Zhang Yuhe, Wójs A, Jain J K
Department of Physics, The Pennsylvania State University, University Park, Pennsylvania 16802, USA.
Department of Theoretical Physics, Wroclaw University of Technology, Wybrzeze Wyspianskiego 27, 50-370 Wroclaw, Poland.
Phys Rev Lett. 2016 Sep 9;117(11):116803. doi: 10.1103/PhysRevLett.117.116803. Epub 2016 Sep 8.
The spin transitions in the fractional quantum Hall effect provide a direct measure of the tiny energy differences between differently spin-polarized states and thereby serve as an extremely sensitive test of the quantitative accuracy of the theory of the fractional quantum Hall effect, and, in particular, of the role of Landau-level mixing in lifting the particle-hole symmetry. We report on an accurate quantitative study of this physics, evaluating the effect of Landau-level mixing in a nonperturbative manner using a fixed-phase diffusion Monte Carlo method. We find excellent agreement between our calculated critical Zeeman energies and the experimentally measured values. In particular, we find, as also do experiments, that the critical Zeeman energies for fractional quantum Hall states at filling factors ν=2-n/(2n±1) are significantly higher than those for ν=n/(2n±1), a quantitative signature of the lifting of particle-hole symmetry due to Landau-level mixing.
分数量子霍尔效应中的自旋跃迁提供了对不同自旋极化态之间微小能量差的直接测量,从而成为对分数量子霍尔效应理论定量准确性的极其灵敏的检验,尤其是对朗道能级混合在打破粒子-空穴对称性中所起作用的检验。我们报告了对这一物理现象的精确量化研究,使用固定相位扩散蒙特卡罗方法以非微扰方式评估朗道能级混合的效应。我们发现计算得到的临界塞曼能量与实验测量值之间具有极好的一致性。特别地,我们发现,正如实验所表明的,填充因子ν=2 - n/(2n±1) 时分数量子霍尔态的临界塞曼能量显著高于ν=n/(2n±1) 时的临界塞曼能量,这是由于朗道能级混合导致粒子-空穴对称性被打破的一个定量特征。