目錄:江陰韻翔光電技術有限公司>>光學元件>>窗口片>> 鍺窗口片
| 價格區間 | 面議 | 應用領域 | 醫療衛生,環保,化工,電子 |
|---|---|---|---|
| 組件類別 | 光學元件 |
鍺窗口片
?可選未鍍膜版和鍍增透膜版，適用于各種紅外應用
?低色散使色像差相對變得極低
?非常適合用于需要堅固光學窗口片的紅外應用
TECHSPEC® 鍺 (Ge) 窗口片有現貨，可選三種增透膜: 3 - 5μm波段的增透膜適用于中紅外應用，3 - 12μm波段的增透膜適用于寬帶多光譜應用, 8 - 12μm波段的增透膜適用于熱成像應用。鍺光學材料也比較適合做設計波長在8-12μm內的增透膜（AR）鍍膜的膜層材料。鍺受溫度影響嚴重，透過率隨溫度的升高而降低，因此，它們只能在100®C以下應用。在設計對重量有嚴格要求的系統的時候要考慮鍺的密度(5.33 g/cm3)。鍺主要應用在熱成像系統和前視紅外（FLIR）領域里面。鍺的努氏硬度是780，大概是氟化鎂硬度的兩倍，這使它比較適合變化光學的IR領域的應用。
鍺窗口片
Common Specifications
表面平整度: | λ/10 @ 10.6μm |
有效孔徑 (%): | 90 |
平行度（弧分）: | <1 |
表面質量: | 60-40 |
基底: | Germanium (Ge) |
訂購信息：
| Dia. (mm) | 厚度 (mm) | 涂層 | 產品編碼 |
| 5.00 | 1.00 | Uncoated | #20-167 |
| 10.00 | 1.50 | Uncoated | #68-734 |
| 10.00 | 1.50 | BBAR (3000-5000nm) | #89-558 |
| 10.00 | 1.50 | BBAR (3000-12000nm) | #62-643 |
| 10.00 | 1.50 | BBAR (8000-12000nm) | #47-685 |
| 12.50 | 1.00 | Uncoated | #83-341 |
| 12.50 | 1.00 | BBAR (3000-5000nm) | #89-559 |
| 12.50 | 1.00 | BBAR (3000-12000nm) | #83-347 |
| 12.50 | 1.00 | BBAR (8000-12000nm) | #83-353 |
| 12.50 | 2.00 | Uncoated | #68-735 |
| 12.50 | 2.00 | BBAR (3000-5000nm) | #89-560 |
| 12.50 | 2.00 | BBAR (3000-12000nm) | #62-644 |
| 12.50 | 2.00 | BBAR (8000-12000nm) | #47-686 |
| 12.50 | 3.00 | Uncoated | #83-342 |
| 12.50 | 3.00 | BBAR (3000-5000nm) | #89-561 |
| 12.50 | 3.00 | BBAR (3000-12000nm) | #83-348 |
| 12.50 | 3.00 | BBAR (8000-12000nm) | #83-354 |
| 20.00 | 2.00 | Uncoated | #68-736 |
| 20.00 | 2.00 | BBAR (3000-5000nm) | #89-562 |
| 20.00 | 2.00 | BBAR (3000-12000nm) | #64-377 |
| 20.00 | 2.00 | BBAR (8000-12000nm) | #63-213 |
| 25.00 | 1.00 | Uncoated | #83-343 |
| 25.00 | 1.00 | BBAR (3000-5000nm) | #89-563 |
| 25.00 | 1.00 | BBAR (3000-12000nm) | #83-349 |
| 25.00 | 1.00 | BBAR (8000-12000nm) | #83-355 |
| 25.00 | 2.00 | Uncoated | #83-344 |
| 25.00 | 2.00 | BBAR (3000-5000nm) | #89-564 |
| 25.00 | 2.00 | BBAR (3000-12000nm) | #83-350 |
| 25.00 | 2.00 | BBAR (8000-12000nm) | #83-356 |
| 25.00 | 3.00 | Uncoated | #68-737 |
| 25.00 | 3.00 | BBAR (3000-5000nm) | #89-565 |
| 25.00 | 3.00 | BBAR (3000-12000nm) | #62-645 |
| 25.00 | 3.00 | BBAR (8000-12000nm) | #47-687 |
| 25.40 | 3.00 | Uncoated | #11-862 |
| 25.40 | 3.00 | BBAR (3000-5000nm) | #11-865 |
| 25.40 | 3.00 | BBAR (3000-12000nm) | #11-868 |
| 25.40 | 3.00 | BBAR (8000-12000nm) | #11-871 |
| 30.00 | 3.00 | Uncoated | #68-738 |
| 30.00 | 3.00 | BBAR (3000-5000nm) | #89-566 |
| 30.00 | 3.00 | BBAR (3000-12000nm) | #64-378 |
| 30.00 | 3.00 | BBAR (8000-12000nm) | #63-214 |
| 40.00 | 4.00 | Uncoated | #68-739 |
| 40.00 | 4.00 | BBAR (3000-5000nm) | #89-567 |
| 40.00 | 4.00 | BBAR (3000-12000nm) | #64-379 |
| 40.00 | 4.00 | BBAR (8000-12000nm) | #63-215 |
| 50.00 | 1.00 | Uncoated | #83-345 |
| 50.00 | 1.00 | BBAR (3000-5000nm) | #89-568 |
| 50.00 | 1.00 | BBAR (3000-12000nm) | #83-351 |
| 50.00 | 1.00 | BBAR (8000-12000nm) | #83-357 |
| 50.00 | 2.00 | Uncoated | #83-346 |
| 50.00 | 2.00 | BBAR (3000-5000nm) | #89-569 |
| 50.00 | 2.00 | BBAR (3000-12000nm) | #83-352 |
| 50.00 | 2.00 | BBAR (8000-12000nm) | #83-358 |
| 50.00 | 3.00 | Uncoated | #68-740 |
| 50.00 | 3.00 | BBAR (3000-5000nm) | #89-570 |
| 50.00 | 3.00 | BBAR (3000-12000nm) | #62-646 |
| 50.00 | 3.00 | BBAR (8000-12000nm) | #47-688 |
| 50.80 | 3.00 | Uncoated | #11-863 |
| 50.80 | 3.00 | BBAR (3000-5000nm) | #11-866 |
| 50.80 | 3.00 | BBAR (3000-12000nm) | #11-869 |
| 50.80 | 3.00 | BBAR (8000-12000nm) | #11-872 |
| 75.00 | 5.00 | Uncoated | #68-741 |
| 75.00 | 5.00 | BBAR (3000-5000nm) | #89-571 |
| 75.00 | 5.00 | BBAR (3000-12000nm) | #64-380 |
| 75.00 | 5.00 | BBAR (8000-12000nm) | #48-857 |
| 76.20 | 5.00 | Uncoated | #11-864 |
| 76.20 | 5.00 | BBAR (3000-5000nm) | #11-867 |
| 76.20 | 5.00 | BBAR (3000-12000nm) | #11-870 |
| 76.20 | 5.00 | BBAR (8000-12000nm) | #11-873 |
| 100.00 | 6.00 | Uncoated | #17-669 |
| 100.00 | 6.00 | BBAR (8000-12000nm) | #17-678 |
| 125.00 | 6.00 | Uncoated | #17-670 |
| 150.00 | 8.00 | Uncoated | #17-671 |
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