1）消除球差 2）有多個(gè)鍍膜選項(xiàng)可供選擇 3）各種數(shù)值孔徑可供選擇 精密模造的非球面透鏡能夠消除球差和改善各種激光應(yīng)用的聚焦和準(zhǔn)直的準(zhǔn)確度。低數(shù)值孔徑的精密模造非球面透鏡設(shè)計(jì)用于保持光束的形狀，而高數(shù)值孔徑的精密模造非球面透鏡則可收集所有可用光源，以保持長距離下的光束功率。精密模造的非球面透鏡是一系列廣泛應(yīng)用的理想選擇，包括瞄準(zhǔn)系統(tǒng)、條形碼掃描器、激光二極管到光纖耦合、光學(xué)數(shù)據(jù)存儲或生物醫(yī)學(xué)激光。 高精度壓鑄的非球面透鏡 Common Specifications 傳輸波前，P-V (λ): | Diffraction Limit | 表面質(zhì)量: | 40-20 | 工作溫度 (°C): | ≤200 |
訂購信息：
數(shù)字孔徑 NA | 直徑 (mm) | 有效焦距 EFL (mm) | 涂層 | 產(chǎn)品號 | 0.13 | 6.33 | 22 | BBAR (350-700nm) | #83-543 | 0.13 | 6.33 | 22 | BBAR (600-1050nm) | #83-544 | 0.15 | 2 | 5 | BBAR (350-700nm) | #83-546 | 0.15 | 2 | 5 | BBAR (1050-1600nm) | #48-158 | 0.15 | 6.5 | 18.4 | BBAR (350-700nm) | #87-113 | 0.15 | 6.5 | 18.4 | BBAR (600-1050nm) | #87-114 | 0.15 | 6.5 | 18.4 | BBAR (1050-1600nm) | #87-115 | 0.16 | 6.5 | 15.29 | BBAR (350-700nm) | #37-098 | 0.16 | 6.5 | 15.29 | BBAR (600-1050nm) | #37-099 | 0.16 | 6.5 | 15.29 | BBAR (1050-1600nm) | #37-100 | 0.2 | 6 | 11 | BBAR (350-700nm) | #37-109 | 0.2 | 6 | 11 | BBAR (600-1050nm) | #37-110 | 0.2 | 6 | 11 | BBAR (1050-1600nm) | #37-111 | 0.25 | 7.2 | 11 | BBAR (350-700nm) | #87-117 | 0.25 | 7.2 | 11 | BBAR (600-1050nm) | #87-118 | 0.25 | 7.2 | 11 | BBAR (1050-1600nm) | #87-119 | 0.3 | 6.51 | 7.5 | BBAR (350-700nm) | #87-129 | 0.3 | 6.51 | 7.5 | BBAR (600-1050nm) | #87-130 | 0.3 | 6.51 | 7.5 | BBAR (1050-1600nm) | #87-131 | 0.3 | 7.2 | 11 | BBAR (350-700nm) | #87-121 | 0.3 | 7.2 | 11 | BBAR (600-1050nm) | #87-122 | 0.3 | 7.2 | 11 | BBAR (1050-1600nm) | #87-123 | 0.4 | 7.2 | 6.24 | BBAR (350-700nm) | #87-125 | 0.4 | 7.2 | 6.24 | BBAR (600-1050nm) | #87-126 | 0.4 | 7.2 | 6.24 | BBAR (1050-1600nm) | #87-127 | 0.43 | 4.7 | 4.5 | BBAR (350-700nm) | #83-578 | 0.43 | 4.7 | 4.5 | BBAR (600-1050nm) | #83-579 | 0.43 | 4.7 | 4.5 | BBAR (1050-1600nm) | #83-580 | 0.5 | 1 | 0.55 | BBAR (350-700nm) | #37-112 | 0.5 | 1 | 0.55 | BBAR (600-1050nm) | #37-113 | 0.5 | 1 | 0.55 | BBAR (1050-1600nm) | #37-114 | 0.5 | 3 | 2 | BBAR (350-700nm) | #83-582 | 0.5 | 3 | 2 | BBAR (600-1050nm) | #83-583 | 