产品描述
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.
| 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 |
Ravg>98% @ 340 - 488nm (0°, All Polarizations) Ravg>98% @ 320 - 450nm (45°, All Polarizations) Ravg>99% @ 320 - 450nm (45°, S-Polarization) | 320 - 450 | 5.00 | #37-558 |
Ravg>98% @ 340 - 488nm (0°, All Polarizations) Ravg>98% @ 320 - 450nm (45°, All Polarizations) Ravg>99% @ 320 - 450nm (45°, S-Polarization) | 320 - 450 | 6.35 | #39-190 |
Ravg>98% @ 340 - 488nm (0°, All Polarizations) Ravg>98% @ 320 - 450nm (45°, All Polarizations) Ravg>99% @ 320 - 450nm (45°, S-Polarization) | 320 - 450 | 10.00 | #37-559 |
Ravg>98% @ 340 - 488nm (0°, All Polarizations) Ravg>98% @ 320 - 450nm (45°, All Polarizations) Ravg>99% @ 320 - 450nm (45°, S-Polarization) | 320 - 450 | 12.50 | #37-560 |
Ravg>98% @ 340 - 488nm (0°, All Polarizations) Ravg>98% @ 320 - 450nm (45°, All Polarizations) Ravg>99% @ 320 - 450nm (45°, S-Polarization) | 320 - 450 | 12.70 | #39-389 |
Ravg>98% @ 340 - 488nm (0°, All Polarizations) Ravg>98% @ 320 - 450nm (45°, All Polarizations) Ravg>99% @ 320 - 450nm (45°, S-Polarization) | 320 - 450 | 15.00 | #37-562 |
Ravg>98% @ 340 - 488nm (0°, All Polarizations) Ravg>98% @ 320 - 450nm (45°, All Polarizations) Ravg>99% @ 320 - 450nm (45°, S-Polarization) | 320 - 450 | 19.10 | #39-204 |
Ravg>98% @ 340 - 488nm (0°, All Polarizations) Ravg>98% @ 320 - 450nm (45°, All Polarizations) Ravg>99% @ 320 - 450nm (45°, S-Polarization) | 320 - 450 | 20.00 | #37-563 |
Ravg>98% @ 340 - 488nm (0°, All Polarizations) Ravg>98% @ 320 - 450nm (45°, All Polarizations) Ravg>99% @ 320 - 450nm (45°, S-Polarization) | 320 - 450 | 25.00 | #37-564 |
Ravg>98% @ 340 - 488nm (0°, All Polarizations) Ravg>98% @ 320 - 450nm (45°, All Polarizations) Ravg>99% @ 320 - 450nm (45°, S-Polarization) | 320 - 450 | 25.40 | #39-390 |
Ravg>98% @ 340 - 488nm (0°, All Polarizations) Ravg>98% @ 320 - 450nm (45°, All Polarizations) Ravg>99% @ 320 - 450nm (45°, S-Polarization) | 320 - 450 | 30.00 | #37-568 |
Ravg>98% @ 340 - 488nm (0°, All Polarizations) Ravg>98% @ 320 - 450nm (45°, All Polarizations) Ravg>99% @ 320 - 450nm (45°, S-Polarization) | 320 - 450 | 35.00 | #37-569 |
Ravg>98% @ 340 - 488nm (0°, All Polarizations) Ravg>98% @ 320 - 450nm (45°, All Polarizations) Ravg>99% @ 320 - 450nm (45°, S-Polarization) | 320 - 450 | 38.10 | #39-218 |
Ravg>98% @ 340 - 488nm (0°, All Polarizations) Ravg>98% @ 320 - 450nm (45°, All Polarizations) Ravg>99% @ 320 - 450nm (45°, S-Polarization) | 320 - 450 | 40.00 | #37-570 |
Ravg>98% @ 340 - 488nm (0°, All Polarizations) Ravg>98% @ 320 - 450nm (45°, All Polarizations) Ravg>99% @ 320 - 450nm (45°, S-Polarization) | 320 - 450 | 50.00 | #37-571 |
Ravg>98% @ 340 - 488nm (0°, All Polarizations) Ravg>98% @ 320 - 450nm (45°, All Polarizations) Ravg>99% @ 320 - 450nm (45°, S-Polarization) | 320 - 450 | 50.80 | #39-225 |
Ravg>98% @ 400 - 750nm (0 - 45°) Ravg>99% @ 400 - 750nm (0°) | 400 - 750 | 5.00 | #87-366 |
