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Design and laser damage properties of a dichroic beam combiner coating for 22.5° incidence and S polarization with high transmission at 527 nm and high reflection at 1054 nm

机译:设计和激光损伤二向色束组合物涂层的22.5°入射和S偏振,高速传递,在527nm处,高速反射在1054nm

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We have designed a dichroic beam combiner coating consisting of 11 HfO_2/SiO_2 layer pairs deposited on a large fused silica substrate. The coating provides high transmission (HT) at 527 nm and high reflection (HR) at 1054 nm for light at 22.5° angle of incidence (AOI) in air in S polarization (Spol). The coating's design is based on layers of near half-wave optical thickness in the design space for stable HT at 527 nm, with layer modifications that provide HR at 1054 nm while preserving HT at 527 nm. Its implementation in the 527 nm/1054 nm dual wavelength beam combiner arrangement has two options, with each option requiring one or the other of the high intensity beams to be incident on the dichroic coating from within the substrate (from glass). We show that there are differences between the two options with respect to the laser-induced damage threshold (LIDT) properties of the coating, and analyze the differences in terms of the 527 nm and 1054 nm E-field intensity behaviors for air → coating and glass → coating incidence. Our E-field analysis indicates that LIDTs for air → coating incidence should be higher than for glass → coating incidence. LIDT measurements for Spol at the use AOI with ns pulses at 532 nm and 1064 nm confirm this analysis with the LIDTs for glass → coating incidence being about half those for air → coating incidence at both wavelengths. These LIDT results and the E-field analysis clearly indicate that the best beam combiner option is the one for which the high intensity 527 nm beam is incident on the coating from air and the 1054 nm high intensity beam is incident on the coating from glass.
机译:我们设计了一种二向色束组合器涂层,其由11个HFO_2 / SiO_2层对沉积在大熔融二氧化硅基板上。涂层在S偏振(SPOL)中的22.5°入射角(AOI)的光,在527nm处以527nm和高反射(Hr)提供高透射(HT)。涂层的设计基于设计空间中的近半波光学厚度的层,用于527nm的稳定HT,具有1054nm的层改性,同时在527nm处保留HT。其在527nm / 1054nm双波长束组合器布置中的实现具有两种选择,每个选项需要一个或另一个的高强度光束入射在基板内(来自玻璃)的二向色涂层。我们表明,对于涂层的激光诱导的损伤阈值(LIDT)性质,两种选择之间存在差异,并分析了527nm和1054nm的空气→涂层和1054nm E场强度行为的差异玻璃→涂层发病率。我们的电子场分析表明,空气→涂层发病率的LIDTS应高于玻璃→涂层发病率。使用AOI在532nm和1064nm的使用AOI的液体测量结果用玻璃→涂层发射的盖子的盖子确认了该分析,其中涂层发射是空气→涂布率在两个波长下的一半。这些LIDT结果和E场分析清楚地表明,最佳光束组合器选项是高强度527nm光束入射在空气中的涂层上的选择,并且1054nm高强度束入射在玻璃涂层上。

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