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Dynamically coupled plasmon-phonon modes in GaP: An indirect-gap polar semiconductor

机译:GaP中的动态耦合等离子体激元-声子模:间接间隙极性半导体

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摘要

The ultrafast coupling dynamics of coherent optical phonons and the photoexcited electron-hole plasma in the indirect gap semiconductor GaP are investigated by experiment and theory. For below-gap excitation and probing by 800-nm light, only the bare longitudinal optical (LO) phonons are observed. For above-gap excitation with 400-nm light, the photoexcitation creates a high density, nonequilibrium e-h plasma, which introduces an additional, faster decaying oscillation due to an LO phonon-plasmon coupled (LOPC) mode. The LOPC mode frequency exhibits very similar behavior for both n- and p-doped GaP, downshifting from the LO to the transverse optical (TO) phonon frequency limits with increasing photoexcited carrier density. We assign the LOPC mode to the LO phonons coupled with the photoexcited multicomponent plasma. For the 400-nm excitation, the majority of the photoexcited electrons are scattered from the Γ valley into the satellite X valley, while the light and spin-split holes are scattered into the heavy hole band, within 30 fs. The resulting mixed plasma is strongly damped, leading to the LOPC frequency appearing in the reststrahlen gap. Due to the large effective masses of the X electrons and heavy holes, the coupled mode appears most distinctly at carrier densities approx>5 × 10~(18) cm~(-3). We perform theoretical calculations of the nuclear motions and the electronic polarizations following an excitation with an ultrashort optical pulse to obtain the transient reflectivity responses of the coupled modes. We find that, while the longitudinal diffusion of photoexcited carriers is insignificant, the lateral inhomogeneity of the photoexcited carriers due to the laser intensity profile should be taken into account to reproduce the major features of the observed coupled mode dynamics.
机译:通过实验和理论研究了相干光子与间接激发间隙半导体GaP中光激发电子-空穴等离子体的超快耦合动力学。对于间隙不足的激发和800​​ nm光的探测,仅观察到裸露的纵向光学(LO)声子。对于使用400 nm光的间隙以上激发,光激发会产生高密度的非平衡e-h等离子体,由于LO声子-等离激元耦合(LOPC)模式,它会引入额外的,更快的衰减振荡。对于n掺杂和p掺杂的GaP,LOPC模式频率表现出非常相似的行为,随着光激发载流子密度的增加,从LO降到横向光学(TO)声子频率极限。我们将LOPC模式分配给与光激发多组分等离子体耦合的LO声子。对于400 nm激发,大多数光激发电子从Γ谷散射到卫星X谷,而光和自旋分裂的空穴在30 fs内散射到重空穴带中。产生的混合等离子体被强烈阻尼,导致LOPC频率出现在剩余间隙中。由于X电子的有效质量大且空穴重,因此在载流子密度约> 5×10〜(18)cm〜(-3)时,耦合模式表现得最为明显。我们对超短光脉冲激发后的核运动和电子极化进行理论计算,以获得耦合模式的瞬态反射率响应。我们发现,尽管光激发载流子的纵向扩散微不足道,但应考虑由于激光强度分布而引起的光激发载流子的横向不均匀性,以重现观察到的耦合模态动力学的主要特征。

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  • 来源
    《Physical review》 |2015年第20期|205203.1-205203.10|共10页
  • 作者单位

    Nano Characterization Unit, National Institute for Materials Science, Tsukuba 305-0047, Japan;

    Philipps-University, Material Sciences Center and Faculty of Physics, D-35032 Marburg, Germany;

    Philipps-University, Material Sciences Center and Faculty of Physics, D-35032 Marburg, Germany;

    Department of Physics, University of Florida, Gainesville, Florida 32611, USA;

    Department of Physics, University of Florida, Gainesville, Florida 32611, USA;

    Department of Physics, University of Florida, Gainesville, Florida 32611, USA;

    Department of Physics and Astronomy and Pittsburgh Quantum Institute, University of Pittsburgh, Pittsburgh, Pennsylvania 15260, USA;

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  • 正文语种 eng
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  • 关键词

    Ⅲ-Ⅴ and Ⅱ-Ⅵ semiconductors;

    机译:Ⅲ-Ⅴ和Ⅱ-Ⅵ族半导体;

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