{"product_id":"t-ps851-n-sf11-equilateral-dispersive-prism-10-mm","title":"T-PS851 - N-SF11 Equilateral Dispersive Prism, 10 mm","description":"\u003cp\u003eT-PS851 - N-SF11 Equilateral Dispersive Prism, 10 mm\u003c\/p\u003e\n\u003cp\u003eN-SF11 is a flint glass that offers excellent performance in the visible and NIR spectral range. It offers a high refractive index and low Abbe number, making it excellent for use in an equilateral dispersive prism.\u003c\/p\u003e\n\u003cp\u003e\u003cstrong\u003ePolarization Effects\u003c\/strong\u003e\u003cbr\u003eFor P-Polarized light (blue line) incident on a dispersing prism at the angle of least deviation, the graph to the right shows that only a small percentage of the P-polarized light is reflected at the surface. Thus, for this polarization, the transmission through a prism fabricated from N-SF11, a RoHS-compliant version of SF11, will be excellent even though there is no AR coating on the surface.\u003c\/p\u003e\n\u003ctable cellspacing=\"0\" width=\"375\" class=\"SpecTable\"\u003e\n\u003cthead\u003e\n\u003ctr\u003e\n\u003cth align=\"left\" id=\"th1289CBB80000\"\u003eMaterial\u003c\/th\u003e\n\u003cth id=\"th1289CBB80001\"\u003eWavelength Range\u003c\/th\u003e\n\u003cth id=\"th1289CBB80002\"\u003eIndex of Refraction\u003c\/th\u003e\n\u003cth id=\"th1289CBB80003\"\u003eAbbe Number\u003c\/th\u003e\n\u003c\/tr\u003e\n\u003c\/thead\u003e\n\u003ctbody\u003e\n\u003ctr\u003e\n\u003ctd headers=\"th1289CBB80000\"\u003e\u003cstrong\u003eF2\u003c\/strong\u003e\u003c\/td\u003e\n\u003ctd align=\"center\" headers=\"th1289CBB80001\"\u003e385 nm - 2 µm\u003c\/td\u003e\n\u003ctd align=\"center\" headers=\"th1289CBB80002\"\u003e1.617 @ 633 nm\u003c\/td\u003e\n\u003ctd align=\"center\" headers=\"th1289CBB80003\"\u003e36.37\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003ctd headers=\"th1289CBB80000\"\u003e\u003cstrong\u003eN-F2\u003c\/strong\u003e\u003c\/td\u003e\n\u003ctd align=\"center\" headers=\"th1289CBB80001\"\u003e420 nm - 2 µm\u003c\/td\u003e\n\u003ctd align=\"center\" headers=\"th1289CBB80002\"\u003e1.617 @ 633 nm\u003c\/td\u003e\n\u003ctd align=\"center\" headers=\"th1289CBB80003\"\u003e36.43\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr align=\"left\" valign=\"top\"\u003e\n\u003ctd headers=\"th1289CBB80000\"\u003e\u003cstrong\u003eN-SF11\u003c\/strong\u003e\u003c\/td\u003e\n\u003ctd align=\"center\" headers=\"th1289CBB80001\"\u003e420 nm - 2.3 µm\u003c\/td\u003e\n\u003ctd align=\"center\" headers=\"th1289CBB80002\"\u003e1.779 @ 633 nm\u003c\/td\u003e\n\u003ctd align=\"center\" headers=\"th1289CBB80003\"\u003e25.76\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr align=\"left\" valign=\"top\"\u003e\n\u003ctd headers=\"th1289CBB80000\"\u003e\u003cstrong\u003eCaF\u003csub\u003e2\u003c\/sub\u003e\u003c\/strong\u003e\u003c\/td\u003e\n\u003ctd align=\"center\" headers=\"th1289CBB80001\"\u003e180 nm - 8 µm\u003c\/td\u003e\n\u003ctd align=\"center\" headers=\"th1289CBB80002\"\u003e1.433 @ 633 nm\u003c\/td\u003e\n\u003ctd align=\"center\" headers=\"th1289CBB80003\"\u003e95.00\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr align=\"left\" valign=\"top\"\u003e\n\u003ctd headers=\"th1289CBB80000\"\u003e\u003cstrong\u003eZnSe\u003c\/strong\u003e\u003c\/td\u003e\n\u003ctd align=\"center\" headers=\"th1289CBB80001\"\u003e600 nm - 16 µm\u003c\/td\u003e\n\u003ctd align=\"center\" headers=\"th1289CBB80002\"\u003e2.403 @ 10.6 µm\u003c\/td\u003e\n\u003ctd align=\"center\" headers=\"th1289CBB80003\"\u003eN\/A\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\n\u003c\/table\u003e\n\u003cp\u003e \u003c\/p\u003e\n\u003ctable width=\"600\" class=\"SpecTable\" cellspacing=\"0\"\u003e\n\u003cthead\u003e\n\u003ctr\u003e\n\u003cth valign=\"bottom\" id=\"th13DFEE700000\" align=\"left\"\u003eItem #\u003c\/th\u003e\n\u003cth