{"title":"SWIR Telecentric Lens","description":"\u003cp class=\"PDq2pG_selectionAnchorContainer\"\u003eThe SWIR Telecentric Lens Series is designed for precision imaging with SWIR cameras, offering \u003cstrong\u003e400–1200nm\u003c\/strong\u003e and \u003cstrong\u003e950–1800nm\u003c\/strong\u003e wavelength options. With a \u003cstrong\u003e1.1\" image circle\u003c\/strong\u003e and \u003cstrong\u003e0.5–4.0× magnification\u003c\/strong\u003e, it provides stable, low-distortion imaging for demanding inspection and measurement applications.\u003cspan class=\"PDq2pG_selectionAnchor\"\u003e\u003c\/span\u003e\u003c\/p\u003e\n\u003cp\u003eAvailable with a \u003cstrong\u003eC-mount\u003c\/strong\u003e, these lenses are an excellent match for \u003cstrong\u003eSony IMX990\u003c\/strong\u003e and \u003cstrong\u003e1.1\" InGaAs SWIR sensors\u003c\/strong\u003e, making them suitable for semiconductor inspection, precision measurement, and advanced SWIR machine vision.\u003c\/p\u003e","products":[{"product_id":"j-visible-swir-telecentric-lens-focus-shift-correction","title":"400–1200 nm Visible-SWIR Telecentric Lens | Focus Shift Correction TLVS-H1.1","description":"\u003ch2\u003eProduct Description\u003c\/h2\u003e\n\u003cp\u003eThe Visible-SWIR Telecentric Lens Series is designed for high-precision imaging across a broad spectral range from 400–1200 nm, enabling seamless imaging from visible light to SWIR without refocusing. Featuring advanced focus shift correction, these lenses maintain sharp images across wavelengths, making them ideal for applications requiring both visible and near-infrared imaging.\u003c\/p\u003e\n\u003cp\u003eAvailable in 0.7×, 1×, 2×, and 4× magnifications, the series supports image circles up to Φ24 mm and offers both coaxial and non-coaxial illumination configurations. By eliminating focal shifts between visible and SWIR wavelengths, these telecentric lenses reveal material differences and defects that are difficult or impossible to detect with visible light alone.\u003c\/p\u003e\n\u003cp\u003eDesigned for machine vision, semiconductor inspection, solar cell analysis, and scientific imaging, the Visible-SWIR Telecentric Lens Series provides reliable, distortion-free imaging for demanding industrial applications.\u003c\/p\u003e\n\u003ch2\u003eKey Features\u003cbr\u003e\n\u003c\/h2\u003e\n\u003cul\u003e\n\u003cli\u003eBroad spectral range: 400–1200 nm\u003c\/li\u003e\n\u003cli\u003eFocus shift correction from visible to SWIR\u003c\/li\u003e\n\u003cli\u003eNo refocusing required between visible and SWIR imaging\u003c\/li\u003e\n\u003cli\u003eMagnification options: 0.7×, 1×, 2×, 4×\u003c\/li\u003e\n\u003cli\u003eImage circle up to Φ24 mm\u003c\/li\u003e\n\u003cli\u003eCoaxial and non-coaxial illumination versions available\u003c\/li\u003e\n\u003cli\u003eHigh-contrast, low-distortion telecentric optics\u003c\/li\u003e\n\u003cli\u003eSuitable for industrial and scientific imaging\u003cbr\u003e\n\u003c\/li\u003e\n\u003c\/ul\u003e\n\u003ch2\u003eMain Applications\u003cbr\u003e\n\u003c\/h2\u003e\n\u003cul\u003e\n\u003cli\u003eSemiconductor