首页> 外文期刊>Journal of Physics. Condensed Matter >Drag thermopower in nanowires and bulk potassium crystals under the conditions of competition between the boundary and bulk mechanisms of phonon relaxation
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Drag thermopower in nanowires and bulk potassium crystals under the conditions of competition between the boundary and bulk mechanisms of phonon relaxation

机译:将纳米线和散装钾晶体中的蒸发散热器拖曳在声子放松的边界和散装机制之间的竞争条件下

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摘要

At low temperatures, the influence of anisotropy of elastic energy on the electron-phonon drag and thermopower in square cross-section single crystals of potassium has been studied. Change in the role of quasi-longitudinal and quasi-transverse phonons in the anisotropy of the drag thermopower under the conditions of transition from nanowires to bulk single crystals has been analyzed. In the regime of the Knudsen phonon gas flow, slow quasi-transverse phonons are shown to predominantly contribute to the drag thermopower in the nanowires but only in the directions close to the focusing of longitudinal phonons. Change in the drag thermopower anisotropy under the conditions of competition between the boundary and bulk phonon relaxation mechanisms has been investigated. As the sample's cross-section increases, the drag thermopower anisotropy varies non-monotonically. This occurs due to stronger scattering of longitudinal phonons by electrons. When transitioning from the Knudsen phonon gas flow regime to the bulk relaxation mechanisms, the drag thermopower anisotropy first rises, then reaches a maximum and afterward disappears. The contribution of quasi-transverse phonons in bulk potassium crystals exceeds that of longitudinal phonons by an order of magnitude. This result evidences that the model of an isotropic medium cannot properly describe the electron-phonon drag in metals.
机译:在低温下,研究了在钾的方形横截面单晶中的电子位置拖曳和热电机上的各向异性的影响。已经分析了在从纳米线到散装单晶的转变条件下的准纵向和准横向声子的作用。在Chaudsen声子流量的制度中,示出慢的准横向声子被认为主要有助于纳米线中的拖曳热量,而是仅在靠近纵向声子的聚焦的方向上。研究了在边界和散装音张弛豫机制之间竞争条件下的阻力热量各向异性的变化。随着样品的横截面增加,拖曳热量各向异性无单调地变化。这是由于电子通过电子纵向声子散射的散射而发生。当从Knudsen声子气流制度转变为散装弛豫机构时,拖曳热电机各向异性首先升高,然后达到最大,然后之后消失。准横向声子在散装钾晶体中的贡献超过了纵向声子的数量级的贡献。该结果证明了各向同性培养基的模型不能正确描述金属中的电子 - 声子阻力。

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