Abstract

We consider a C6_6 invariant lattice of magnetic moments coupled via a Kondo exchange JJ 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, Qν{\mathbf Q}_ν (ν=1,2,3ν=1,2,3), is dictated by the Fermi wave number kFk_F: ∣Qν∣=2kF|{\mathbf Q}_ν |=2k_F. Consequently, the topological contribution to the Hall conductivity of the 2DEG becomes of the order of the quantized value, e2/he^2/h, when JJ is comparable to the Fermi energy εFε_F.

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