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Soliton-induced nonlocal resonances observed through high-intensity tunable spectrally compressed second-harmonic peaks

机译:通过高强度可调谐光谱压缩的二次谐波峰观察到孤子引起的非局部共振

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摘要

Experimental data of femtosecond thick-crystal second-harmonic generation show that when tuning away from phase matching, a dominating narrow spectral peak appears in the second harmonic that can be tuned over hundreds of nanometers by changing the phase-mismatch parameter. Traditional theory explains this as phase matching between a sideband in the broadband pump to its second harmonic. However, our experiment is conducted under high input intensities and instead shows excellent quantitative agreement with a nonlocal theory describing cascaded quadratic nonlinearities. This theory explains the detuned peak as a nonlocal resonance that arises due to phase matching between the pump and a detuned second-harmonic frequency, but where in contrast to the traditional theory the pump is assumed dispersion free. As a soliton is inherently dispersion free, the agreement between our experiment and the nonlocal theory indirectly proves that we have observed a soliton-induced nonlocal resonance. The soliton exists in the self-defocusing regime of the cascaded nonlinear interaction and in the normal dispersion regime of the crystal, and needs high input intensities to become excited.
机译:飞秒厚晶体二次谐波产生的实验数据表明,当调离相位匹配时,次谐波中会出现一个占主导地位的窄光谱峰,该峰可以通过改变相位不匹配参数在数百纳米范围内调谐。传统理论将其解释为宽带泵的边带与其二次谐波之间的相位匹配。然而,我们的实验是在高输入强度下进行的,并且与描述级联二次非线性的非局部理论显示了极好的定量一致性。该理论将失谐峰解释为由于泵与失谐的二次谐波频率之间的相位匹配而产生的非局部共振,但与传统理论相反,该泵被假定为无色散。由于孤子本质上是无色散的,因此我们的实验与非局部理论之间的一致性间接证明了我们已经观察到了孤子引起的非局部共振。孤子存在于级联非线性相互作用的自散焦状态和晶体的正常色散状态,并且需要高输入强度才能激发。

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