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The first harmonic generation and linear susceptibility tensor variation at crystal boundary

机译:晶体边界处的一次谐波产生和线性磁化率张量变化

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It’s widely agreed that optical characteristics at crystal boundary may change comparing to the internalpart of bulk crystal but, as far as we know, sometimes the phenomenon, for example, the variation ofsusceptibility usually can’t be intuitively, simply presented in experiments. Recently, we observe akind of special harmonic generation which is at the same wavelength as incident light. Besides, thiskind of harmonic generation behaves in a similar way with nonlinear Cherenkov radiation, thus we callit linear Cherenkov radiation (LCR). We theoretically predict and calculate the phase-matching schemeand radiation path of LCR. In our experiment, we employ a polished KDP to verify our theory aboutthe conversion of polarization in this process, and the phenomenon also help to rule out the possibilityof birefringence at boundary. Combining with the coupling wave equation, we can derive new elementsin linear susceptibility tensor according to the polarization states of incident light and LCR. The resulttells us the linear susceptibility at the KDP boundary is assuredly different from that in bulk crystal,and this is mainly because of the breakdown of crystal symmetry at boundary, in our opinion. Theexistence of LCR is evidence of the variation of linear susceptibility. And in return, we could use thisphenomenon to probe the non-zero elements in the tensor.
机译:人们普遍认为,与内部相比,晶体边界处的光学特性可能会发生变化。 块状晶体的一部分,但据我们所知,有时会出现这种现象,例如 通常在实验中无法简单地直观地看出磁化率。最近,我们观察到 一种特殊的谐波产生,与入射光具有相同的波长。除此以外 一种谐波的产生与非线性Cherenkov辐射的行为类似,因此我们称 它是线性切伦科夫辐射(LCR)。我们从理论上预测并计算相位匹配方案 和LCR的辐射路径。在我们的实验中,我们使用了完善的KDP来验证关于 在此过程中极化的转换,这种现象也有助于排除可能性 边界处的双折射。结合耦合波方程,我们可以得出新的元素 线性磁化张量根据入射光和LCR的偏振态而定。结果 告诉我们,KDP边界处的线性磁化率肯定与块状晶体中的线性磁化率不同, 我们认为,这主要是由于边界处晶体对称性的破坏。这 LCR的存在是线性磁化率变化的证据。作为回报,我们可以使用这个 现象以探究张量中的非零元素。

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