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电话：15933752505
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硒化锌 （ZnSe） 平凸 （PCX） 透镜
由爱特蒙特光学设计，II-VI 材料制成
优质等级的硒化锌材料
无镀膜或宽带抗反射镀膜选项
TECHSPEC? 硒化锌 (ZnSe) 平凸?(PCX) 透镜的设计用于中波和长波红外光谱中的聚焦或准直应用。这些透镜由 II-VI 红外硒化锌材料制成，在 10.6μm 波长上的体积吸收系数为 <0.0005cm-1，可提供无镀膜或多种宽带抗反射镀膜选项。8-12μm 镀膜非常适合与 CO2?激光器和热感照相机应用搭配使用，而双波段的 3-12μm 镀膜则适用于高光谱应用。TECHSPEC??硒化锌平凸透镜在 10.6μm 波长上的不规则性为 <λ/20 ，表面质量为 40-20，表面粗糙度 <50?。提供三种直径选项，有效焦距范围从 12.7mm 到 200mm。
硒化锌 （ZnSe） 平凸 （PCX） 透镜通用规格
| 基底?: | II-VI Infrared ZnSe |
| 表面质量?: | 40-20 |
| Power (P-V) @ 632.8nm?: | λ/10 |
| Irregularity (P-V) @ 632.8nm?: | λ/20 |
| 有效孔径 CA（mm）?: | 90 |
| 焦距波长 (nm)?: | 10.6 |
| Bulk Absorption Coefficient (cm1)?: | <0.0005 @ 10.6μm |
订购信息
| Dia.(mm) | EFL (mm) | 涂层 | 产品编码 |
| 12.70 | 12.70 | Uncoated | #39-519 |
| 12.70 | 20.00 | Uncoated | #39-522 |
| 12.70 | 25.40 | Uncoated | #39-524 |
| 12.70 | 35.00 | Uncoated | #39-525 |
| 12.70 | 50.80 | Uncoated | #39-528 |
| 25.40 | 25.40 | Uncoated | #39-530 |
| 25.40 | 35.00 | Uncoated | #39-531 |
| 25.40 | 50.80 | Uncoated | #39-532 |
| 25.40 | 75.00 | Uncoated | #39-533 |
| 25.40 | 100.00 | Uncoated | #39-534 |
| 25.40 | 150.00 | Uncoated | #39-535 |
| 25.40 | 250.00 | Uncoated | #39-536 |
| 50.80 | 50.80 | Uncoated | #39-537 |
| 50.80 | 75.00 | Uncoated | #39-538 |
| 50.80 | 100.00 | Uncoated | #39-539 |
| 50.80 | 150.00 | Uncoated | #39-540 |
| 50.80 | 200.00 | Uncoated | #39-541 |
| 12.70 | 12.70 | BBAR (8000-12000nm) | #39-542 |
| 12.70 | 20.00 | BBAR (8000-12000nm) | #39-543 |
| 12.70 | 25.40 | BBAR (8000-12000nm) | #39-544 |
| 12.70 | 35.00 | BBAR (8000-12000nm) | #39-545 |
| 12.70 | 50.80 | BBAR (8000-12000nm) | #39-546 |
| 25.40 | 25.40 | BBAR (8000-12000nm) | #39-547 |
| 25.40 | 35.00 | BBAR (8000-12000nm) | #39-548 |
| 25.40 | 50.80 | BBAR (8000-12000nm) | #39-549 |
| 25.40 | 75.00 | BBAR (8000-12000nm) | #39-550 |
| 25.40 | 100.00 | BBAR (8000-12000nm) | #39-551 |
| 25.40 | 150.00 | BBAR (8000-12000nm) | #39-552 |
| 25.40 | 250.00 | BBAR (8000-12000nm) | #39-553 |
| 50.80 | 50.80 | BBAR (8000-12000nm) | #11-408 |
| 50.80 | 75.00 | BBAR (8000-12000nm) | #11-409 |
| 50.80 | 100.00 | BBAR (8000-12000nm) | #11-410 |
| 50.80 | 150.00 | BBAR (8000-12000nm) | #11-411 |
| 50.80 | 200.00 | BBAR (8000-12000nm) | #11-412 |
| 12.70 | 12.70 | BBAR (3000-12000nm) | #11-418 |
| 12.70 | 20.00 | BBAR (3000-12000nm) | #11-419 |
| 12.70 | 25.40 | BBAR (3000-12000nm) | #11-420 |
| 12.70 | 35.00 | BBAR (3000-12000nm) | #11-421 |
| 12.70 | 50.80 | BBAR (3000-12000nm) | #11-422 |
| 25.40 | 25.40 | BBAR (3000-12000nm) | #11-423 |
| 25.40 | 35.00 | BBAR (3000-12000nm) | #11-424 |
| 25.40 | 50.80 | BBAR (3000-12000nm) | #11-425 |
| 25.40 | 75.00 | BBAR (3000-12000nm) | #11-426 |
| 25.40 | 100.00 | BBAR (3000-12000nm) | #11-427 |
| 25.40 | 150.00 | BBAR (3000-12000nm) | #11-428 |
| 25.40 | 250.00 | BBAR (3000-12000nm) | #11-429 |
| 50.80 | 50.80 | BBAR (3000-12000nm) | #11-430 |
| 50.80 | 75.00 | BBAR (3000-12000nm) | #11-431 |
| 50.80 | 100.00 | BBAR (3000-12000nm) | #11-432 |
| 50.80 | 150.00 | BBAR (3000-12000nm) | #11-433 |
| 50.80 | 200.00 | BBAR (3000-12000nm) | #11-434 |
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