隻折射聚合物加入到2塊玻璃基板的結構的波長板。
因相比水晶波長板價格低廉,適合偏光基礎實驗及對精度無要求的實驗。波長板的複折射因光波長不同,其位相差異會變動。
因此在使用波長以外的波長時,可能無法獲得波長板的效果。
波長板的表面與背面加工有使用波長下的反射防止膜。
請勿在高溫環境及高能量激光下使用。因為溫度變化可能導致位相差變化。
亦可提供因溫度變化導致位相差變化較小的S33系列。
款型 | 位相差(延遲) | 適應雷射 | 波長(nm) |
S333A-405-2 | λ/2 | LD | 405 |
S333A-488-2 | λ/2 | Ar | 488 |
S333A-532-2 | λ/2 | YAG | 532 |
S333A-633-2 | λ/2 | He-Ne | 633 |
S333A-650-2 | λ/2 | LD | 650 |
S333A-780-2 | λ/2 | LD | 780 |
S333A-830-2 | λ/2 | LD | 830 |
S333A-980-2 | λ/2 | LD | 980 |
S333A-1064-2 | λ/2 | YAG | 1064 |
S333A-1300-2 | λ/2 | LD | 1300 |
S333A-1550-2 | λ/2 | LD | 1550 |
S333-405-2 | λ/2 | LD | 405 |
S333-488-2 | λ/2 | Ar | 488 |
S333-532-2 | λ/2 | YAG | 532 |
S333-633-2 | λ/2 | He-Ne | 633 |
S333-650-2 | λ/2 | LD | 650 |
S333-780-2 | λ/2 | LD | 780 |
S333-830-2 | λ/2 | LD | 830 |
S333-980-2 | λ/2 | LD | 980 |
S333-1064-2 | λ/2 | YAG | 1064 |
S333-1300-2 | λ/2 | LD | 1300 |
S333-1550-2 | λ/2 | LD | 1550 |
S333A-405-4 | λ/4 | LD | 405 |
S333A-488-4 | λ/4 | Ar | 488 |
S333A-532-4 | λ/4 | YAG | 532 |
S333A-633-4 | λ/4 | He-Ne | 633 |
S333A-650-4 | λ/4 | LD | 650 |
S333A-780-4 | λ/4 | LD | 780 |
S333A-830-4 | λ/4 | LD | 830 |
S333A-980-4 | λ/4 | LD | 980 |
S333A-1064-4 | λ/4 | YAG | 1064 |
S333A-1300-4 | λ/4 | LD | 1300 |
S333A-1550-4 | λ/4 | LD | 1550 |
S333-405-4 | λ/4 | LD | 405 |
S333-488-4 | λ/4 | Ar | 488 |
S333-532-4 | λ/4 | YAG | 532 |
S333-633-4 | λ/4 | He-Ne | 633 |
S333-650-4 | λ/4 | LD | 650 |
S333-780-4 | λ/4 | LD | 780 |
S333-830-4 | λ/4 | LD | 830 |
S333-980-4 | λ/4 | LD | 980 |
S333-1064-4 | λ/4 | YAG | 1064 |
S333-1300-4 | λ/4 | LD | 1300 |
S333-1550-4 | λ/4 | LD | 1550 |
款型 | 位相差(延遲) | 適應雷射 | 波長(nm) | CAD |
S333A-405-2 | λ/2 | LD | 405 | - |
S333A-488-2 | λ/2 | Ar | 488 | - |
S333A-532-2 | λ/2 | YAG | 532 | - |
S333A-633-2 | λ/2 | He-Ne | 633 | - |
S333A-650-2 | λ/2 | LD | 650 | - |
S333A-780-2 | λ/2 | LD | 780 | - |
S333A-830-2 | λ/2 | LD | 830 | - |
S333A-980-2 | λ/2 | LD | 980 | - |
S333A-1064-2 | λ/2 | YAG | 1064 | - |
S333A-1300-2 | λ/2 | LD | 1300 | - |
S333A-1550-2 | λ/2 | LD | 1550 | - |
S333-405-2 | λ/2 | LD | 405 | - |
S333-488-2 | λ/2 | Ar | 488 | - |
S333-532-2 | λ/2 | YAG | 532 | - |
S333-633-2 | λ/2 | He-Ne | 633 | - |
S333-650-2 | λ/2 | LD | 650 | - |
S333-780-2 | λ/2 | LD | 780 | - |
S333-830-2 | λ/2 | LD | 830 | - |
S333-980-2 | λ/2 | LD | 980 | - |
S333-1064-2 | λ/2 | YAG | 1064 | - |
S333-1300-2 | λ/2 | LD | 1300 | - |
S333-1550-2 | λ/2 | LD | 1550 | - |
S333A-405-4 | λ/4 | LD | 405 | - |
S333A-488-4 | λ/4 | Ar | 488 | - |
S333A-532-4 | λ/4 | YAG | 532 | - |
S333A-633-4 | λ/4 | He-Ne | 633 | - |
S333A-650-4 | λ/4 | LD | 650 | - |
S333A-780-4 | λ/4 | LD | 780 | - |
S333A-830-4 | λ/4 | LD | 830 | - |
S333A-980-4 | λ/4 | LD | 980 | - |
S333A-1064-4 | λ/4 | YAG | 1064 | - |
S333A-1300-4 | λ/4 | LD | 1300 | - |
S333A-1550-4 | λ/4 | LD | 1550 | - |
S333-405-4 | λ/4 | LD | 405 | - |
S333-488-4 | λ/4 | Ar | 488 | - |
S333-532-4 | λ/4 | YAG | 532 | - |
S333-633-4 | λ/4 | He-Ne | 633 | - |
S333-650-4 | λ/4 | LD | 650 | - |
S333-780-4 | λ/4 | LD | 780 | - |
S333-830-4 | λ/4 | LD | 830 | - |
S333-980-4 | λ/4 | LD | 980 | - |
S333-1064-4 | λ/4 | YAG | 1064 | - |
S333-1300-4 | λ/4 | LD | 1300 | - |
S333-1550-4 | λ/4 | LD | 1550 | - |
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