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The Nonlinear Coefficient d_(36) of CdSiP_2

机译:CdSiP_2的非线性系数d_(36)

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The new nonlinear crystal for the mid-IR CdSiP_2 was discovered only very recently but the interest in this chalcopyrite is enormous because it possesses most of the attractive properties of the related ZnGeP_2 but allows in addition pumping at 1064 nm without two-photon absorption and uncritical phase-matching for 6 μm generation with maximized effective nonlinearity. The last feature is due to the fact that this crystal is negative uniaxial in contrast to ZnGeP_2 which shows positive birefringence. We now measured its nonlinear coefficient using SHG of femtosecond pulses generated near 4.6 μm from a seeded KNbO_3 optical parametric amplifier. The SHG efficiency was compared for uncoated samples of CdSiP_2 and ZnGeP_2, both ≈0.5 mm thick, in the low conversion limit (<10% internal conversion efficiency) which justifies the use of the plane wave approximation. Taking into account the experimentally determined phase-matching angles for type-Ⅰ SHG (oo-e type in CdSiP_2 and ee-o type in ZnGeP_2), which were in good agreement with the existing Sellmeier approximations, we arrived at d_(36)(CdSiP_2)~d_(36)(ZnGeP_2) which is rather unexpected having in mind the larger band-gap of CdSiP_2. The reliability of the measurement was tested at the same wavelength by comparing ZnGeP_2 with HgGa_2S_4 which led to the result d_(36)(ZnGeP_2)~3d_(36)(HgGa_2S_4), in very good agreement with previous estimations.
机译:用于中红外CdSiP_2的新型非线性晶体是最近才发现的,但对该黄铜矿的兴趣是巨大的,因为它具有相关ZnGeP_2的大部分吸引人的特性,但允许在1064 nm处进行泵浦,而没有两光子吸收且不临界相位匹配可产生6μm的光,并具有最大的有效非线性。最后一个特征是由于该晶体与显示正双折射的ZnGeP_2相反是负单轴的。现在,我们使用从种子KNbO_3光学参量放大器产生的4.6μm附近产生的飞秒脉冲的SHG来测量其非线性系数。在低转换极限(内部转换效率<10%)下比较了≈0.5mm厚的未涂覆CdSiP_2和ZnGeP_2样品的SHG效率,这证明了使用平面波近似是合理的。考虑到实验确定的Ⅰ型SHG(CdSiP_2中的oo-e型和ZnGeP_2中的ee-o型)的相位匹配角与现有的Sellmeier近似吻合得很好,我们得出d_(36)( CdSiP_2)〜d_(36)(ZnGeP_2),考虑到CdSiP_2的较大带隙,这是出乎意料的。通过比较ZnGeP_2和HgGa_2S_4在相同波长下测试的可靠性,得出的结果为d_(36)(ZnGeP_2)〜3d_(36)(HgGa_2S_4),与先前的估计非常吻合。

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