power-cylindrical-lens-array-mlas35-005-p13-n","title":"High Power Cylindrical Lens Array MLAS35-005-P13-N","description":"\u003ch3\u003eOverview\u003c\/h3\u003e\n\u003cp\u003eThis High Power Cylindrical Lens Array is a refractive microlens array for one-dimensional beam shaping and homogenization. Cylindrical lenslets are figured directly into a UV fused silica substrate in a single-sided cylindrical lens array, giving a 1.3 mm array period and an f-number of 11.15. The 35×35×2 mm element offers a 32.5×32.5 mm clear aperture and spreads the incident beam over a 5.16 ° divergence angle across the 200-2100 nm operating range. Microlens focal length: 12.8 mm @248 nm; 14.1 mm @532 nm; 14.5 mm @1064 nm. The element is a solid single-material UV fused silica component with no polymer or adhesive layer in the beam path, consistent with its high-power designation.\u003c\/p\u003e\n\u003ch3\u003eApplications\u003c\/h3\u003e\n\u003cul\u003e\n  \u003cli\u003eHigh-power laser beam homogenization and flat-top profile generation\u003c\/li\u003e\n  \u003cli\u003eOne-dimensional line generation and structured illumination\u003c\/li\u003e\n  \u003cli\u003eDiode-bar and fiber-laser beam shaping\u003c\/li\u003e\n  \u003cli\u003eLaser materials processing and line-beam illumination\u003c\/li\u003e\n  \u003cli\u003eUniform illumination in lithography and imaging systems\u003c\/li\u003e\n\u003c\/ul\u003e\n\u003ch3\u003eConstruction \u0026amp; Performance\u003c\/h3\u003e\n\u003cp\u003eThe lenslets are arranged in a single-sided cylindrical lens array on a UV fused silica blank of 35×35×2 mm outer dimensions, with a 6.5 mm radius of curvature per lenslet. The surfaces are left uncoated, which keeps the damage threshold as high as the bare substrate allows. Transmittance is \u0026gt;90% @248-1064 nm. Key specifications for this model:\u003c\/p\u003e\n\u003cul\u003e\n  \u003cli\u003e\n\u003cstrong\u003eOptical Component Size:\u003c\/strong\u003e 35×35×2 mm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eOperating Wavelength:\u003c\/strong\u003e 200-2100 nm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eClear Aperture:\u003c\/strong\u003e 32.5×32.5 mm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eDivergence Angle:\u003c\/strong\u003e 5.16 °\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eMaterial:\u003c\/strong\u003e UV fused silica\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eStructural Type:\u003c\/strong\u003e Single-sided cylindrical lens array\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eTransmittance:\u003c\/strong\u003e \u0026gt;90% @248-1064 nm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eArray Period:\u003c\/strong\u003e 1.3 mm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eMicrolens Focal Length:\u003c\/strong\u003e 12.8 mm @248 nm; 14.1 mm @532 nm; 14.5 mm @1064 nm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eF-number:\u003c\/strong\u003e 11.15\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eRadius of Curvature:\u003c\/strong\u003e 6.5 mm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eAR Coating:\u003c\/strong\u003e No Coating\u003c\/li\u003e\n\u003c\/ul\u003e\n\u003ch3\u003eStorage \u0026amp; Handling\u003c\/h3\u003e\n\u003cp\u003eHandle the array by its edges and avoid contact with the clear aperture. Keep the microlens surfaces free of dust and fingerprints; when cleaning is required, use clean optical-grade solvents and lens tissue, wiping along the lenslet axis. Note the orientation of the lenslet axis when mounting so the shaped beam lies in the intended plane. Store in the original container in a clean, dry environment, away from direct sunlight, condensation and corrosive vapors.