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

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

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

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Avalanches <strong>in</strong> <strong>the</strong> <strong>in</strong>f<strong>in</strong>ite-range sp<strong>in</strong> glass (Sherr<strong>in</strong>gton-Kirpatrick model):“self-organized criticality” (Pazm<strong>and</strong>i, Zar<strong>and</strong>, Zimanyi 1999)H = ∑ i

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Spectroscopic aspect of the cationic dye Basic Orange 21

Planar Hall-effect magnetic random access memory

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Cooper-pair-insulator-to-Superinsulator transition in thin ... - PhysioNet

Amir Bashan -CV - PhysioNet

Avalanches <strong>in</strong> <strong>the</strong> <strong>in</strong>f<strong>in</strong>ite-range sp<strong>in</strong> glass (Sherr<strong>in</strong>gton-Kirpatrick model):“self-organized criticality” (Pazm<strong>and</strong>i, Zar<strong>and</strong>, Zimanyi 1999)H = ∑ i

Page 1 and 2: Elementary excitations andavalanche
Page 3 and 4: Classical electron glass model (Efr
Page 5 and 6: One-particle energy:ɛɛ i = ∑ j
Page 7 and 8: Dipole excitations:ω ij = ɛ j −
Page 9: Charge avalanches1. Find a local mi
Page 13 and 14: “Equilibrium glass phase”Infini
Page 15 and 16: obust and does not require fine tun
Page 17 and 18: Average number of dipoles destabili
Page 19 and 20: Long hops explain why cutoff S c
Page 22 and 23: Numerical determination of the 1-DO
Page 24 and 25: Self-consistent equation (SCE):(Efr
Page 26 and 27: Zero temperature 1-DOSFinite-size e