2019/11/30 by Zhentao Wang, Ying Su, Shi-Zeng Lin +1
Physics and Astronomy · #cond-mat.str-el #cond-mat.mes-hall #cond-mat.mtrl-sci
paper · pdf · doi:10.1103/physrevlett.124.207201
published as Phys. Rev. Lett. 124, 207201 (2020) · 7 pages, 4 figures
arxiv created 2020/05/19 · arxiv updated 2020/05/20
We consider a C6 invariant lattice of magnetic moments coupled via a Kondo exchange J with a 2D electron gas (2DEG). The effective Ruderman-Kittel-Kasuya-Yosida interaction between the moments stabilizes a magnetic skyrmion crystal in the presence of magnetic field and easy-axis anisotropy. An attractive aspect of this mechanism is that the magnitude of the magnetic ordering wave vectors, \mathbf Qν (ν=1,2,3), is dictated by the Fermi wave number kF: |\mathbf Qν |=2kF. Consequently, the topological contribution to the Hall conductivity of the 2DEG becomes of the order of the quantized value, e2/h, when J is comparable to the Fermi energy εF.