Elementary excitations and avalanches in the Coulomb ... - PhysioNet

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$J. Phys. A: Math. Gen., Vol. 9. No. 9,1976. Printed in Great Britain ...$

Charged excitations: variable-range hoppingɛµ∆Wijrg(ɛ)g 0 (µ) ∝ 1 WMottIf(TMσ = σ 0 exp −Tg(ɛ) =c d |ɛ − µ| d−1Efros-Shklovskii) 1/4σ = σ 0 exp −(TEST) 1/2Massey and Lee, PRL 1995
Dipole excitations:ω ij = ɛ j − ɛ i − 1/r ijɛjµ∆Wirg(ɛ)r 0g 0 (µ) ∝ 1 WCompact: typical sizer 0 ∼ ∆ −1 , typical separation ∼ ω −1/3
Page 1 and 2: Elementary excitations andavalanche
Page 3 and 4: Classical electron glass model (Efr
Page 5: One-particle energy:ɛɛ i = ∑ j
Page 9: Charge avalanches1. Find a local mi
Page 12 and 13: Infinite-range spin glass3D Coulomb
Page 14 and 15: Avalanches and nonlinear screeningB
Page 16 and 17: Avalanche size distribution for dip
Page 18 and 19: # of unstable long hops created (3D
Page 20: Infinite-range spin glass3D Coulomb
Page 23 and 24: Equilibrium finite temperature 1-DO
Page 25 and 26: Zero temperature 1-DOSL = 100L = 10
Page 27: conclusionsyessaturatedquadratic ga

Elementary excitations and avalanches in the Coulomb ... - PhysioNet

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