薄膜偏振器可以分离266nm~1570nms偏振和p偏振分量,消光比Tp/Ts>200:1和Tp/Ts>1000:1。激光薄膜偏振片TFP有四种类型,分别是标准Rs/Tp:>99.5/95.0%、高透射率Rs/Tp:>99.5/99.0%、超高透射率Ts<0.2%Rp<0.2%和高消光比Tp>98%,Ts<0.1%四种。Eksma薄膜激光偏振器入射角度56°,所以又可以叫作56度薄膜偏振器和偏振分光镜,薄膜偏光片镜片形状有圆形和矩形。
所属品牌: 立陶宛EKSMA Optics
应用类型:
产品型号:420-1110E、420-1240E、420-1270、420-1370等
负责人:郭sy
联系电话:13434776712
电子邮箱:syguo@welloptics.cn
薄膜偏振器56°入射,266-1570nm,消光比Tp/Ts>200:1、>1000:1
BK7和UV FS薄膜激光偏振器(TFP)种类繁多,可快速交付。薄膜偏振器具有高激光损伤阈值,专为要求最苛刻的应用而设计,适用于Nd基激光器在1040-1070 nm范围内的运行,以及飞秒级Ti:Sapphire或Yb:KGW/KYW激光器。56度薄膜偏振器又可以叫作薄膜偏光片、偏振分光镜和薄膜偏振片TFP。
激光薄膜偏振片TFP分离特定波长或波长范围的s偏振和p偏振分量。由于激光薄膜偏振片TFP在1064nm处达到10J/cm2的高损伤阈值,10ns薄膜偏振器在高能激光器的应用中取代了Glan激光偏振棱镜或立方体偏振分束器。
薄膜偏光片用于高能激光器。激光薄膜偏振片TFP可用于Yb:KGW/KYW或Ti:Sapphire激光器的基波波长及其谐波,或是用作腔内Q开关保持偏振器。使用薄膜激光偏振器的最有效方法是在布儒斯特角-56°±2°,损耗最小。
我们提供四种类型的薄膜偏振器:
标准-Rs/Tp:>99.5/95.0%,消光比Tp/Ts>200:1
高透射率(HT)-Rs/Tp:>99.5/99.0%,消光比Tp/Ts>200:1
超高透射率(UHT)-Ts<0.2%,Rp<0.2%,消光比Tp/Ts>200:1
高消光比(HE)-Tp>98%,Ts<0.1%,消光比Tp/Ts>1000:1
薄膜激光偏振器的规格
|
56度薄膜偏振器基底材料 |
UV FS(紫外熔融石英) |
|
表面质量 |
20-10划痕/麻点(符合MIL-PRF-13830B标准) |
|
透射波前畸变 |
λ/10@633nm |
|
偏振分光镜平行度 |
<30弧秒(arcsec) |
|
56度薄膜偏振器通光孔径 |
圆形:>85%,矩形:56°入射角下椭圆通光区的>85% |
|
56度薄膜偏振器入射角 |
56° |
|
入射角公差 |
±2° |
|
直径公差 |
+0.0 / -0.12mm |
|
偏振分光镜厚度公差 |
±0.2mm |
|
激光损伤阈值 |
10J/cm²,1064nm下10ns脉冲,50Hz(典型值) |
|
消光比Tₚ/Tₛ |
标准/HT/UHT系列:>200:1 |
薄膜偏振器型号
|
型号 |
波长 |
基底 |
偏振性能 |
消光比 |
薄膜偏光片尺寸 |
|
420-1110E |
266nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
ø12.7×3 mm |
|
420-1240E |
266nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
ø25.4×3 mm |
|
420-1270 |
266nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
28.6×14.3×3 mm |
|
420-1370 |
266nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
35×20×3 mm |
|
420-1510E |
266nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
ø50.8×6 mm |
|
420-1242HE |
343nm |
UV FS |
Tp>98%,Ts<0.1% |
>1000:1 |
ø25.4×3 mm |
|
420-1242HT |
343nm |
UV FS |
Rs/Tp:>99.5/99.0% |
>200:1 |
ø25.4×3 mm |
|
420-1112E |
343nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
ø12.7×3 mm |
|
420-1242E |
343nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
ø25.4×3 mm |
|
420-1512E |
343nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
ø50.8×6 mm |
|
420-1272 |
343nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
28.6×14.3×3 mm |
|
420-1372 |
343nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
35×20×3 mm |
|
420-1122E |
355nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
ø12.7×3 mm |
|
420-1252HE |
355nm |
UV FS |
Tp>98%,Ts<0.1% |
>1000:1 |
ø25.4×3 mm |
|
420-1252HT |
355nm |
UV FS |
Rs/Tp:>99.5/99.0% |
>200:1 |
ø25.4×3 mm |
|
420-1252E |
355nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
ø25.4×3 mm |
|
420-1282 |
355nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
28.6×14.3×3 mm |
|
420-1382 |
355nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
35×20×3 mm |
|
420-1502E |
355nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
