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.
The finite-buffer multisubband system does not produce a second pair of fitted master curves, but a tabulated family of master surfaces on the(κ, λ)grid
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Thermodynamic Charge Partition in Accumulation-Layer Heterostructures
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.