\u003c\/p\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47717849366682,"sku":"MLAS35-005-P13-N","price":5600.95,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/high-power-cylindrical-lens-array-product_bfba67a1-9e46-4750-a694-5e3f7ce38970.jpg?v=1785983702"},{"product_id":"high-power-cylindrical-lens-array-mlas35-011-op13-n","title":"High Power Cylindrical Lens Array MLAS35-011-OP13-N","description":"\u003ch3\u003eOverview\u003c\/h3\u003e\n\u003cp\u003eThis High Power Cylindrical Lens Array is a refractive microlens array for one-dimensional beam shaping and homogenization. Cylindrical lenslets are figured directly into a UV fused silica substrate in a double-sided orthogonal cylindrical lens array, giving a 1.3 mm array period and an f-number of 5.12. The 35×35×2 mm element offers a 32.5×32.5 mm clear aperture and spreads the incident beam over a 11.21 ° divergence angle across the 200-2100 nm operating range. Microlens focal length: 5.88 mm @248 nm; 6.49 mm @532 nm; 6.65 mm @1064 nm. The element is a solid single-material UV fused silica component with no polymer or adhesive layer in the beam path, consistent with its high-power designation.\u003c\/p\u003e\n\u003ch3\u003eApplications\u003c\/h3\u003e\n\u003cul\u003e\n  \u003cli\u003eHigh-power laser beam homogenization and flat-top profile generation\u003c\/li\u003e\n  \u003cli\u003eTwo-axis (orthogonal) beam spreading in a single element\u003c\/li\u003e\n  \u003cli\u003eDiode-bar and fiber-laser beam shaping\u003c\/li\u003e\n  \u003cli\u003eLaser materials processing and line-beam illumination\u003c\/li\u003e\n  \u003cli\u003eUniform illumination in lithography and imaging systems\u003c\/li\u003e\n\u003c\/ul\u003e\n\u003ch3\u003eConstruction \u0026amp; Performance\u003c\/h3\u003e\n\u003cp\u003eThe lenslets are arranged in a double-sided orthogonal cylindrical lens array on a UV fused silica blank of 35×35×2 mm outer dimensions, with a 2.99 mm radius of curvature per lenslet. The surfaces are left uncoated, which keeps the damage threshold as high as the bare substrate allows. Transmittance is \u0026gt;90% @248-1064 nm. Key specifications for this model:\u003c\/p\u003e\n\u003cul\u003e\n  \u003cli\u003e\n\u003cstrong\u003eOptical Component Size:\u003c\/strong\u003e 35×35×2 mm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eOperating Wavelength:\u003c\/strong\u003e 200-2100 nm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eClear Aperture:\u003c\/strong\u003e 32.5×32.5 mm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eDivergence Angle:\u003c\/strong\u003e 11.21 °\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eMaterial:\u003c\/strong\u003e UV fused silica\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eStructural Type:\u003c\/strong\u003e Double-sided orthogonal cylindrical lens array\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eTransmittance:\u003c\/strong\u003e \u0026gt;90% @248-1064 nm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eArray Period:\u003c\/strong\u003e 1.3 mm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eMicrolens Focal Length:\u003c\/strong\u003e 5.88 mm @248 nm; 6.49 mm @532 nm; 6.65 mm @1064 nm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eF-number:\u003c\/strong\u003e 5.12\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eRadius of Curvature:\u003c\/strong\u003e 2.99 mm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eAR Coating:\u003c\/strong\u003e No Coating\u003c\/li\u003e\n\u003c\/ul\u003e\n\u003ch3\u003eStorage \u0026amp; Handling\u003c\/h3\u003e\n\u003cp\u003eHandle the array by its edges and avoid contact with the clear aperture. Keep the microlens surfaces free of dust and fingerprints; when cleaning is required, use clean optical-grade solvents and lens tissue, wiping along the lenslet axis. Note the orientation of the lenslet axis when mounting so the shaped beam lies in the intended plane. Store in the original container in a clean, dry environment, away from direct sunlight, condensation and corrosive vapors.