ø50.8×6 mm |
|
420-1253B |
390-410nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
ø25.4×3 mm |
|
420-1383B |
390-410nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
35×20×3 mm |
|
420-1503B |
390-410nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
ø50.8×6 mm |
|
420-1123E |
400nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
ø12.7×3 mm |
|
420-1253E |
400nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
ø25.4×3 mm |
|
420-1283 |
400nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
28.6×14.3×3 mm |
|
420-1383 |
400nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
35×20×3 mm |
|
420-1503E |
400nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
ø50.8×6 mm |
|
420-1114E |
515nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
ø12.7×3 mm |
|
420-1244HE |
515nm |
UV FS |
Tp>98%,Ts<0.1% |
>1000:1 |
ø25.4×3 mm |
|
420-1244HT |
515nm |
UV FS |
Rs/Tp:>99.5/99.0% |
>200:1 |
ø25.4×3 mm |
|
420-1244E |
515nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
ø25.4×3 mm |
|
420-1274 |
515nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
28.6×14.3×3 mm |
|
420-1374 |
515nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
35×20×3 mm |
|
420-1514E |
515nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
ø50.8×6 mm |
|
420-1124E |
532nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
ø12.7×3 mm |
|
420-1484HE |
532nm |
UV FS |
Tp>98%,Ts<0.1% |
>1000:1 |
20×15×6 mm |
|
420-1254HE |
532nm |
UV FS |
Tp>98%,Ts<0.1% |
>1000:1 |
ø25.4×3 mm |
|
420-1254UHT |
532nm |
UV FS |
Ts<0.2%,Rp<0.2% |
>500:1 |
ø25.4×3 mm |
|
420-1254HT |
532nm |
UV FS |
Rs/Tp:>99.5/99.0% |
>200:1 |
ø25.4×3 mm |
|
420-1254E |
532nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
ø25.4×3 mm |
|
420-1284 |
532nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
28.6×14.3×3 mm |
|
420-1584HE |
532nm |
UV FS |
Tp>98%,Ts<0.1% |
>1000:1 |
30×20×6 mm |
|
420-1384 |
532nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
35×20×3 mm |
|
420-1504E |
532nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
ø50.8×6 mm |
|
420-0285 |
633nm |
BK7 |
Rs/Tp:>99.5/95.0% |
>200:1 |
28.6×14.3×3 mm |
|
420-1136E |
780-820nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
ø12.7×3 mm |
|
420-1266E |
780-820nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
ø25.4×3 mm |
|
420-1296 |
780-820nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
28.6×14.3×3 mm |
|
420-1396 |
780-820nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
35×20×3 mm |
|
420-1526E |
780-820nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
ø50.8×6 mm |
|
420-1126E |
800nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
ø12.7×3 mm |
|
420-1256E |
800nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
ø25.4×3 mm |
|
420-1256HE |
800nm |
UV FS |
Tp>98%,Ts<0.1% |
>1000:1 |
ø25.4×3 mm |
|
420-1256UHT |
800nm |
UV FS |
Ts<0.2%,Rp<0.2% |
>500:1 |
ø25.4×3 mm |
|
420-1256HT |
