4.6 Article

Photoinduced anomalous Hall effect in two-dimensional transition metal dichalcogenides

Journal

PHYSICAL REVIEW B
Volume 103, Issue 12, Pages -

Publisher

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevB.103.125420

Keywords

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Funding

  1. U.S. Department of Energy, Office of Science, Basic Energy Sciences [DE-SC0019326]
  2. Research Grants Committee funds from the University of Alabama
  3. U.S. Department of Energy (DOE) [DE-SC0019326] Funding Source: U.S. Department of Energy (DOE)

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This study investigates the photoinduced anomalous Hall effect in undoped TMDs irradiated by a strong coherent laser field. The strong field renormalizes the equilibrium bands and opens up a dynamical energy gap, leading to notable resonant effects under the simultaneous influence of the strong ac pump field and the weak dc probe field. The anomalous Hall current is mainly driven by the intraband response of photon-dressed electron populations near the dynamical gap at both valleys, highlighting the importance of photon-dressed bands and nonequilibrium distribution functions in understanding this effect.
A circularly polarized ac pump field illuminated near resonance on two-dimensional transition metal dichalcogenides (TMDs) produces an anomalous Hall effect in response to a dc bias field. In this work, we develop a theory for this photoinduced anomalous Hall effect in undoped TMDs irradiated by a strong coherent laser field. The strong field renormalizes the equilibrium bands and opens up a dynamical energy gap where single-photon resonance occurs. The resulting photon dressed states, or Floquet states, are treated within the rotating-wave approximation. A quantum kinetic equation approach is developed to study the nonequilibrium density matrix and time-averaged transport currents under the simultaneous influence of the strong ac pump field and the weak dc probe field. Dissipative effects are taken into account in the kinetic equation that captures relaxation and dephasing. The photoinduced longitudinal and Hall conductivities display notable resonant signatures when the pump field frequency reaches the spin-split interband transition energies. Rather than valley polarization, we find that the anomalous Hall current is mainly driven by the intraband response of photon-dressed electron populations near the dynamical gap at both valleys, accompanied by a smaller contribution due to the interband response. These findings highlight the importance of photon-dressed bands and nonequilibrium distribution functions in achieving a proper understanding of the photoinduced anomalous Hall effect in a strong pump field.

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