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By using Table I, we havedet( ˜β) = α2 0 − β2 0 for Rashba-Dresselhaus system, det( ˜β) = η2 for Weyl 11 system and G = 0 for PST system

Matrix elements M Ic,ab for dz ̸= 0 Suppose that dz = dz(k), we have Re[M yy,xy −1,1 ] = N ( (− ˆd2 z) ∂dy ∂kx 1 − ky d ∂d ∂ky + ∂dy ∂ky ky d ∂d ∂kx + G ˆdx d ky 1 − k d ∂d ∂k )

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Shift spin photocurrents in two-dimensional systems

cond-mat.mes-hall · 2024-11-27 · conditional · novelty 5.0

In 2D spin-orbit coupled systems, circularly polarized light can drive pure spin photocurrents, which vanish in all k-linear models unless a Zeeman field splits the bands.

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  • Shift spin photocurrents in two-dimensional systems cond-mat.mes-hall · 2024-11-27 · conditional · none · ref 2

    In 2D spin-orbit coupled systems, circularly polarized light can drive pure spin photocurrents, which vanish in all k-linear models unless a Zeeman field splits the bands.