800nm |
UV FS |
Rs/Tp:>99.5/99.0% |
>200:1 |
ø25.4×3 mm |
|
420-0286 |
800nm |
BK7 |
Rs/Tp:>99.5/95.0% |
>200:1 |
28.6×14.3×3 mm |
|
420-1286 |
800nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
28.6×14.3×3 mm |
|
420-1386 |
800nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
35×20×3 mm |
|
420-1506E |
800nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
ø50.8×6 mm |
|
420-1138E |
1010-1050nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
ø12.7×3 mm |
|
420-1268E |
1010-1050nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
ø25.4×3 mm |
|
420-1298 |
1010-1050nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
28.6×14.3×3 mm |
|
420-1398 |
1010-1050nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
35×20×3 mm |
|
420-1528E |
1010-1050nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
ø50.8×6 mm |
|
420-0118E |
1030nm |
BK7 |
Rs/Tp:>99.5/95.0% |
>200:1 |
ø12.7×3 mm |
|
420-1118E |
1030nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
ø12.7×3 mm |
|
420-1478HE |
1030nm |
UV FS |
Tp>98%,Ts<0.1% |
>1000:1 |
20×15×6 mm |
|
420-1248HE |
1030nm |
UV FS |
Tp>98%,Ts<0.1% |
>1000:1 |
ø25.4×3 mm |
|
420-1248UHT |
1030nm |
UV FS |
Ts<0.2%,Rp<0.2% |
>500:1 |
ø25.4×3 mm |
|
420-1248HT |
1030nm |
UV FS |
Rs/Tp:>99.5/99.0% |
>200:1 |
ø25.4×3 mm |
|
420-1248E |
1030nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
ø25.4×3 mm |
|
420-1278 |
1030nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
28.6×14.3×3 mm |
|
420-1278HT |
1030nm |
UV FS |
Rs/Tp:>99.5/99.0% |
>200:1 |
28.6×14.3×3 mm |
|
420-1578HE |
1030nm |
UV FS |
Tp>98%,Ts<0.1% |
>1000:1 |
30×20×6 mm |
|
420-1378 |
1030nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
35×20×3 mm |
|
420-1518E |
1030nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
ø50.8×6 mm |
|
420-1128E |
1064nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
ø12.7×3 mm |
|
420-1488HE |
1064nm |
UV FS |
Tp>98%,Ts<0.1% |
>1000:1 |
20×15×6 mm |
|
420-1258HE |
1064nm |
UV FS |
Tp>98%,Ts<0.1% |
>1000:1 |
ø25.4×3 mm |
|
420-1258UHT |
1064nm |
UV FS |
Ts<0.2%,Rp<0.2% |
>500:1 |
ø25.4×3 mm |
|
420-1258HT |
1064nm |
UV FS |
Rs/Tp:>99.5/99.0% |
>200:1 |
ø25.4×3 mm |
|
420-1258E |
1064nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
ø25.4×3 mm |
|
420-1288HT |
1064nm |
UV FS |
Rs/Tp:>99.5/99.0% |
>200:1 |
28.6×14.3×3 mm |
|
420-1288 |
1064nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
28.6×14.3×3 mm |
|
420-1588HE |
1064nm |
UV FS |
Tp>98%,Ts<0.1% |
>1000:1 |
30×20×6 mm |
|
420-1388 |
1064nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
35×20×3 mm |
|
420-1508E |
1064nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
ø50.8×6 mm |
|
420-0259E |
1550nm |
BK7 |
Rs/Tp:>99.5/95.0% |
>200:1 |
ø25.4×3 mm |
|
420-1269E |
1530-1570nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
ø25.4×3 mm |
|
420-1399 |
1530-1570nm |
UV FS |
Rs/Tp:>99.5/95.0% |
>200:1 |
35×20×3 mm |