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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)~d36(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 HgGa2S4 which led to the result d_(36)(ZnGeP_2)~3d_(36)(HgGa_2S_4), in very good agreement with previous estimations.
机译:对于中红外CdSiP_2新的非线性晶体只发现最近,但在这个铜矿的利益是巨大的,因为它在1064nm具有最相关ZnGeP_2的吸引人的特性,但是能够在除了抽不双光子吸收,不带偏见相位匹配为6μm的代与最大化有效非线性。最后一个功能是由于这种晶体是在对比ZnGeP_2这表明正双折射负单轴。现在,我们使用从播种KNbO_3光参量放大器附近4.6微米产生飞秒脉冲的SHG测量其非线性系数。在SHG效率CdSiP_2和ZnGeP_2,既≈0.5毫米厚的未涂覆的样品,在低转化率极限(<10%的内部转换效率),其证明使用的平面波近似的进行比较。考虑到为实验确定的相位匹配角度的I型SHG(在CdSiP_2 OO-e型和EE-O在ZnGeP_2型),这是在与现有的谢米尔近似一致,我们到达了D_(36)( CdSiP_2)〜D36(ZnGeP_2),它是相当意外的具有记CdSiP_2的较大带隙。测量的可靠性通过比较ZnGeP_2与HgGa2S4而导致的结果D_(36)(ZnGeP_2)以相同的波长测试〜3d_(36)(HgGa_2S_4),与先前的估计非常好的一致性。

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