Relativistic magnetotransport in graphene, at quantum ... - ICTP

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Compare graphene to Strongly coupled relativistic liquids Response for special strongly coupled relativistic fluids (maximally supersymmetric SU(N) Yang Mills theory with N → ∞ colors) By mapping to weakly coupled gravity problem: AdS (gravity) ↔ CFT 2+1 [SU(N>>1)] weak coupling ↔ strong coupling S. Hartnoll, P. Kovtun, MM, S. Sachdev (2007) Obtain exact results for transport via the AdS–CFT correspondence
SU(N) transport from AdS/CFT Gravitational dual to SUSY SU(N)-CFT 2+1 : Einstein-Maxwell theory It has a black hole solution (with electric and magnetic charge): AdS 3+1 Black hole (embedded in M theory as ) z = 0 Electric charge q and magnetic charge h ↔ μ and B for the CFT
Page 1 and 2: Relativistic magnetotransport in gr
Page 3 and 4: Quantum critical systems in condens
Page 5 and 6: Relativistic fluid at the Dirac poi
Page 7 and 8: Other relativistic fluids: • Syst
Page 9 and 10: Simplest example exhibiting “quan
Page 11 and 12: Graphene - Fermi liquid? 1. Tight b
Page 13 and 14: Consequences for transport 1. -Coll
Page 15 and 16: Boltzmann approach Boltzmann equati
Page 17 and 18: Hydrodynamics Hydrodynamic collisio
Page 19 and 20: Thermoelectric response S. Hartnoll
Page 21 and 22: Yes! Relativistic hydrodynamics fro
Page 23: Au+Au collisions at RHIC Quark-gluo
Page 27 and 28: Compare graphene to Strongly couple
Page 29 and 30: Graphene α = 1 T. Schäfer, Phys.
Page 31: Summary • Undoped graphene is str

Relativistic magnetotransport in graphene, at quantum ... - ICTP

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