Published June 19, 2026 | Version v1

Data for: "Coulomb screening of the orbital inverse Faraday effect in finite-size diffusive conductors"

  • 1. ROR icon National University of Science and Technology
  • 2. ROR icon Moscow Institute of Physics and Technology
  • 3. ROR icon Institute for Physics of Microstructures

Description

Data contains Matlab fig. files used to generate Figures 3, 4, 5, and 6 in the main text.

The numerical data in this repository were generated using the convention

\[ q_{\rm TF}^{\rm data} =\frac{2\pi e^2\nu}{\epsilon_{\rm env}} =\frac{1}{a_B^*}, \]

where \(\nu=m^*/2\pi\) is the density of states per spin projection. In the revised manuscript we adopt the conventional Thomas–Fermi wave vector for a spin-degenerate two-dimensional electron gas,

\[ q_{\rm TF} =\frac{4\pi e^2\nu}{\epsilon_{\rm env}} =\frac{2}{a_B^*} =2q_{\rm TF}^{\rm data}. \]

Accordingly, the numerical values of \(q_{\rm TF}\ell\) quoted in the revised manuscript are twice those used in the labels/parameters of the original deposited data. This is only a change of convention; the physical Coulomb coupling and the calculated results are unchanged. For example, \(q_{\rm TF}^{\rm data}\ell=0.1,\,0.2,\,0.5\) correspond to \(q_{\rm TF}\ell=0.2,\,0.4,\,1.0\) in the revised manuscript.

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