HANBURY BROWN & TWISS* INTERFEROMETRY WITH ANYONS

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<strong>ANYONS</strong>– why are they non trivial? no “second quantization” (cannot assign “Klein factors”)
e iπν i − e πν KLEIN FACTORS (=statistical factors) cannot be can be assigned to ANYONIC FIELD OPERATORS
Page 1 and 2: HANBURY BROWN & TWISS* INTERFEROMET
Page 3 and 4: Motivation: Two-particle interferen
Page 5 and 6: Fermions, Bosons, Classical particl
Page 7 and 8: Fermions: b ⎛ D1 ⎞ ˆ S1 ⎜
Page 9 and 10: … adding another handle: A-B flux
Page 11 and 12: ealization of HBT + AB Mach-Zehnder
Page 13 and 14: D # 2 QPC M# 2 # G G # 1 # air brid
Page 15: actual sample Neder, Ofek, Heiblum
Page 19 and 20: S1 D2 S2 S2 D2
Page 21 and 22: S1 D2 S2 S2 D2
Page 23 and 24: zero temp. kinetic eq. 0 p 0 p 1 2
Page 25 and 26: A CARICATURE WITH (Abelian) ANYONS
Page 27 and 28: Hanbury Brown & Twiss with Ferrmion
Page 29 and 30: 3 anyons + 3 anyons interferometry
Page 31 and 32: ingredients of the analysis 3 state
Page 33 and 34: One & Two Qp processes
Page 35 and 36: RATE EQUATION TREATMENT: three-stat
Page 39 and 40: qp-electron tunneling hybrids qp el

HANBURY BROWN & TWISS* INTERFEROMETRY WITH ANYONS

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