The paper derives a density-independent renormalization of Fermi polaron g factors, g1,2 = g_X ± ξg_c, and predicts a tunable crossover from linear to elliptical polarization when magnetic field and strain compete.
For exciton inK − valley the self-energy is ΣL Mo,0 EL 0 = MT MX 2 ET ×ln 1 +MX MT ˜Er F EL 0−εL 0 +ET− MT MX ˜Er F ! .(A3b) Appendix B: Strained TMDC monolayers
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Magnetic-field control of Fermi polaron fine structure and polarization in strained monolayer semiconductors
The paper derives a density-independent renormalization of Fermi polaron g factors, g1,2 = g_X ± ξg_c, and predicts a tunable crossover from linear to elliptical polarization when magnetic field and strain compete.