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首页> 外文期刊>Physical review. B, Condensed Matter And Materials Physics >Weak-and strong-coupling limits of the two-dimensional Frohlich polaron with spin-orbit Rashba interaction
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Weak-and strong-coupling limits of the two-dimensional Frohlich polaron with spin-orbit Rashba interaction

机译:具有自旋轨道Rashba相互作用的二维Frohlich极化子的弱耦合和强耦合极限

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摘要

The continuous progress in fabricating low-dimensional systems with large spin-orbit couplings has reached a point in which nowadays materials may display spin-orbit splitting energies ranging from a few to hundreds of meV. This situation calls for a better understanding of the interplay between the spin-orbit coupling and other interactions ubiquitously present in solids, in particular when the spin-orbit splitting is comparable in magnitude with characteristic energy scales such as the Fermi energy and the phonon frequency. In this article, the two-dimensional Froehlich electron-phonon problem is reformulated by introducing the coupling to a spin-orbit Rashba potential, allowing for a description of the spin-orbit effects on the electron-phonon interaction. The ground state of the resulting Froehlich-Rashba polaron is studied in the weak and strong-coupling limits of the electron-phonon interaction for arbitrary values of the spin-orbit splitting. The weak-coupling case is studied within the Rayleigh-Schroedinger perturbation theory, while the strong-coupling electron-phonon regime is investigated by means of variational polaron wave functions in the adiabatic limit. It is found that, for both weak- and strong-coupling polarons, the ground-state energy is systematically lowered by the spin-orbit interaction, indicating that the polaronic character is strengthened by the Rashba coupling. It is also shown that, consistently with the lowering of the ground state, the polaron effective mass is enhanced compared to the zero spin-orbit limit. Finally, it is argued that the crossover between weakly and strongly coupled polarons can be shifted by the spin-orbit interaction.
机译:在制造具有大自旋轨道耦合的低维系统方面的不断发展已经达到了如今材料可以显示出几兆至几百meV的自旋轨道分裂能的程度。这种情况要求更好地了解自旋轨道耦合与固体中普遍存在的其他相互作用之间的相互作用,特别是当自旋轨道分裂的幅度与费米能和声子频率等特征能级相当时。在本文中,通过将耦合引入自旋轨道Rashba势来重构二维Froehlich电子-声子问题,从而可以描述自旋轨道对电子-声子相互作用的影响。对于自旋轨道分裂的任意值,在电子-声子相互作用的弱耦合和强耦合极限中研究了所得Froehlich-Rashba极化子的基态。在Rayleigh-Schroedinger扰动理论中研究了弱耦合情况,而在绝热极限中通过变极化子波函数研究了强耦合电子-声子状态。发现,对于弱耦合和强耦合极化子,自旋轨道相互作用都会系统地降低基态能量,这表明拉什巴耦合会增强极化子特性。还表明,与基态的降低一致,极化子有效质量与零自旋轨道极限相比有所提高。最后,有人争论说,弱耦合极化子和强耦合极化子之间的交叉点可以通过自旋轨道相互作用而移动。

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