消除球差
有多个镀膜选项可供选择
各种数值孔径可供选择
通用规格
焦距容差 (%): | ±1 |
表面质量: | 40-20 |
工作温度 (°C): | ≤200 |
产品介绍
LightPath® 模压非球面透镜能够消除球差和改善各种激光应用的聚焦和准直的准确度。低数值孔径的精密模造非球面透镜设计用于保持光束的形状,而高数值孔径的精密模造非球面透镜则可收集所有可用光源,以保持长距离下的光束功率。LightPath® 模压非球面透镜是一系列广泛应用的理想选择,包括瞄准系统、条形码扫描器、激光二极管到光纤耦合、光学数据存储或生物医学激光。
产品信息
NA | Dia. (mm) | EFL (mm) | 涂层 | 产品编码 |
0.13 | 6.33 | 22.00 | BBAR (350-700nm) | #83-543 |
0.13 | 6.33 | 22.00 | BBAR (600-1050nm) | #83-544 |
0.15 | 2.00 | 5.00 | BBAR (350-700nm) | #83-546 |
0.15 | 2.00 | 5.00 | BBAR (1050-1600nm) | #48-158 |
0.15 | 6.50 | 18.40 | BBAR (350-700nm) | #87-113 |
0.15 | 6.50 | 18.40 | BBAR (600-1050nm) | #87-114 |
0.15 | 6.50 | 18.40 | BBAR (1050-1600nm) | #87-115 |
0.16 | 6.50 | 15.29 | BBAR (350-700nm) | #37-098 |
0.16 | 6.50 | 15.29 | BBAR (600-1050nm) | #37-099 |
0.16 | 6.50 | 15.29 | BBAR (1050-1600nm) | #37-100 |
0.20 | 6.00 | 11.00 | BBAR (350-700nm) | #37-109 |
0.20 | 6.00 | 11.00 | BBAR (600-1050nm) | #37-110 |
0.20 | 6.00 | 11.00 | BBAR (1050-1600nm) | #37-111 |
0.26 | 4.70 | 2.76 | BBAR (350-700nm) | #87-133 |
0.26 | 4.70 | 2.76 | BBAR (600-1050nm) | #87-134 |
0.26 | 4.70 | 2.76 | BBAR (1050-1600nm) | #87-135 |
0.30 | 7.20 | 11.00 | BBAR (350-700nm) | #87-117 |
0.30 | 7.20 | 11.00 | BBAR (600-1050nm) | #87-118 |
0.30 | 7.20 | 11.00 | BBAR (1050-1600nm) | #87-119 |
0.30 | 6.51 | 7.50 | BBAR (350-700nm) | #87-129 |
0.30 | 6.51 | 7.50 | BBAR (600-1050nm) | #87-130 |
0.30 | 6.51 | 7.50 | BBAR (1050-1600nm) | #87-131 |
0.30 | 7.20 | 11.00 | BBAR (350-700nm) | #87-121 |
0.30 | 7.20 | 11.00 | BBAR (600-1050nm) | #87-122 |
0.30 | 7.20 | 11.00 | BBAR (1050-1600nm) | #87-123 |
0.32 | 3.00 | 2.51 | Uncoated | #83-573 |
0.40 | 7.20 | 6.24 | BBAR (350-700nm) | #87-125 |
0.40 | 7.20 | 6.24 | BBAR (600-1050nm) | #87-126 |
0.40 | 7.20 | 6.24 | BBAR (1050-1600nm) | #87-127 |
0.43 | 4.70 | 4.50 | BBAR (350-700nm) | #83-578 |
0.43 | 4.70 | 4.50 | BBAR (600-1050nm) | #83-579 |
0.43 | 4.70 | 4.50 | BBAR (1050-1600nm) | #83-580 |
0.50 | 1.00 | 0.55 | BBAR (350-700nm) | #37-112 |
0.50 | 1.00 | 0.55 | BBAR (600-1050nm) | #37-113 |
0.50 | 1.00 | 0.55 | BBAR (1050-1600nm) | #37-114 |
0.50 | 3.00 | 2.00 | BBAR (350-700nm) | #83-582 |
0.50 | 3.00 | 2.00 | BBAR (600-1050nm) | #83-583 |
0.50 | 6.33 | 6.70 | BBAR (350-700nm) | #37-101 |
0.50 | 9.94 | 8.00 | BBAR (350-700nm) | #37-102 |
0.50 | 9.94 | 8.00 | BBAR (600-1050nm) | #37-103 |
0.50 | 9.94 | 8.00 | BBAR (1050-1600nm) | #37-104 |
0.50 | 11.00 | 10.00 | BBAR (350-700nm) | #33-425 |
0.50 | 11.00 | 10.00 | BBAR (600-1050nm) | #33-426 |
0.50 | 11.00 | 10.00 | BBAR (1050-1600nm) | #33-427 |
0.55 | 4.00 | 2.73 | BBAR (350-700nm) | #83-605 |
0.55 | 4.00 | 2.73 | BBAR (600-1050nm) | #83-606 |
0.55 | 4.00 | 2.73 | BBAR (1050-1600nm) | #83-607 |
0.55 | 4.50 | 2.75 | BBAR (350-700nm) | #83-616 |
0.55 | 4.50 | 2.75 | BBAR (600-1050nm) | #66-926 |
0.55 | 4.50 | 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 | 6.00 | 4.60 | BBAR (350-700nm) | #87-157 |
0.55 | 6.00 | 4.60 | BBAR (600-1050nm) | #87-158 |
0.55 | 6.00 | 4.60 | BBAR (1050-1600nm) | #87-159 |
0.56 | 7.20 | 5.50 | BBAR (350-700nm) | #87-145 |
0.56 | 7.20 | 5.50 | BBAR (600-1050nm) | #87-146 |
0.56 | 7.20 | 5.50 | BBAR (1050-1600nm) | #87-147 |
0.58 |
|