目錄:江陰韻翔光電技術(shù)有限公司>>光學(xué)元件>>透鏡>> 精密非球面透鏡
| 參考價(jià) | 面議 |
| 參考價(jià) | 面議 |
更新時(shí)間：2023-12-16 14:44:37瀏覽次數(shù)：3119評(píng)價(jià)
聯(lián)系我們時(shí)請(qǐng)說(shuō)明是化工儀器網(wǎng)上看到的信息，謝謝!
| 價(jià)格區(qū)間 | 面議 | 應(yīng)用領(lǐng)域 | 醫(yī)療衛(wèi)生,環(huán)保,電子 |
|---|---|---|---|
| 組件類別 | 光學(xué)元件 |
由愛特蒙特光學(xué)設(shè)計(jì)及制造
減少球面像差
備有寬帶AR鍍膜供選擇
精密非球面透鏡通用規(guī)格
| 焦距波長(zhǎng) (nm): | 587.6 |
| 中心厚度容差 (mm): | ±0.1 |
| 有效孔徑 (%): | 90 |
| 非球面圖形誤差 (µm RMS): | 0.75 |
| 表面質(zhì)量: | 60-40 |
| 中心偏（弧分）: | ≤5 |
產(chǎn)品介紹
TECHSPEC®精密非球面透鏡設(shè)計(jì)用于聚焦光線，同時(shí)消除高度擴(kuò)散光源應(yīng)用中的球面像差，其中的應(yīng)用之一包括聚焦來(lái)自激光二極管的輸出。非球面透鏡能提高透鏡的數(shù)值孔徑，同時(shí)限度地減少系統(tǒng)像差。非球面透鏡也能減少多元件光學(xué)系統(tǒng)所需的元件數(shù)量。非球面透鏡可以降低系統(tǒng)總重量，同時(shí)提供諸多優(yōu)勢(shì)，如簡(jiǎn)化裝配及提高光通量。
TECHSPEC®精密非球面透鏡備有低f#，以帶來(lái).佳光線收集性能。
我們提供完整的設(shè)計(jì)數(shù)據(jù)，能輕易將這些非球面透鏡整合到光學(xué)系統(tǒng)中。
這些透鏡均經(jīng)過計(jì)算機(jī)優(yōu)化以消除球差，同時(shí)限度地減少較別的像差。
VIS鍍膜選項(xiàng)能為波長(zhǎng)介于425 – 675nm的光線提供小于1.5%的反射度。
NIR鍍膜選項(xiàng)則能為波長(zhǎng)介于600 – 1050nm的光線提供小于1.5%的反射度。
有關(guān)定制非球面透鏡以及批量定價(jià)的詳細(xì)信息，請(qǐng)聯(lián)系我們的銷售部門。
產(chǎn)品信息
| Dia. (mm) | EFL (mm) | NA | CT (mm) | 涂層 | 產(chǎn)品編碼 |
| 10.00 | 7.50 | 0.67 | 5.00 | Uncoated | #69-852 |
| 10.00 | 7.50 | 0.67 | 5.00 | BBAR (425-675nm) | #69-856 |
| 10.00 | 7.50 | 0.67 | 5.00 | BBAR (600-1050nm) | #69-860 |
| 10.00 | 10.00 | 0.50 | 4.00 | Uncoated | #69-853 |
| 10.00 | 10.00 | 0.50 | 4.00 | BBAR (425-675nm) | #69-857 |
| 10.00 | 10.00 | 0.50 | 4.00 | BBAR (600-1050nm) | #69-861 |
| 12.50 | 9.50 | 0.66 | 5.00 | Uncoated | #69-854 |
| 12.50 | 9.50 | 0.66 | 5.00 | BBAR (425-675nm) | #69-858 |
| 12.50 | 9.50 | 0.66 | 5.00 | BBAR (600-1050nm) | #69-862 |
| 12.50 | 12.50 | 0.50 | 5.00 | Uncoated | #69-855 |
| 12.50 | 12.50 | 0.50 | 5.00 | BBAR (425-675nm) | #69-859 |
| 12.50 | 12.50 | 0.50 | 5.00 | BBAR (600-1050nm) | #69-863 |
| 15.00 | 9.00 | 0.83 | 7.00 | Uncoated | #67-243 |
| 15.00 | 9.00 | 0.83 | 7.00 | BBAR (425-675nm) | #67-250 |
| 15.00 | 9.00 | 0.83 | 7.00 | BBAR (600-1050nm) | #67-257 |
| 15.00 | 11.25 | 0.66 | 7.00 | Uncoated | #47-725 |
| 15.00 | 11.25 | 0.66 | 7.00 | BBAR (425-675nm) | #49-097 |
| 15.00 | 11.25 | 0.66 | 7.00 | BBAR (600-1050nm) | #49-109 |
| 15.00 | 15.00 | 0.50 | 5.50 | Uncoated | #47-726 |
| 15.00 | 15.00 | 0.50 | 5.50 | BBAR (425-675nm) | #49-098 |
| 15.00 | 15.00 | 0.50 | 5.50 | BBAR (600-1050nm) | #49-110 |
| 15.00 | 18.75 | 0.40 | 4.50 | Uncoated | #47-727 |
| 15.00 | 18.75 | 0.40 | 4.50 | BBAR (425-675nm) | #49-099 |
| 15.00 | 18.75 | 0.40 | 4.50 | BBAR (600-1050nm) | #49-111 |
| 15.00 | 22.50 | 0.33 | 4.00 | Uncoated | #47-728 |
| 15.00 | 22.50 | 0.33 | 4.00 | BBAR (425-675nm) | #49-100 |
| 15.00 | 22.50 | 0.33 | 4.00 | BBAR (600-1050nm) | #49-112 |
| 20.00 | 12.50 | 0.80 | 9.00 | Uncoated | #67-244 |
| 20.00 | 12.50 | 0.80 | 9.00 | BBAR (425-675nm) | #67-251 |
| 20.00 | 12.50 | 0.80 | 9.00 | BBAR (600-1050nm) | #67-258 |
| 20.00 | 15.00 | 0.66 | 9.60 | Uncoated | #66-309 |
