Abstract:We study theoretically and numerically the ground state of a gas of 2D abelian anyons in an external trapping potential. We treat anyon statistics in the magnetic gauge picture, perturbatively around the bosonic end. This leads to a mean-field energy functional, whose ground state displays vortex lattices similar to those found in rotating Bose-Einstein condensates. A crucial difference is however that the vortex density is proportional to the underlying matter density of the gas. PACS numbers: 05.30.Pr, 03.75… Show more
“…Only recently have we become aware of the work in Refs. [160,161], for which a similar effective theory is considered. We find consistent findings with these studies at the points where both works overlap.…”
Topological field theories emerge at low energy in strongly correlated condensed matter systems and appear in the context of planar gravity. In particular, the study of Chern-Simons terms gives rise to the concept of flux attachment when the gauge field is coupled to matter, yielding flux-charge composites. We investigate the generation of flux attachment in a Bose-Einstein condensate in the presence of nonlinear synthetic gauge potentials. In doing so, we identify the U (1) Chern-Simons gauge field as a singular density-dependent gauge potential, which in turn can be expressed as a Berry connection. We envisage a proof-of-concept scheme where the artificial gauge field is perturbatively induced by an effective light-matter detuning created by interparticle interactions. At a mean field level, we recover the action of a "charged" superfluid minimally coupled to both a background and a Chern-Simons gauge field. Remarkably, a localized density perturbation in combination with a nonlinear gauge potential gives rise to an effective composite boson model of fractional quantum Hall effect, displaying anyonic vortices.
“…Only recently have we become aware of the work in Refs. [160,161], for which a similar effective theory is considered. We find consistent findings with these studies at the points where both works overlap.…”
Topological field theories emerge at low energy in strongly correlated condensed matter systems and appear in the context of planar gravity. In particular, the study of Chern-Simons terms gives rise to the concept of flux attachment when the gauge field is coupled to matter, yielding flux-charge composites. We investigate the generation of flux attachment in a Bose-Einstein condensate in the presence of nonlinear synthetic gauge potentials. In doing so, we identify the U (1) Chern-Simons gauge field as a singular density-dependent gauge potential, which in turn can be expressed as a Berry connection. We envisage a proof-of-concept scheme where the artificial gauge field is perturbatively induced by an effective light-matter detuning created by interparticle interactions. At a mean field level, we recover the action of a "charged" superfluid minimally coupled to both a background and a Chern-Simons gauge field. Remarkably, a localized density perturbation in combination with a nonlinear gauge potential gives rise to an effective composite boson model of fractional quantum Hall effect, displaying anyonic vortices.
“…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].…”
In two-dimensional space there are possibilities for quantum statistics continuously interpolating between the bosonic and the fermionic one. Quasi-particles obeying such statistics can be described as ordinary bosons and fermions with magnetic interactions. We study a limit situation where the statistics/magnetic interaction is seen as a "perturbation from the fermionic end". We vindicate a mean-field approximation, proving that the ground state of a gas of anyons is described to leading order by a semi-classical, Vlasov-like, energy functional. The ground state of the latter displays anyonic behavior in its momentum distribution. Our proof is based on coherent states, Husimi functions, the Diaconis-Freedman theorem and a quantitative version of a semi-classical Pauli pinciple.
“…[66][67][68][69][70][71]. Another approach has been to first regularize the Hamiltonian (5) by making the fluxes extended [72][73][74][75], and in this situation an exact averagefield theory and a corresponding Thomas-Fermi theory may be derived in the almost-bosonic limit α ∼ N −1 → 0 [28,[76][77][78][79]. Also singular or point-interacting anyons may be considered [80][81][82][83][84], as well as anyons regularized by a strong magnetic field [85].…”
Section: A Regular Anyon Hamiltonianmentioning
confidence: 99%
“…From the practical point of view, however, it does not give much insight concerning a physical realization. Indeed there has been a recent upsurge in interest concerning the realization of anyons as emergent quasiparticles in experimentally feasible systems, in particular from the perspective of deriving robust, testable predictions such as density signatures [22][23][24][25][26][27][28]. Also the emergence of anyons in a FQHE setting by means of attachment of flux via Laughlin quasiholes was recently revisited and elaborated on arXiv:1912.07890v1 [cond-mat.quant-gas] 17 Dec 2019 in Ref.…”
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