2020
DOI: 10.1103/physrevb.102.144109
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Quantum impurity model for anyons

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Cited by 17 publications
(16 citation statements)
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References 118 publications
(154 reference statements)
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“…We also note that the treatment in [25,31] differs from the one discussed in Refs. [21,22]: the flux tube in the latter is self-induced by an emergent (external) gauge field within the classical Fröhlich-Bogoliubov theory (which is a particular instance of the standard Maxwell electrodynamics), while in our case the flux attachment is a primary constraint built upon the microscopic Lagrangian description of the coupled systemenvironment complex (see A for further details on the microscopic Lagrangian). The consequences of this property at the microscopic level are better illustrated in terms of the imaginary-time path integral formalism, which has played a major role in the description of Brownian systems [29,30].…”
Section: Flux-carrying Brownian Particlesmentioning
confidence: 99%
See 1 more Smart Citation
“…We also note that the treatment in [25,31] differs from the one discussed in Refs. [21,22]: the flux tube in the latter is self-induced by an emergent (external) gauge field within the classical Fröhlich-Bogoliubov theory (which is a particular instance of the standard Maxwell electrodynamics), while in our case the flux attachment is a primary constraint built upon the microscopic Lagrangian description of the coupled systemenvironment complex (see A for further details on the microscopic Lagrangian). The consequences of this property at the microscopic level are better illustrated in terms of the imaginary-time path integral formalism, which has played a major role in the description of Brownian systems [29,30].…”
Section: Flux-carrying Brownian Particlesmentioning
confidence: 99%
“…The retarded self-energy in the real time domain is given by Eq. (22). To show the latter we begin with the frequency-dependent Fourier transforms of the dynamical susceptibilities, which can be computed from the back imaginary-time Fourier transforms (4), ( 10) and ( 11) via the analytic continuation [26], e.g.…”
Section: Appendix A: Nonequilibrium Generating Functionalmentioning
confidence: 99%
“…They have been conjectured [2,42,53] to be relevant for the fractional quantum Hall effect (see [24,30,28] for review). They could also be simulated in certain cold atoms systems with synthetic gauge fields [17,10,61,63,64,12].…”
Section: Model and Main Resultsmentioning
confidence: 99%
“…The full Hamiltonian (3) acts on an appropriate dense domain in the tensor product Hilbert space of the impurities L 2 sym/asym (S 2 × S 2 ), where L 2 sym (S 2 × S 2 ) is the bosonic Hilbert space and L 2 asym (S 2 × S 2 ) the fermionic one, with the Fock space F L 2 S 2 of the bath. Following the analysis for impurity problems in the planar case [25], the statistics gauge field emerges from H angulon,Ω , by restricting it to the ground state of its pure many-…”
Section: Emerging Gauge Field From the Angulon Hamiltonianmentioning
confidence: 99%
“…This opens up a whole new domain of quantum statistics known as intermediate or fractional statistics. Even though the realization of anyons in experimentally feasible systems has been subject of recent research [18][19][20][21][22][23][24][25], all these works concern particles moving on the Euclidean plane R 2 , or a subset thereof. However, since the statistical behaviour of anyons depends on the topology, and even more importantly on the geometry and symmetry, of the underlying space, investigations on curved spaces can demonstrate novel properties of quantum statistics [2,[26][27][28][29][30][31][32] (see also graph geometries [33,34]).…”
Section: Introductionmentioning
confidence: 99%