\u003c\/p\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47717854347418,"sku":"MLAS35-011-OP13-N","price":9013.38,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/high-power-cylindrical-lens-array-product_eb81f794-3727-4d65-abf7-4ea7416d1c57.jpg?v=1785983723"},{"product_id":"high-power-cylindrical-lens-array-mlas35-011-p13-n","title":"High Power Cylindrical Lens Array MLAS35-011-P13-N","description":"\u003ch3\u003eOverview\u003c\/h3\u003e\n\u003cp\u003eThis High Power Cylindrical Lens Array is a refractive microlens array for one-dimensional beam shaping and homogenization. Cylindrical lenslets are figured directly into a UV fused silica substrate in a single-sided cylindrical lens array, giving a 1.3 mm array period and an f-number of 5.12. The 35×35×2 mm element offers a 32.5×32.5 mm clear aperture and spreads the incident beam over a 11.21 ° divergence angle across the 200-2100 nm operating range. Microlens focal length: 5.88 mm @248 nm; 6.49 mm @532 nm; 6.65 mm @1064 nm. The element is a solid single-material UV fused silica component with no polymer or adhesive layer in the beam path, consistent with its high-power designation.\u003c\/p\u003e\n\u003ch3\u003eApplications\u003c\/h3\u003e\n\u003cul\u003e\n  \u003cli\u003eHigh-power laser beam homogenization and flat-top profile generation\u003c\/li\u003e\n  \u003cli\u003eOne-dimensional line generation and structured illumination\u003c\/li\u003e\n  \u003cli\u003eDiode-bar and fiber-laser beam shaping\u003c\/li\u003e\n  \u003cli\u003eLaser materials processing and line-beam illumination\u003c\/li\u003e\n  \u003cli\u003eUniform illumination in lithography and imaging systems\u003c\/li\u003e\n\u003c\/ul\u003e\n\u003ch3\u003eConstruction \u0026amp; Performance\u003c\/h3\u003e\n\u003cp\u003eThe lenslets are arranged in a single-sided cylindrical lens array on a UV fused silica blank of 35×35×2 mm outer dimensions, with a 2.99 mm radius of curvature per lenslet. The surfaces are left uncoated, which keeps the damage threshold as high as the bare substrate allows. Transmittance is \u0026gt;90% @248-1064 nm. Key specifications for this model:\u003c\/p\u003e\n\u003cul\u003e\n  \u003cli\u003e\n\u003cstrong\u003eOptical Component Size:\u003c\/strong\u003e 35×35×2 mm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eOperating Wavelength:\u003c\/strong\u003e 200-2100 nm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eClear Aperture:\u003c\/strong\u003e 32.5×32.5 mm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eDivergence Angle:\u003c\/strong\u003e 11.21 °\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eMaterial:\u003c\/strong\u003e UV fused silica\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eStructural Type:\u003c\/strong\u003e Single-sided cylindrical lens array\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eTransmittance:\u003c\/strong\u003e \u0026gt;90% @248-1064 nm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eArray Period:\u003c\/strong\u003e 1.3 mm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eMicrolens Focal Length:\u003c\/strong\u003e 5.88 mm @248 nm; 6.49 mm @532 nm; 6.65 mm @1064 nm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eF-number:\u003c\/strong\u003e 5.12\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eRadius of Curvature:\u003c\/strong\u003e 2.99 mm\u003c\/li\u003e\n  \u003cli\u003e\n\u003cstrong\u003eAR Coating:\u003c\/strong\u003e No Coating\u003c\/li\u003e\n\u003c\/ul\u003e\n\u003ch3\u003eStorage \u0026amp; Handling\u003c\/h3\u003e\n\u003cp\u003eHandle the array by its edges and avoid contact with the clear aperture. Keep the microlens surfaces free of dust and fingerprints; when cleaning is required, use clean optical-grade solvents and lens tissue, wiping along the lenslet axis. Note the orientation of the lenslet axis when mounting so the shaped beam lies in the intended plane. Store in the original container in a clean, dry environment, away from direct sunlight, condensation and corrosive vapors.\u003c\/p\u003e","brand":"WaveQuanta","offers":[{"title":"Default Title","offer_id":47717858771098,"sku":"MLAS35-011-P13-N","price":5600.95,"currency_code":"SGD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/files\/high-power-cylindrical-lens-array-product_ed53ab74-94a7-4a48-8864-e453945654f3.jpg?v=1785983740"}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0734\/6156\/3546\/collections\/high-power-cylindrical-lens-array-product_d62eb04d-2f00-4a22-a940-134118609c24.jpg?v=1785984339","url":"https:\/\/waveqvanta.com\/collections\/lbtek-micro-nano-optics-homogenizer-high-power-cylindrical-lens-array.oembed","provider":"WaveQuanta","version":"1.0","type":"link"}