| 20.00 | 15.00 | 0.66 | 9.60 | BBAR (425-675nm) | #66-319 |
| 20.00 | 15.00 | 0.66 | 9.60 | BBAR (600-1050nm) | #66-329 |
| 20.00 | 20.00 | 0.50 | 8.00 | Uncoated | #66-310 |
| 20.00 | 20.00 | 0.50 | 8.00 | BBAR (425-675nm) | #66-320 |
| 20.00 | 20.00 | 0.50 | 8.00 | BBAR (600-1050nm) | #66-330 |
| 25.00 | 15.00 | 0.83 | 11.00 | Uncoated | #67-245 |
| 25.00 | 15.00 | 0.83 | 11.00 | BBAR (425-675nm) | #67-252 |
| 25.00 | 15.00 | 0.83 | 11.00 | BBAR (600-1050nm) | #67-259 |
| 25.00 | 18.75 | 0.66 | 10.00 | Uncoated | #47-729 |
| 25.00 | 18.75 | 0.66 | 10.00 | BBAR (425-675nm) | #49-101 |
| 25.00 | 18.75 | 0.66 | 10.00 | BBAR (600-1050nm) | #49-113 |
| 25.00 | 25.00 | 0.50 | 7.50 | Uncoated | #47-730 |
| 25.00 | 25.00 | 0.50 | 7.50 | BBAR (425-675nm) | #49-102 |
| 25.00 | 25.00 | 0.50 | 7.50 | BBAR (600-1050nm) | #49-114 |
| 25.00 | 31.25 | 0.40 | 6.50 | Uncoated | #47-731 |
| 25.00 | 31.25 | 0.40 | 6.50 | BBAR (425-675nm) | #49-103 |
| 25.00 | 31.25 | 0.40 | 6.50 | BBAR (600-1050nm) | #49-115 |
| 25.00 | 37.50 | 0.33 | 6.00 | Uncoated | #47-732 |
| 25.00 | 37.50 | 0.33 | 6.00 | BBAR (425-675nm) | #49-104 |
| 25.00 | 37.50 | 0.33 | 6.00 | BBAR (600-1050nm) | #49-116 |
| 25.00 | 50.00 | 0.25 | 5.50 | Uncoated | #33-944 |
| 25.00 | 50.00 | 0.25 | 5.50 | BBAR (425-675nm) | #33-945 |
| 25.00 | 50.00 | 0.25 | 5.50 | BBAR (600-1050nm) | #33-946 |
| 30.00 | 17.50 | 0.86 | 13.50 | Uncoated | #67-246 |
| 30.00 | 17.50 | 0.86 | 13.50 | BBAR (425-675nm) | #67-253 |
| 30.00 | 17.50 | 0.86 | 13.50 | BBAR (600-1050nm) | #67-260 |
| 30.00 | 22.50 | 0.66 | 14.40 | Uncoated | #66-311 |
| 30.00 | 22.50 | 0.66 | 14.40 | BBAR (425-675nm) | #66-321 |
| 30.00 | 22.50 | 0.66 | 14.40 | BBAR (600-1050nm) | #66-331 |
| 30.00 | 30.00 | 0.50 | 11.70 | Uncoated | #66-312 |
| 30.00 | 30.00 | 0.50 | 11.70 | BBAR (425-675nm) | #66-322 |
| 30.00 | 30.00 | 0.50 | 11.70 | BBAR (600-1050nm) | #66-332 |
| 40.00 | 25.00 | 0.80 | 15.50 | Uncoated | #67-247 |
| 40.00 | 25.00 | 0.80 | 15.50 | BBAR (425-675nm) | #67-254 |
| 40.00 | 25.00 | 0.80 | 15.50 | BBAR (600-1050nm) | #67-261 |
| 40.00 | 30.00 | 0.66 | 15.50 | Uncoated | #66-313 |
| 40.00 | 30.00 | 0.66 | 15.50 | BBAR (425-675nm) | #66-323 |
| 40.00 | 30.00 | 0.66 | 15.50 | BBAR (600-1050nm) | #66-333 |
| 40.00 | 40.00 | 0.50 | 15.50 | Uncoated | #66-314 |
| 40.00 | 40.00 | 0.50 | 15.50 | BBAR (425-675nm) | #66-324 |
| 40.00 | 40.00 | 0.50 | 15.50 | BBAR (600-1050nm) | #66-334 |
| 50.00 | 30.00 | 0.83 | 20.00 | Uncoated | #67-248 |
| 50.00 | 30.00 | 0.83 | 20.00 | BBAR (425-675nm) | #67-255 |
| 50.00 | 30.00 | 0.83 | 20.00 | BBAR (600-1050nm) | #67-262 |
| 50.00 | 37.50 | 0.66 | 19.40 | Uncoated | #66-315 |
| 50.00 | 37.50 | 0.66 | 19.40 | BBAR (425-675nm) | #66-325 |
| 50.00 | 37.50 | 0.66 | 19.40 | BBAR (600-1050nm) | #66-335 |
| 50.00 | 50.00 | 0.50 | 19.40 | Uncoated | #66-316 |
| 50.00 | 50.00 | 0.50 | 19.40 | BBAR (425-675nm) | #66-326 |
| 50.00 | 50.00 | 0.50 | 19.40 | BBAR (600-1050nm) | #66-336 |
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