首页> 外文会议>Annual laser damage symposium >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
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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:具有22.5°入射角和S偏振的二向色合束器涂层的设计和激光损伤特性,在527 nm处具有高透射率,在1054 nm处具有高反射率

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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合束器涂层,该涂层由沉积在大型熔融石英基体上的11对HfO_2 / SiO_2层对组成。对于在S偏振(Spol)下的空气中22.5°入射角(AOI)的光,该涂层在527 nm处提供高透射率(HT),在1054 nm处提供高反射率(HR)。涂层的设计基于设计空间中近半波光学厚度的层,以在527 nm处稳定HT,并进行了层修改,以在1054 nm处提供HR,同时保留527 nm处的HT。它在527 nm / 1054 nm双波长光束组合器装置中的实现有两个选择,每个选择都要求一个或另一个高强度光束从基板内部(从玻璃)入射到二向色涂层上。我们表明,在涂层的激光诱导损伤阈值(LIDT)特性方面,这两种选择之间存在差异,并分析了空气→涂层和527 nm和1054 nm电场强度行为的差异。玻璃→涂层的发生率。我们的电场分析表明,空气→涂层发生率的LIDTs应该高于玻璃→涂层发生率的LIDTs。在使用AOI的AOI上在532 nm和1064 nm的ns脉冲下对Spol的LIDT测量证实了这一分析,其中玻璃→涂层入射率的LIDT约为空气→涂层在两个波长入射率的一半。这些LIDT结果和电场分析清楚地表明,最佳的光束组合器选项是将527 nm高强度光束从空气入射到涂层上,并将1054 nm高强度光束从玻璃入射到涂层上。

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