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arXiv 2403.04040physics.optics
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扭曲高斯谢尔模型光束的反常二次谐波产生

Anomalous Second Harmonic Generation of Twisted Gaussian Schell Model Beams

M. Gil de Oliveira, A. L. S. Santos Junior, A. C. Barbosa, B. Pinheiro da Silva, G. H. dos Santos, G. Cañas, P. H. Souto Ribeiro, S. P. Walborn, A. Z. Khoury

AI总结:

本研究通过理论与实验探究扭曲高斯谢尔模型光束的二次谐波产生,发现两种合成方法下输出光束特性不同,一种仍为TGSM光束,另一种呈带凹陷的反常交叉谱密度,且凹陷深度与扭曲相位参数相关。

摘要:

我们从理论和实验上研究了以扭曲高斯谢尔模型(twisted Gaussian Schell model, TGSM)光束为基频场的光学二次谐波产生(second harmonic generation, SHG)。我们采用II类相位匹配,分析了当输入基频光具备TGSM结构时,SHG输出光束的交叉谱密度(cross spectral density, CSD)。我们分析了两种制备TGSM基频光束的合成方法,发现其中一种方法产生的SHG仍为TGSM光束;另一种方法产生的SHG并非TGSM光束,且呈现反常的交叉谱密度,其横向空间结构中存在凹陷而非峰值。此外,我们证明该凹陷深度与扭曲相位参数直接相关,无扭曲的GSM光束不存在此凹陷。我们的结果表明,基频TGSM光束产生的SHG既可以是倍频TGSM光束,也可以是非TGSM光束,具体取决于合成方法。

英文摘要:

We investigate theoretically and experimentally the optical second harmonic generation (SHG) with a twisted Gaussian Schell model (TGSM) beam as the fundamental field. We use Type-II phase matching and analyze the cross spectral density (CSD) of the SHG output beam when the input fundamental is prepared with a TGSM structure. We analyze two synthetization methods for preparing the TGSM fundamental beam and we find that for one method the SHG is also a TGSM beam. For the other method, we find that the SHG is not a TGSM beam and presents an anomalous CSD possessing a dip instead of a peak in the transverse spatial structure. Moreover, we show that the dip depth is directly related to the twisted phase parameter, being absent for a non twisted GSM beam. Our results show that the SHG from a fundamental TGSM beam can result in a doubled frequency TGSM or in a non-TGSM beam depending on the synthetization method.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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