Enhanced effective masses, spin-orbit polarization, and dispersion relations in 2D hole gases under strongly asymmetric confinement

Fuente: arXiv
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Autori principali: Cockton, N. A., Sfigakis, F., Korkusinski, M., Harrigan, S. R., Nichols, G., Merino, Z. D., Zou, T., Coschizza, A. C., Joshi, T., Shetty, A., Tam, M. C., Wasilewski, Z. R., Studenikin, S. A., Austing, D. G., Baugh, J., Kycia, J. B.
Natura: Preprint
Pubblicazione: 2026
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author Cockton, N. A.
Sfigakis, F.
Korkusinski, M.
Harrigan, S. R.
Nichols, G.
Merino, Z. D.
Zou, T.
Coschizza, A. C.
Joshi, T.
Shetty, A.
Tam, M. C.
Wasilewski, Z. R.
Studenikin, S. A.
Austing, D. G.
Baugh, J.
Kycia, J. B.
author_facet Cockton, N. A.
Sfigakis, F.
Korkusinski, M.
Harrigan, S. R.
Nichols, G.
Merino, Z. D.
Zou, T.
Coschizza, A. C.
Joshi, T.
Shetty, A.
Tam, M. C.
Wasilewski, Z. R.
Studenikin, S. A.
Austing, D. G.
Baugh, J.
Kycia, J. B.
contents The dispersion of Rashba-split heavy-hole subbands in GaAs two-dimensional hole gases (2DHGs) is difficult to access experimentally because strong heavy-hole-light-hole mixing produces non-parabolicity and breaks the usual correspondence between carrier density and Fermi wave vector. Here we use low-field magnetotransport (B < 1 T) to reconstruct the dispersions of the two spin-orbit-split heavy-hole branches (HH-, HH+) in undoped (100) GaAs/AlGaAs single heterojunction 2DHGs operated in an accumulation-mode field-effect geometry. The dopant-free devices sustain out-of-plane electric fields up to 26 kV/cm while maintaining mobilities up to 84 m$^2$/Vs and exhibiting a spin-orbit polarization as large as 36%. Fourier analysis of Shubnikov-de Haas (SdH) oscillations resolves the individual HH-/HH+ subband densities; fitting the temperature dependence of the corresponding Fourier amplitudes yields both branch-resolved SdH effective masses over the same magnetic field window. SdH regimes in which reliable subband parameters can be extracted are delineated. Over 2DHG densities (0.76-1.9) $\times$ 10$^{15}$ /m$^2$, the HH- mass is nearly density independent ($\approx 0.34m_e$), implying a near-parabolic HH- dispersion below the first LH+/HH- anticrossing, whereas HH+ exhibits strong non-parabolicity with an effective mass that increases with density. Combining the extracted dispersions yields a transport-based determination of the spin-orbit splitting energy $Δ_\text{HH}$ between HH and HH+ as a function of in-plane wave vector. Parameter-free Luttinger-model calculations reproduce the qualitative trends but underestimate both masses by a common factor $\approx$ 2, suggesting a many-body renormalization of the heavy-hole mass in this strongly asymmetric regime.
format Preprint
id arxiv_https___arxiv_org_abs_2602_10852
institution arXiv
publishDate 2026
record_format arxiv
spellingShingle Enhanced effective masses, spin-orbit polarization, and dispersion relations in 2D hole gases under strongly asymmetric confinement
Cockton, N. A.
Sfigakis, F.
Korkusinski, M.
Harrigan, S. R.
Nichols, G.
Merino, Z. D.
Zou, T.
Coschizza, A. C.
Joshi, T.
Shetty, A.
Tam, M. C.
Wasilewski, Z. R.
Studenikin, S. A.
Austing, D. G.
Baugh, J.
Kycia, J. B.
Mesoscale and Nanoscale Physics
The dispersion of Rashba-split heavy-hole subbands in GaAs two-dimensional hole gases (2DHGs) is difficult to access experimentally because strong heavy-hole-light-hole mixing produces non-parabolicity and breaks the usual correspondence between carrier density and Fermi wave vector. Here we use low-field magnetotransport (B < 1 T) to reconstruct the dispersions of the two spin-orbit-split heavy-hole branches (HH-, HH+) in undoped (100) GaAs/AlGaAs single heterojunction 2DHGs operated in an accumulation-mode field-effect geometry. The dopant-free devices sustain out-of-plane electric fields up to 26 kV/cm while maintaining mobilities up to 84 m$^2$/Vs and exhibiting a spin-orbit polarization as large as 36%. Fourier analysis of Shubnikov-de Haas (SdH) oscillations resolves the individual HH-/HH+ subband densities; fitting the temperature dependence of the corresponding Fourier amplitudes yields both branch-resolved SdH effective masses over the same magnetic field window. SdH regimes in which reliable subband parameters can be extracted are delineated. Over 2DHG densities (0.76-1.9) $\times$ 10$^{15}$ /m$^2$, the HH- mass is nearly density independent ($\approx 0.34m_e$), implying a near-parabolic HH- dispersion below the first LH+/HH- anticrossing, whereas HH+ exhibits strong non-parabolicity with an effective mass that increases with density. Combining the extracted dispersions yields a transport-based determination of the spin-orbit splitting energy $Δ_\text{HH}$ between HH and HH+ as a function of in-plane wave vector. Parameter-free Luttinger-model calculations reproduce the qualitative trends but underestimate both masses by a common factor $\approx$ 2, suggesting a many-body renormalization of the heavy-hole mass in this strongly asymmetric regime.
title Enhanced effective masses, spin-orbit polarization, and dispersion relations in 2D hole gases under strongly asymmetric confinement
topic Mesoscale and Nanoscale Physics
url https://arxiv.org/abs/2602.10852