inspection\u003c\/li\u003e\n\u003cli\u003eSolar cell and wafer inspection\u003c\/li\u003e\n\u003cli\u003eMaterial identification\u003c\/li\u003e\n\u003cli\u003eDisplay and glass inspection\u003c\/li\u003e\n\u003cli\u003ePCB and electronics inspection\u003c\/li\u003e\n\u003cli\u003ePrecision measurement and metrology\u003c\/li\u003e\n\u003cli\u003eScientific and laboratory imaging\u003c\/li\u003e\n\u003cli\u003eDefect detection beyond visible wavelengths\u003c\/li\u003e\n\u003c\/ul\u003e\n\u003ch2\u003eSpecifications\u003cspan style=\"color: rgb(255, 42, 0);\"\u003e\u003c\/span\u003e\n\u003c\/h2\u003e\n\u003ctable style=\"width: 99.964%; height: 203.4px;\"\u003e\n\u003cthead\u003e\n\u003ctr style=\"height: 39.2px;\"\u003e\n\u003cth style=\"text-align: center; width: 25.6022%; height: 39.2px;\"\u003eModel\u003c\/th\u003e\n\u003cth style=\"text-align: center; width: 15.9787%; height: 39.2px;\"\u003eMag.\u003c\/th\u003e\n\u003cth style=\"text-align: center; width: 16.3265%; height: 39.2px;\"\u003eWD\u003c\/th\u003e\n\u003cth style=\"text-align: center; width: 22.5308%; height: 39.2px;\"\u003eImage Circle\u003c\/th\u003e\n\u003cth style=\"text-align: center; width: 18.8839%; height: 39.2px;\"\u003eCoaxial\u003c\/th\u003e\n\u003c\/tr\u003e\n\u003c\/thead\u003e\n\u003ctbody\u003e\n\u003ctr style=\"height: 21.2px;\"\u003e\n\u003ctd style=\"text-align: center; width: 25.6022%; height: 21.2px;\"\u003eTLVS-0.7XD-H1.1\u003c\/td\u003e\n\u003ctd style=\"text-align: center; width: 15.9787%; height: 21.2px;\"\u003e0.7X\u003c\/td\u003e\n\u003ctd style=\"text-align: center; width: 16.3265%; height: 21.2px;\"\u003e110 mm\u003c\/td\u003e\n\u003ctd style=\"text-align: center; width: 22.5308%; height: 21.2px;\"\u003eΦ20.5 mm\u003c\/td\u003e\n\u003ctd style=\"text-align: center; width: 18.8839%; height: 21.2px;\"\u003eYes\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr style=\"height: 19.6px;\"\u003e\n\u003ctd style=\"text-align: center; width: 25.6022%; height: 19.6px;\"\u003eTLVS-0.7X-H1.1\u003c\/td\u003e\n\u003ctd style=\"text-align: center; width: 15.9787%; height: 19.6px;\"\u003e0.7X\u003c\/td\u003e\n\u003ctd style=\"text-align: center; width: 16.3265%; height: 19.6px;\"\u003e110 mm\u003c\/td\u003e\n\u003ctd style=\"text-align: center; width: 22.5308%; height: 19.6px;\"\u003eΦ20.5 mm\u003c\/td\u003e\n\u003ctd style=\"text-align: center; width: 18.8839%; height: 19.6px;\"\u003eNo\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr style=\"height: 21.2px;\"\u003e\n\u003ctd style=\"text-align: center; width: 25.6022%; height: 21.2px;\"\u003eTLVS-1.0XD-H1.1\u003c\/td\u003e\n\u003ctd style=\"text-align: center; width: 15.9787%; height: 21.2px;\"\u003e1.0X\u003c\/td\u003e\n\u003ctd style=\"text-align: center; width: 16.3265%; height: 21.2px;\"\u003e110 mm\u003c\/td\u003e\n\u003ctd style=\"text-align: center; width: 22.5308%; height: 21.2px;\"\u003eΦ24 mm\u003c\/td\u003e\n\u003ctd style=\"text-align: center; width: 18.8839%; height: 21.2px;\"\u003eYes\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr style=\"height: 19.6px;\"\u003e\n\u003ctd style=\"text-align: center; width: 25.6022%; height: 19.6px;\"\u003eTLVS-1.0X-H1.1\u003c\/td\u003e\n\u003ctd style=\"text-align: center; width: 15.9787%; height: 19.6px;\"\u003e1.0X\u003c\/td\u003e\n\u003ctd style=\"text-align: center; width: 16.3265%; height: 19.6px;\"\u003e110 mm\u003c\/td\u003e\n\u003ctd style=\"text-align: center; width: 22.5308%; height: 19.6px;\"\u003eΦ24 mm\u003c\/td\u003e\n\u003ctd style=\"text-align: center; width: 18.8839%; height: 19.6px;\"\u003eNo\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr style=\"height: 20.2px;\"\u003e\n\u003ctd style=\"text-align: center; width: 25.6022%; height: 20.2px;\"\u003eTLVS-2.0XD-H1.1\u003c\/td\u003e\n\u003ctd style=\"text-align: center; width: 15.9787%; height: 20.2px;\"\u003e2.0X\u003c\/td\u003e\n\u003ctd style=\"text-align: center; width: 16.3265%; height: 20.2px;\"\u003e110 mm\u003c\/td\u003e\n\u003ctd style=\"text-align: center; width: 22.5308%; height: 20.2px;\"\u003eΦ24 mm\u003c\/td\u003e\n\u003ctd style=\"text-align: center; width: 18.8839%; height: 20.2px;\"\u003eYes\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr style=\"height: 19.6px;\"\u003e\n\u003ctd style=\"text-align: center; width: 25.6022%; height: 19.6px;\"\u003eTLVS-2.0X-H1.1\u003c\/td\u003e\n\u003ctd style=\"text-align: center; width: 15.9787%; height: 19.6px;\"\u003e2.0X\u003c\/td\u003e\n\u003ctd style=\"text-align: center; width: 16.3265%; height: 19.6px;\"\u003e110 mm\u003c\/td\u003e\n\u003ctd style=\"text-align: center; width: 22.5308%; height: 19.6px;\"\u003eΦ24 mm\u003c\/td\u003e\n\u003ctd style=\"text-align: center; width: 18.8839%; height: 19.6px;\"\u003eNo\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr style=\"height: 23.2px;\"\u003e\n\u003ctd style=\"text-align: center; width: 25.6022%; height: 23.2px;\"\u003eTLVS-4.0XD-H1.1\u003c\/td\u003e\n\u003ctd style=\"text-align: center; width: 15.9787%; height: 23.2px;\"\u003e4.0X\u003c\/td\u003e\n\u003ctd style=\"text-align: center; width: 16.3265%; height: 23.2px;\"\u003e110 mm\u003c\/td\u003e\n\u003ctd style=\"text-align: center; width: 22.5308%; height: 23.2px;\"\u003eΦ20.5 mm\u003c\/td\u003e\n\u003ctd style=\"text-align: center; width: 18.8839%; height: 23.2px;\"\u003eYes\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr style=\"height: 19.6px;\"\u003e\n\u003ctd style=\"text-align: center; width: 25.6022%; height: 19.6px;\"\u003eTLVS-4.0X-H1.1\u003c\/td\u003e\n\u003ctd style=\"text-align: center; width: 15.9787%; height: 19.6px;\"\u003e4.0X\u003c\/td\u003e\n\u003ctd style=\"text-align: center; width: 16.3265%; height: 19.6px;\"\u003e110 mm\u003c\/td\u003e\n\u003ctd style=\"text-align: center; width: 22.5308%; height: 19.6px;\"\u003eΦ20.5 mm\u003c\/td\u003e\n\u003ctd style=\"text-align: center; width: 18.8839%; height: 19.6px;\"\u003eNo\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\n\u003c\/table\u003e\n\u003cdiv style=\"text-align: start;\"\u003e\u003cimg src=\"https:\/\/cdn.shopify.com\/s\/files\/1\/0655\/5490\/7394\/files\/6_a072c416-d7f3-4daa-b7cf-688bc96d0cf6.jpg?v=1700619683\" alt='applications of 1.1\" vis swir telecentric lens' style=\"float: none;\"\u003e\u003c\/div\u003e\n\u003cp\u003e\u003ciframe width=\"560\" height=\"315\" src=\"https:\/\/www.youtube.com\/embed\/xYVWKmiUWrk?si=AtkjBJIMjvdJevca\" title=\"YouTube video player\"\u003e\u003c\/iframe\u003e\u003c\/p\u003e","brand":"Vision Datum","offers":[{"title":"0.7x WD: 110mm \/ Coaxial","offer_id":46594807595266,"sku":"TLVS-0.7XD-H1.1","price":6900.0,"currency_code":"USD","in_stock":true},{"title":"0.7x WD: 110mm \/ Non-Coaxial","offer_id":46595044212994,"sku":"TLVS-0.7X-H1.1","price":6800.0,"currency_code":"USD","in_stock":true},{"title":"1.0x WD: 110mm \/ Coaxial","offer_id":48035056910594,"sku":"TLVS-1.0XD-H1.1","price":6900.0,"currency_code":"USD","in_stock":true},{"title":"1.0x WD: 110mm \/ Non-Coaxial","offer_id":48035056943362,"sku":"TLVS-1.0X-H1.1","price":6800.0,"currency_code":"USD","in_stock":true},{"title":"2.0x WD: 110mm \/ Coaxial","offer_id":48035056976130,"sku":"TLVS-2.0XD-H1.1","price":6900.0,"currency_code":"USD","in_stock":true},{"title":"2.0x WD: 110mm \/ Non-Coaxial","offer_id":48035057008898,"sku":"TLVS-2.0X-H1.1","price":6800.0,"currency_code":"USD","in_stock":true},{"title":"4.0x WD: 110mm \/ Coaxial","offer_id":48035057041666,"sku":"TLVS-4.0XD-H1.1","price":6900.0,"currency_code":"USD","in_stock":true},{"title":"4.0x WD: 110mm \/ Non-Coaxial","offer_id":48035057074434,"sku":"TLVS-4.0X-H1.1","price":6800.0,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0655\/5490\/7394\/files\/400-1200-nm-visible-swir-telecentric-lens-focus-shift-correction-tlvs-h11-5190441.jpg?v=1783299311"},{"product_id":"j-tlsw-h1-1-swir-telecentric-lens-series-950-1800nm","title":"TLSW-H1.1 SWIR Telecentric Lens Series | 950–1800nm for 1.1\" InGaAs Sensors","description":"\u003ch2\u003eProduct Description\u003c\/h2\u003e\n\u003cp\u003eThe TLSW Series SWIR Telecentric Lenses are optimized for 1.1\" InGaAs sensors, including the Sony IMX990, delivering high-precision imaging across the 950–1800 nm spectral range. Available in 0.5×, 0.7×, 1×, 2×, and 4× magnifications, these lenses reveal material differences and defects invisible to visible-light systems.\u003c\/p\u003e\n\u003cp\u003eDesigned for machine vision and precision metrology, the TLSW Series offers ultra-low distortion, high resolution, and both coaxial and non-coaxial configurations. The 1× and 2× models feature adjustable iris control for flexible depth-of-field optimization. Compatible with SWIR cameras and C-Mount systems, these lenses are ideal for semiconductor inspection, wafer analysis, solar cell inspection, and scientific imaging applications.\u003c\/p\u003e\n\u003ch2\u003eKey Features\u003cbr\u003e\n\u003c\/h2\u003e\n\u003cul\u003e\n\u003cli\u003eOptimized for Sony IMX990 and 1.1\" InGaAs sensors\u003c\/li\u003e\n\u003cli\u003eSWIR transmission from 950–1800 nm\u003c\/li\u003e\n\u003cli\u003eMagnifications from 0.5× to 4×\u003c\/li\u003e\n\u003cli\u003eUltra-low distortion and high resolution\u003c\/li\u003e\n\u003cli\u003eCoaxial and non-coaxial versions available\u003c\/li\u003e\n\u003cli\u003eAdjustable iris on 1× and 2× models\u003c\/li\u003e\n\u003cli\u003eC-Mount