0.5 | 6.33 | 6.7 | BBAR (350-700nm) | #37-101 | 0.5 | 9.94 | 8 | BBAR (350-700nm) | #37-102 | 0.5 | 9.94 | 8 | BBAR (600-1050nm) | #37-103 | 0.5 | 9.94 | 8 | BBAR (1050-1600nm) | #37-104 | 0.5 | 11 | 10 | BBAR (350-700nm) | #33-425 | 0.5 | 11 | 10 | BBAR (600-1050nm) | #33-426 | 0.5 | 11 | 10 | BBAR (1050-1600nm) | #33-427 | 0.52 | 4.7 | 2.76 | BBAR (350-700nm) | #87-133 | 0.52 | 4.7 | 2.76 | BBAR (600-1050nm) | #87-134 | 0.52 | 4.7 | 2.76 | BBAR (1050-1600nm) | #87-135 | 0.55 | 4 | 2.73 | BBAR (350-700nm) | #83-605 | 0.55 | 4 | 2.73 | BBAR (600-1050nm) | #83-606 | 0.55 | 4 | 2.73 | BBAR (1050-1600nm) | #83-607 | 0.55 | 4.5 | 2.75 | BBAR (350-700nm) | #83-616 | 0.55 | 4.5 | 2.75 | BBAR (600-1050nm) | #66-926 | 0.55 | 4.5 | 2.75 | BBAR (1050-1600nm) | #66-927 | 0.55 | 6.33 | 4.51 | BBAR (350-700nm) | #87-153 | 0.55 | 6.33 | 4.51 | BBAR (600-1050nm) | #87-154 | 0.55 | 6.33 | 4.51 | BBAR (1050-1600nm) | #87-155 | 0.55 | 6 | 4.6 | BBAR (350-700nm) | #87-157 | 0.55 | 6 | 4.6 | BBAR (600-1050nm) | #87-158 | 0.55 | 6 | 4.6 | BBAR (1050-1600nm) | #87-159 | 0.56 | 7.2 | 5.5 | BBAR (350-700nm) | #87-145 | 0.56 | 7.2 | 5.5 | BBAR (600-1050nm) | #87-146 | 0.56 | 7.2 | 5.5 | BBAR (1050-1600nm) | #87-147 | 0.58 | 2.4 | 1.45 | BBAR (350-700nm) | #83-613 | 0.58 | 2.4 | 1.45 | BBAR (600-1050nm) | #83-614 | 0.58 | 2.4 | 1.45 | BBAR (1050-1600nm) | #83-615 | 0.6 | 15 | 10 | BBAR (350-700nm) | #37-105 | 0.6 | 15 | 10 | BBAR (600-1050nm) | #37-106 | 0.6 | 15 | 10 | BBAR (1050-1600nm) | #37-107 | 0.64 | 4 | 2.75 | BBAR (350-700nm) | #83-626 | 0.64 | 4 | 2.75 | BBAR (600-1050nm) | #83-627 | 0.64 | 4 | 2.75 | BBAR (1050-1600nm) | #83-628 | 0.64 | 6.33 | 4.03 | BBAR (350-700nm) | #87-161 | 0.64 | 6.33 | 4.03 | BBAR (600-1050nm) | #87-162 | 0.64 | 6.33 | 4.03 | BBAR (1050-1600nm) | #87-163 | 0.68 | 6.33 | 3.1 | BBAR (350-700nm) | #87-165 | 0.68 | 6.33 | 3.1 | BBAR (600-1050nm) | #87-166 | 0.68 | 6.33 | 3.1 | BBAR (1050-1600nm) | #87-167 | 0.77 | 6.33 | 3.1 | BBAR (600-1050nm) | #83-674 |
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