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- W2115803839 abstract "The Boltzmann equation with electron-electron (e − e) interactions has been reduced to a Fokker-Planck equation (e − e FP ) in a previuos paper. In steady-state conditions, its solution q 0 (v) (where v is the electron speed) depends on the square of the acceleration a = eE/m. If we introduce the nonrenormalized zero-point field (ZPF) of QED, i.e., the one considered in stochastic electrodynamics, so that [Formula: see text], then q 0 (v) becomes similar to the Fermi-Dirac equation, and the two collision frequencies ν 1 (v) and ν 2 (v) appearing in the e − e FP become both proportional to 1/v in a small δv interval. The condition ν 1 (v) ∝ ν 2 (v) ∝ 1/v is at the threshold of the runaways. In the same δv range, the time-dependent solution q 0 (v,τ) of the e − e FP decays no longer exponentially but according to a power law ∝ τ − ɛ where 0.004 < ɛ < 0.006, until τ → ∞. That extremely long memory of a fluctuation implies the same dependence τ − ɛ for the conductance correlation function, hence a corresponding power-spectral noise S(f) ∝ f ɛ−1 where f is the frequency. That behaviour is maintained even for a small sample because the back diffusion velocity of the electrons in the effective range δv, where they are in runaway conditions, is much larger than the drift velocity." @default.
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- W2115803839 date "2007-09-01" @default.
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- W2115803839 title "VERY LONG DECAY TIME FOR ELECTRON VELOCITY DISTRIBUTION IN SEMICONDUCTORS, AND CONSEQUENT 1/f NOISE" @default.
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- W2115803839 doi "https://doi.org/10.1142/s0219477507003842" @default.
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