Infinite randomness and the superconductor-metal transition - PiTP

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Putting it all together ν ψ φ RTFIM 2 1/2 (1+√5)/2 SMT 1.9(2) 0.53(6) 1.6(2) Numerical confirmation of the strong disorder RG calculations of Hoyos, Kotabage and Vojta!
Origin of correspondence The physics of infinite randomness comes from the slow dynamics and large contribution of rare regions imaginary time space
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 and 38: Dynamic susceptibilites We have dir
Page 39 and 40: Dynamic susceptibilites We have dir
Page 41: Activated Dynamical Scaling Can der
Page 45 and 46: Effective classical theories RTFIM

Infinite randomness and the superconductor-metal transition - PiTP

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