interface for easy integration\u003c\/li\u003e\n\u003cli\u003eSuitable for precision measurement and SWIR inspection\u003cbr\u003e\n\u003c\/li\u003e\n\u003c\/ul\u003e\n\u003ch2\u003eMain Applications\u003cbr\u003e\n\u003c\/h2\u003e\n\u003cul\u003e\n\u003cli\u003eSemiconductor and wafer inspection\u003c\/li\u003e\n\u003cli\u003eSolar cell and photovoltaic analysis\u003c\/li\u003e\n\u003cli\u003ePrecision metrology\u003c\/li\u003e\n\u003cli\u003eElectronics inspection\u003c\/li\u003e\n\u003cli\u003eMaterial identification\u003c\/li\u003e\n\u003cli\u003eSWIR machine vision\u003c\/li\u003e\n\u003cli\u003eScientific imaging and research\u003c\/li\u003e\n\u003c\/ul\u003e\n\u003ch2\u003eSpecifications\u003c\/h2\u003e\n\u003cp\u003e\u003cstrong\u003e1.1\" C-Mount 950-1800nm SWIR Telecentric Lens\u003c\/strong\u003e\u003c\/p\u003e\n\u003ctable style=\"width: 99.964%; height: 156.8px;\"\u003e\n\u003cthead\u003e\n\u003ctr style=\"height: 19.6px;\"\u003e\n\u003cth style=\"text-align: center; width: 29.2337%; height: 19.6px;\"\u003eModel\u003c\/th\u003e\n\u003cth align=\"center\" style=\"text-align: center; width: 14.1629%; height: 19.6px;\"\u003eCoaxial\u003c\/th\u003e\n\u003cth align=\"center\" style=\"text-align: center; width: 12.8919%; height: 19.6px;\"\u003eMag.\u003c\/th\u003e\n\u003cth align=\"center\" style=\"text-align: center; width: 16.1686%; height: 19.6px;\"\u003eWD\u003c\/th\u003e\n\u003cth align=\"center\" style=\"text-align: center; width: 10.8862%; height: 19.6px;\"\u003eF\/#\u003c\/th\u003e\n\u003cth align=\"center\" style=\"text-align: center; width: 15.7971%; height: 19.6px;\"\u003eDOF\u003c\/th\u003e\n\u003c\/tr\u003e\n\u003c\/thead\u003e\n\u003ctbody\u003e\n\u003ctr style=\"height: 19.6px;\"\u003e\n\u003ctd style=\"text-align: center; width: 29.2337%; height: 19.6px;\"\u003e\u003cstrong\u003eTLSW-0.5XD-H1.1\u003c\/strong\u003e\u003c\/td\u003e\n\u003ctd align=\"center\" style=\"text-align: center; width: 14.1629%; height: 19.6px;\"\u003eYes\u003c\/td\u003e\n\u003ctd align=\"center\" style=\"text-align: center; width: 12.8919%; height: 19.6px;\"\u003e0.5×\u003c\/td\u003e\n\u003ctd align=\"center\" style=\"text-align: center; width: 16.1686%; height: 19.6px;\"\u003e116.4mm\u003c\/td\u003e\n\u003ctd align=\"center\" style=\"text-align: center; width: 10.8862%; height: 19.6px;\"\u003e6.3\u003c\/td\u003e\n\u003ctd align=\"center\" style=\"text-align: center; width: 15.7971%; height: 19.6px;\"\u003e2.02mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr style=\"height: 19.6px;\"\u003e\n\u003ctd style=\"text-align: center; width: 29.2337%; height: 19.6px;\"\u003e\u003cstrong\u003eTLSW-0.7XD-H1.1\u003c\/strong\u003e\u003c\/td\u003e\n\u003ctd align=\"center\" style=\"text-align: center; width: 14.1629%; height: 19.6px;\"\u003eYes\u003c\/td\u003e\n\u003ctd align=\"center\" style=\"text-align: center; width: 12.8919%; height: 19.6px;\"\u003e0.7×\u003c\/td\u003e\n\u003ctd align=\"center\" style=\"text-align: center; width: 16.1686%; height: 19.6px;\"\u003e116.0mm\u003c\/td\u003e\n\u003ctd align=\"center\" style=\"text-align: center; width: 10.8862%; height: 