valign=\"bottom\" id=\"th13DFEE700001\" align=\"center\"\u003eA=B=C=H\u003cbr\u003e(mm)\u003c\/th\u003e\n\u003cth valign=\"bottom\" id=\"th13DFEE700002\" align=\"center\"\u003eMaterial\u003c\/th\u003e\n\u003cth id=\"th13DFEE700003\" align=\"center\"\u003eMinimum Angle\u003cbr\u003eof Deviation\u003c\/th\u003e\n\u003cth valign=\"bottom\" id=\"th13DFEE700004\" align=\"center\"\u003eV\u003c\/th\u003e\n\u003cth id=\"th13DFEE700005\" align=\"center\"\u003eSurface Flatness\u003cbr\u003e@ 633 nm\u003c\/th\u003e\n\u003c\/tr\u003e\n\u003c\/thead\u003e\n\u003ctbody\u003e\n\u003ctr\u003e\n\u003ctd valign=\"top\" headers=\"th13DFEE700000\" align=\"left\"\u003e\u003cstrong\u003eT-PS850\u003c\/strong\u003e\u003c\/td\u003e\n\u003ctd valign=\"top\" headers=\"th13DFEE700001\" align=\"center\"\u003e10 ± 0.15\u003c\/td\u003e\n\u003ctd rowspan=\"2\" headers=\"th13DFEE700002\" align=\"center\"\u003eF2\u003c\/td\u003e\n\u003ctd rowspan=\"2\" headers=\"th13DFEE700003\" align=\"center\"\u003e47.9° @ 633 nm\u003c\/td\u003e\n\u003ctd rowspan=\"2\" headers=\"th13DFEE700004\" align=\"center\"\u003e36.37\u003c\/td\u003e\n\u003ctd rowspan=\"2\" headers=\"th13DFEE700005\" align=\"center\"\u003eλ\/10\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003ctd valign=\"top\" headers=\"th13DFEE700000\" align=\"left\"\u003e\u003cstrong\u003eT-PS852\u003c\/strong\u003e\u003c\/td\u003e\n\u003ctd valign=\"top\" headers=\"th13DFEE700001\" align=\"center\"\u003e25 ± 0.15\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr class=\"subtle\"\u003e\n\u003ctd valign=\"top\" headers=\"th13DFEE700000\" align=\"left\"\u003e\u003cstrong\u003eT-PS856\u003c\/strong\u003e\u003c\/td\u003e\n\u003ctd valign=\"top\" headers=\"th13DFEE700001\" align=\"center\"\u003e15 ± 0.15\u003c\/td\u003e\n\u003ctd rowspan=\"3\" headers=\"th13DFEE700002\" align=\"center\"\u003eN-F2\u003c\/td\u003e\n\u003ctd rowspan=\"3\" headers=\"th13DFEE700003\" align=\"center\"\u003e47.9° @ 633 nm\u003c\/td\u003e\n\u003ctd rowspan=\"3\" headers=\"th13DFEE700004\" align=\"center\"\u003e36.43\u003c\/td\u003e\n\u003ctd rowspan=\"3\" headers=\"th13DFEE700005\" align=\"center\"\u003eλ\/10\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr class=\"subtle\"\u003e\n\u003ctd valign=\"top\" headers=\"th13DFEE700000\" align=\"left\"\u003e\u003cstrong\u003eT-PS858\u003c\/strong\u003e\u003c\/td\u003e\n\u003ctd valign=\"top\" headers=\"th13DFEE700001\" align=\"center\"\u003e20 ± 0.15\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr class=\"subtle\"\u003e\n\u003ctd valign=\"top\" headers=\"th13DFEE700000\" align=\"left\"\u003e\u003cstrong\u003eT-PS854\u003c\/strong\u003e\u003c\/td\u003e\n\u003ctd valign=\"top\" headers=\"th13DFEE700001\" align=\"center\"\u003e50 ± 0.15\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003ctr\u003e\n\u003ctd valign=\"top\" headers=\"th13DFEE700000\" align=\"left\"\u003e\u003cstrong\u003eT-PS851\u003c\/strong\u003e\u003c\/td\u003e\n\u003ctd valign=\"top\" headers=\"th13DFEE700001\" align=\"center\"\u003e10 ± 0.15\u003c\/td\u003e\n\u003ctd rowspan=\"5\" headers=\"th13DFEE700002\" align=\"center\"\u003eN-SF11\u003c\/td\u003e\n\u003ctd rowspan=\"5\" headers=\"th13DFEE700003\" align=\"center\"\u003e65.6° @ 633 nm\u003c\/td\u003e\n\u003ctd rowspan=\"5\" headers=\"th13DFEE700004\" align=\"center\"\u003e25.76\u003c\/td\u003e\n\u003ctd rowspan=\"5\" headers=\"th13DFEE700005\" align=\"center\"\u003eλ\/10\u003c\/td\u003e\n\u003c\/tr\u003e\n\u003c\/tbody\u003e\n\u003c\/table\u003e","brand":"Fosco Connect","offers":[{"title":"Default Title","offer_id":49083590443264,"sku":"T-PS851","price":268.6,"currency_code":"USD","in_stock":true}],"thumbnail_url":"\/\/cdn.shopify.com\/s\/files\/1\/0388\/5331\/2557\/files\/4238-xl.jpg?v=1785202055","url":"https:\/\/alotechparts.com\/products\/t-ps851-n-sf11-equilateral-dispersive-prism-10-mm","provider":"Alo Tech Solutions","version":"1.0","type":"link"}