宽带介质膜 λ/10 反射镜
宽带介质膜 λ/10 反射镜TECHSPEC Broadband Dielectric λ/10 Mirrors为广泛的波长范围提供大于99%的反射率专为入射角是0 – 45°的所有偏振状态而设计采用熔融石英基底,具备优异的热稳定性TECHSPEC® 宽带介质膜λ/10反射镜非常适用于使用多个激光光源的光束偏转或反射应用。这类使用介质膜方式的光学反射镜具有超过99%的反射率,远高于金属镀膜反射镜,能通过最小化能量损失来提高系统性能。此熔融石英基片高度耐用,可提供极低的热膨胀系数,并具有高耐磨性。TECHSPEC® 宽带介质膜λ/10反射镜专为从紫外到近红外光谱范围的应用而设计.通用规格表面平整度:λ/10基底:Fused Silica表面质量:20-10镀膜类型:Dielectric入射角 (°):0-45有效孔径 (%):90产品信息涂层规格波长范围(nm)Dia. (mm)产品编码Ravg98% @ 340 - 488nm (0°, All Polarizations)Ravg98% @ 320 - 450nm (45°, All Polarizations)Ravg99% @ 320 - 450nm (45°, S-Polarization)320 - 4505.00#37-558Ravg98% @ 340 - 488nm (0°, All Polarizations)Ravg98% @ 320 - 450nm (45°, All Polarizations)Ravg99% @ 320 - 450nm (45°, S-Polarization)320 - 4506.35#39-190Ravg98% @ 340 - 488nm (0°, All Polarizations)Ravg98% @ 320 - 450nm (45°, All Polarizations)Ravg99% @ 320 - 450nm (45°, S-Polarization)320 - 45010.00#37-559Ravg98% @ 340 - 488nm (0°, All Polarizations)Ravg98% @ 320 - 450nm (45°, All Polarizations)Ravg99% @ 320 - 450nm (45°, S-Polarization)320 - 45012.50#37-560Ravg98% @ 340 - 488nm (0°, All Polarizations)Ravg98% @ 320 - 450nm (45°, All Polarizations)Ravg99% @ 320 - 450nm (45°, S-Polarization)320 - 45012.70#39-389Ravg98% @ 340 - 488nm (0°, All Polarizations)Ravg98% @ 320 - 450nm (45°, All Polarizations)Ravg99% @ 320 - 450nm (45°, S-Polarization)320 - 45015.00#37-562Ravg98% @ 340 - 488nm (0°, All Polarizations)Ravg98% @ 320 - 450nm (45°, All Polarizations)Ravg99% @ 320 - 450nm (45°, S-Polarization)320 - 45019.10#39-204Ravg98% @ 340 - 488nm (0°, All Polarizations)Ravg98% @ 320 - 450nm (45°, All Polarizations)Ravg99% @ 320 - 450nm (45°, S-Polarization)320 - 45020.00#37-563Ravg98% @ 340 - 488nm (0°, All Polarizations)Ravg98% @ 320 - 450nm (45°, All Polarizations)Ravg99% @ 320 - 450nm (45°, S-Polarization)320 - 45025.00#37-564Ravg98% @ 340 - 488nm (0°, All Polarizations)Ravg98% @ 320 - 450nm (45°, All Polarizations)Ravg99% @ 320 - 450nm (45°, S-Polarization)320 - 45025.40#39-390Ravg98% @ 340 - 488nm (0°, All Polarizations)Ravg98% @ 320 - 450nm (45°, All Polarizations)Ravg99% @ 320 - 450nm (45°, S-Polarization)320 - 45030.00#37-568Ravg98% @ 340 - 488nm (0°, All Polarizations)Ravg98% @ 320 - 450nm (45°, All Polarizations)Ravg99% @ 320 - 450nm (45°, S-Polarization)320 - 45035.00#37-569Ravg98% @ 340 - 488nm (0°, All Polarizations)Ravg98% @ 320 - 450nm (45°, All Polarizations)Ravg99% @ 320 - 450nm (45°, S-Polarization)320 - 45038.10#39-218Ravg98% @ 340 - 488nm (0°, All Polarizations)Ravg98% @ 320 - 450nm (45°, All Polarizations)Ravg99% @ 320 - 450nm (45°, S-Polarization)320 - 45040.00#37-570Ravg98% @ 340 - 488nm (0°, All Polarizations)Ravg98% @ 320 - 450nm (45°, All Polarizations)Ravg99% @ 320 - 450nm (45°, S-Polarization)320 - 45050.00#37-571Ravg98% @ 340 - 488nm (0°, All Polarizations)Ravg98% @ 320 - 450nm (45°, All Polarizations)Ravg99% @ 320 - 450nm (45°, S-Polarization)320 - 45050.80#39-225Ravg98% @ 400 - 750nm (0 - 45°)Ravg99% @ 400 - 750nm (0°)400 - 7505.00#87-366Ravg98% @ 400 - 750nm (0 - 45°)Ravg99% @ 400 - 750nm (0°)400 - 7506.35#39-191Ravg98% @ 400 - 750nm (0 - 45°)Ravg99% @ 400 - 750nm (0°)400 - 75010.00#87-367Ravg98% @ 400 - 750nm (0 - 45°)Ravg99% @ 400 - 750nm (0°)400 - 75012.50#87-368Ravg98% @ 400 - 750nm (0 - 45°)Ravg99% @ 400 - 750nm (0°)400 - 75012.70#39-198Ravg98% @ 400 - 750nm (0 - 45°)Ravg99% @ 400 - 750nm (0°)400 - 75015.00#87-369Ravg98% @ 400 - 750nm (0 - 45°)Ravg99% @ 400 - 750nm (0°)400 - 75019.10#39-205Ravg98% @ 400 - 750nm (0 - 45°)Ravg99% @ 400 - 750nm (0°)400 - 75020.00#87-370Ravg98% @ 400 - 750nm (0 - 45°)Ravg99% @ 400 - 750nm (0°)400 - 75025.00#87-371Ravg98% @ 400 - 750nm (0 - 45°)Ravg99% @ 400 - 750nm (0°)400 - 75025.40#39-212Ravg98% @ 400 - 750nm (0 - 45°)Ravg99% @ 400 - 750nm (0°)400 - 75030.00#87-372Ravg98% @ 400 - 750nm (0 - 45°)Ravg99% @ 400 - 750nm (0°)400 - 75035.00#87-373Ravg98% @ 400 - 750nm (0 - 45°)Ravg99% @ 400 - 750nm (0°)400 - 75038.10#39-219Ravg98% @ 400 - 750nm (0 - 45°)Ravg99% @ 400 - 750nm (0°)400 - 75040.00#87-374Ravg98% @ 400 - 750nm (0 - 45°)Ravg99% @ 400 - 750nm (0°)400 - 75050.00#33-188Ravg98% @ 400 - 750nm (0 - 45°)Ravg99% @ 400 - 750nm (0°)400 - 75050.80#39-226Ravg98% @ 750 - 1100nm (0 - 45°)Ravg99% @ 750 - 1100nm (0°)750 - 11005.00#87-376Ravg98% @ 750 - 1100nm (0 - 45°)Ravg99% @ 750 - 1100nm (0°)750 - 11006.35#39-192Ravg98% @ 750 - 1100nm (0 - 45°)Ravg99% @ 750 - 1100nm (0°)750 - 110010.00#87-377Ravg98% @ 750 - 1100nm (0 - 45°)Ravg99% @ 750 - 1100nm (0°)750 - 110012.50#87-378Ravg98% @ 750 - 1100nm (0 - 45°)Ravg99% @ 750 - 1100nm (0°)750 - 110012.70#39-199Ravg98% @ 750 - 1100nm (0 - 45°)Ravg99% @ 750 - 1100nm (0°)750 - 110015.00#87-379Ravg98% @ 750 - 1100nm (0 - 45°)Ravg99% @ 750 - 1100nm (0°)750 - 110019.10#39-206Ravg98% @ 750 - 1100nm (0 - 45°)Ravg99% @ 750 - 1100nm (0°)750 - 110020.00#87-380Ravg98% @ 750 - 1100nm (0 - 45°)Ravg99% @ 750 - 1100nm (0°)750 - 110025.00#87-381Ravg98% @ 750 - 1100nm (0 - 45°)Ravg99% @ 750 - 1100nm (0°)750 - 110025.40#39-213Ravg98% @ 750 - 1100nm (0 - 45°)Ravg99% @ 750 - 1100nm (0°)750 - 110030.00#87-382Ravg98% @ 750 - 1100nm (0 - 45°)Ravg99% @ 750 - 1100nm (0°)750 - 110035.00#87-383Ravg98% @ 750 - 1100nm (0 - 45°)Ravg99% @ 750 - 1100nm (0°)750 - 110038.10#39-220Ravg98% @ 750 - 1100nm (0 - 45°)Ravg99% @ 750 - 1100nm (0°)750 - 110040.00#87-384Ravg98% @ 750 - 1100nm (0 - 45°)Ravg99% @ 750 - 1100nm (0°)750 - 110050.00#33-189Ravg98% @ 750 - 1100nm (0 - 45°)Ravg99% @ 750 - 1100nm (0°)750 - 110050.80#39-227