19.6px;\"\u003e6.4\u003c\/td\u003e\n\u003ctd align=\"center\" style=\"text-align: center; width: 15.7971%; height: 19.6px;\"\u003e1.05mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr style=\"height: 19.6px;\"\u003e\n\u003ctd style=\"text-align: center; width: 29.2337%; height: 19.6px;\"\u003e\u003cstrong\u003eTLSW-1.0XD-H1.1\u003c\/strong\u003e\u003c\/td\u003e\n\u003ctd align=\"center\" style=\"text-align: center; width: 14.1629%; height: 19.6px;\"\u003eYes\u003c\/td\u003e\n\u003ctd align=\"center\" style=\"text-align: center; width: 12.8919%; height: 19.6px;\"\u003e1.0×\u003c\/td\u003e\n\u003ctd align=\"center\" style=\"text-align: center; width: 16.1686%; height: 19.6px;\"\u003e110.0mm\u003c\/td\u003e\n\u003ctd align=\"center\" style=\"text-align: center; width: 10.8862%; height: 19.6px;\"\u003e7.0\u003c\/td\u003e\n\u003ctd align=\"center\" style=\"text-align: center; width: 15.7971%; height: 19.6px;\"\u003e0.56mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr style=\"height: 19.6px;\"\u003e\n\u003ctd style=\"text-align: center; width: 29.2337%; height: 19.6px;\"\u003e\u003cstrong\u003eTLSW-1.0X-H1.1\u003c\/strong\u003e\u003c\/td\u003e\n\u003ctd align=\"center\" style=\"text-align: center; width: 14.1629%; height: 19.6px;\"\u003eNo\u003c\/td\u003e\n\u003ctd align=\"center\" style=\"text-align: center; width: 12.8919%; height: 19.6px;\"\u003e1.0×\u003c\/td\u003e\n\u003ctd align=\"center\" style=\"text-align: center; width: 16.1686%; height: 19.6px;\"\u003e110.0mm\u003c\/td\u003e\n\u003ctd align=\"center\" style=\"text-align: center; width: 10.8862%; height: 19.6px;\"\u003e7.0\u003c\/td\u003e\n\u003ctd align=\"center\" style=\"text-align: center; width: 15.7971%; height: 19.6px;\"\u003e0.56mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr style=\"height: 19.6px;\"\u003e\n\u003ctd style=\"text-align: center; width: 29.2337%; height: 19.6px;\"\u003e\u003cstrong\u003eTLSW-2.0XD-H1.1\u003c\/strong\u003e\u003c\/td\u003e\n\u003ctd align=\"center\" style=\"text-align: center; width: 14.1629%; height: 19.6px;\"\u003eYes\u003c\/td\u003e\n\u003ctd align=\"center\" style=\"text-align: center; width: 12.8919%; height: 19.6px;\"\u003e2.0×\u003c\/td\u003e\n\u003ctd align=\"center\" style=\"text-align: center; width: 16.1686%; height: 19.6px;\"\u003e110.2mm\u003c\/td\u003e\n\u003ctd align=\"center\" style=\"text-align: center; width: 10.8862%; height: 19.6px;\"\u003e11.5\u003c\/td\u003e\n\u003ctd align=\"center\" style=\"text-align: center; width: 15.7971%; height: 19.6px;\"\u003e0.23mm\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr style=\"height: 19.6px;\"\u003e\n\u003ctd style=\"text-align: center; width: 29.2337%; height: 19.6px;\"\u003e\u003cstrong\u003eTLSW-2.0X-H1.1\u003c\/strong\u003e\u003c\/td\u003e\n\u003ctd align=\"center\" style=\"text-align: center; width: 14.1629%; height: 19.6px;\"\u003eNo\u003c\/td\u003e\n\u003ctd align=\"center\" style=\"text-align: center; width: 12.8919%; height: 19.6px;\"\u003e2.0×\u003c\/td\u003e\n\u003ctd align=\"center\" style=\"text-align: center; 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