Ravg>98% @ 400 - 750nm (0 - 45°) Ravg>99% @ 400 - 750nm (0°) | 400 - 750 | 6.35 | #39-191 |
Ravg>98% @ 400 - 750nm (0 - 45°) Ravg>99% @ 400 - 750nm (0°) | 400 - 750 | 10.00 | #87-367 |
Ravg>98% @ 400 - 750nm (0 - 45°) Ravg>99% @ 400 - 750nm (0°) | 400 - 750 | 12.50 | #87-368 |
Ravg>98% @ 400 - 750nm (0 - 45°) Ravg>99% @ 400 - 750nm (0°) | 400 - 750 | 12.70 | #39-198 |
Ravg>98% @ 400 - 750nm (0 - 45°) Ravg>99% @ 400 - 750nm (0°) | 400 - 750 | 15.00 | #87-369 |
Ravg>98% @ 400 - 750nm (0 - 45°) Ravg>99% @ 400 - 750nm (0°) | 400 - 750 | 19.10 | #39-205 |
Ravg>98% @ 400 - 750nm (0 - 45°) Ravg>99% @ 400 - 750nm (0°) | 400 - 750 | 20.00 | #87-370 |
Ravg>98% @ 400 - 750nm (0 - 45°) Ravg>99% @ 400 - 750nm (0°) | 400 - 750 | 25.00 | #87-371 |
Ravg>98% @ 400 - 750nm (0 - 45°) Ravg>99% @ 400 - 750nm (0°) | 400 - 750 | 25.40 | #39-212 |
Ravg>98% @ 400 - 750nm (0 - 45°) Ravg>99% @ 400 - 750nm (0°) | 400 - 750 | 30.00 | #87-372 |
Ravg>98% @ 400 - 750nm (0 - 45°) Ravg>99% @ 400 - 750nm (0°) | 400 - 750 | 35.00 | #87-373 |
Ravg>98% @ 400 - 750nm (0 - 45°) Ravg>99% @ 400 - 750nm (0°) | 400 - 750 | 38.10 | #39-219 |
Ravg>98% @ 400 - 750nm (0 - 45°) Ravg>99% @ 400 - 750nm (0°) | 400 - 750 | 40.00 | #87-374 |
Ravg>98% @ 400 - 750nm (0 - 45°) Ravg>99% @ 400 - 750nm (0°) | 400 - 750 | 50.00 | #33-188 |
Ravg>98% @ 400 - 750nm (0 - 45°) Ravg>99% @ 400 - 750nm (0°) | 400 - 750 | 50.80 | #39-226 |
Ravg>98% @ 750 - 1100nm (0 - 45°) Ravg>99% @ 750 - 1100nm (0°) | 750 - 1100 | 5.00 | #87-376 |
Ravg>98% @ 750 - 1100nm (0 - 45°) Ravg>99% @ 750 - 1100nm (0°) | 750 - 1100 | 6.35 | #39-192 |
Ravg>98% @ 750 - 1100nm (0 - 45°) Ravg>99% @ 750 - 1100nm (0°) | 750 - 1100 | 10.00 | #87-377 |
Ravg>98% @ 750 - 1100nm (0 - 45°) Ravg>99% @ 750 - 1100nm (0°) | 750 - 1100 | 12.50 | #87-378 |
Ravg>98% @ 750 - 1100nm (0 - 45°) Ravg>99% @ 750 - 1100nm (0°) | 750 - 1100 | 12.70 | #39-199 |
Ravg>98% @ 750 - 1100nm (0 - 45°) Ravg>99% @ 750 - 1100nm (0°) | 750 - 1100 | 15.00 | #87-379 |
Ravg>98% @ 750 - 1100nm (0 - 45°) Ravg>99% @ 750 - 1100nm (0°) | 750 - 1100 | 19.10 | #39-206 |
Ravg>98% @ 750 - 1100nm (0 - 45°) Ravg>99% @ 750 - 1100nm (0°) | 750 - 1100 | 20.00 | #87-380 |
Ravg>98% @ 750 - 1100nm (0 - 45°) Ravg>99% @ 750 - 1100nm (0°) | 750 - 1100 | 25.00 | #87-381 |
Ravg>98% @ 750 - 1100nm (0 - 45°) Ravg>99% @ 750 - 1100nm (0°) | 750 - 1100 | 25.40 | #39-213 |
Ravg>98% @ 750 - 1100nm (0 - 45°) Ravg>99% @ 750 - 1100nm (0°) | 750 - 1100 | 30.00 | #87-382 |
Ravg>98% @ 750 - 1100nm (0 - 45°) Ravg>99% @ 750 - 1100nm (0°) | 750 - 1100 | 35.00 | #87-383 |
Ravg>98% @ 750 - 1100nm (0 - 45°) Ravg>99% @ 750 - 1100nm (0°) | 750 - 1100 | 38.10 | #39-220 |
Ravg>98% @ 750 - 1100nm (0 - 45°) Ravg>99% @ 750 - 1100nm (0°) | 750 - 1100 | 40.00 | #87-384 |
Ravg>98% @ 750 - 1100nm (0 - 45°) Ravg>99% @ 750 - 1100nm (0°) | 750 - 1100 | 50.00 | #33-189 |
Ravg>98% @ 750 - 1100nm (0 - 45°) Ravg>99% @ 750 - 1100nm (0°) | 750 - 1100 | 50.80 | #39-227 |
