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Buffer 1 then promotes this local family to a finiteregion map on the( κ, λ)grid, with λ the canonical width of the region in which the residual field is screened

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cond-mat.mes-hall 1

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Thermodynamic Charge Partition in Accumulation-Layer Heterostructures

cond-mat.mes-hall · 2026-05-01 · unverdicted · novelty 7.0

Treating charge partition as the central state variable in accumulation layers produces a Helmholtz free energy and spectral path selection that yields universal master functions matching magnetocapacitance experiments.

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  • Thermodynamic Charge Partition in Accumulation-Layer Heterostructures cond-mat.mes-hall · 2026-05-01 · unverdicted · none · ref 17

    Treating charge partition as the central state variable in accumulation layers produces a Helmholtz free energy and spectral path selection that yields universal master functions matching magnetocapacitance experiments.