Infinite randomness and the superconductor-metal transition - PiTP

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Dynamic susceptibilites We have direct access to real dynamical quantities Im χ(ω) = 1 L ∑ ∣ Im 〈Ψ ∗ ∣∣iω→ω+iɛ x(iω)Ψ 0 (iω)〉 SN x Im χ loc (ω) = Im 〈Ψ ∗ 0 (iω)Ψ 0(iω)〉 SN ∣ ∣∣iω→ω+iɛ real frequency
Dynamic susceptibilites We have direct access to real dynamical quantities Im χ(ω) = 1 L ∑ ∣ Im 〈Ψ ∗ ∣∣iω→ω+iɛ x(iω)Ψ 0 (iω)〉 SN x Im χ loc (ω) = Im 〈Ψ ∗ 0 (iω)Ψ 0(iω)〉 SN ∣ ∣∣iω→ω+iɛ real frequency The ratio of <strong>the</strong> average to local susceptibility is related to <strong>the</strong> average cluster moment
Page 1 and 2: Infinite randomness at the supercon
Page 3 and 4: Diminutive superconductivity A macr
Page 5 and 6: What role does disorder play near t
Page 7 and 8: Fabrication of ultra-narrow wires N
Page 9 and 10: Pair-breaking in nanowires V>0 V
Page 11 and 12: Pair-breaking in nanowires V>0 V 0
Page 13 and 14: Ramazashvili and Coleman; Herbut; D
Page 15 and 16: Superconductor-metal transition T P
Page 17 and 18: Spatially dependent random coupling
Page 19 and 20: Manifestations of strong disorder U
Page 21 and 22: Exact predictions from the RTFIM D.
Page 23 and 24: Take the large-N limit Enforce a la
Page 25 and 26: Solve-Join-Patch method L = 64 solv
Page 27 and 28: Solve-Join-Patch method L = 64 solv
Page 29 and 30: Numerical investigation of observab
Page 31 and 32: Equal time correlation functions Fi
Page 33 and 34: Energy gap statistics δ ∼ α −
Page 35 and 36: Activated scaling |ln Ω| 16 14 12
Page 37: Dynamic susceptibilites We have dir
Page 41 and 42: Activated Dynamical Scaling Can der
Page 43 and 44: Origin of correspondence The physic
Page 45 and 46: Effective classical theories RTFIM

Infinite randomness and the superconductor-metal transition - PiTP

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