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arXiv 2606.02012physics.opticscond-mat.other
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布拉格增强的传播声栅时域布里渊散射

Bragg-enhanced time-domain Brillouin scattering from a propagating acoustic grating

Technische Universität Dortmund(多特蒙德工业大学)

O. S. Ken, D. O. Horiachyi, V. L. Korenev, A. V. Trifonov, I. A. Akimov, D. R. Yakovlev, M. Bayer

AI总结:

利用高重复频率飞秒激光脉冲激发半导体中的传播声栅,通过布拉格反射增强时域布里渊散射信号,实现10-30倍增强。

摘要:

通过飞秒光脉冲在半导体中产生和检测相干声子是高频声控其电子特性的有力工具。在这里,我们利用重复频率为1 GHz的激光脉冲序列,通过带隙以上激发在体半导体中演示了传播的一维声栅。这种方法能够塑造相干声子谱,并在泵浦-探测配置中在选定的探测波长处显著增强布里渊光散射。我们在原型半导体系统(即体晶GaAs和(Cd,Zn)Te)中于5 K低温下展示了这一效应,这些材料作为所提出方法的基准材料。时域布里渊光散射振幅的光谱依赖性在离散探测波长处表现出共振峰,这些峰源于探测光被传播声栅的布拉格反射。对于GaAs和(Cd,Zn)Te,观察到信号振幅的10-30倍共振增强,这由探测脉冲的有限光谱宽度决定。随着光谱进一步变窄,预计增强可达约100-150倍,这由样品内声栅中应变脉冲的数量N决定,并最终受限于材料参数和样品厚度。

英文摘要:

Generation and detection of coherent phonons in semiconductors by femtosecond optical pulses is a powerful tool for high-frequency acoustic control of their electronic properties. Here, we demonstrate a propagating one-dimensional acoustic grating in bulk semiconductors using above-band-gap excitation by a train of laser pulses with high repetition rate of 1 GHz. This approach enables shaping of the coherent acoustic phonon spectrum and leads to a significant enhancement of Brillouin light scattering at selected probe wavelengths in pump-probe configuration. We demonstrate this effect at a cryogenic temperature of 5 K in prototypical semiconductor systems, namely bulk crystalline GaAs and (Cd,Zn)Te, which serve as benchmark materials for the proposed method. The spectral dependence of the time-domain Brillouin light scattering amplitude exhibits resonant peaks at discrete probe wavelengths arising from Bragg reflection of the probe light by the propagating acoustic grating. A 10-30-fold resonant enhancement of the signal amplitude is observed for GaAs and (Cd,Zn)Te, determined by the finite spectral width of the probe pulse. With further spectral narrowing, enhancements of the order ~ 100-150 are expected, set by the number N of strain pulses in the acoustic grating within the sample and ultimately limited by the material parameters and sample thickness.

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