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arXiv:0812.4145 · Annals of Physics

An explicit realization of fractional statistics in one dimension

S. Sree Ranjani, Prasanta Kumar Panigrahi, Ashok Kumar Kapoor, Avinash Khare

Published Feb 13, 2009• 10 citations
arXivHTMLPDF
DOI
10.1016/j.aop.2009.01.007

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Anyons, unique to two spatial dimensions, underlie extraordinary phenomena such as the fractional quantum Hall effect, but their generalization to higher dimensions has remained elusive. The topology of Eilenberg-MacLane spaces constrains the loop statistics to be only bosonic or fermionic in any dimension. In this Letter, we introduce the novel anyonic statistics for membrane excitations in four dimensions. Analogous to the Z_{N} particle exhibiting Z_{N×gcd(2,N)} anyonic statistics in two dimensions, we show that the Z_{N} membrane possesses Z_{N×gcd(3,N)} anyonic statistics in four dimensions. Given unitary volume operators that create membrane excitations on the boundary, we propose an explicit 56-step unitary sequence that detects the membrane statistics. We further analyze the boundary theory of (5+1)D 1-form Z_{N} symmetry-protected topological phases and demonstrate that their domain walls realize all possible anyonic membrane statistics. We then show that the Z_{3} subgroup persists in all higher dimensions. In addition to the standard fermionic Z_{2} membrane statistics arising from Stiefel-Whitney classes, membranes also exhibit Z_{3} statistics associated with Pontryagin classes. We explicitly verify that the 56-step process detects the nontrivial Z_{3} statistics in five, six, and seven spatial dimensions. Moreover, in seven and higher dimensions, the statistics of membrane excitations stabilize to Z_{2}×Z_{3}, with the Z_{3} sector consistently captured by this process.
Quantum statistics plays a fundamental role in the laws of nature. Haldane fractional exclusion statistics (FES) generalizes the Pauli exclusion statistics, and can emerge in the properties of elementary particles and hole excitations of a quantum system consisting of conventional bosons or fermions. FES has a long history of intensive studies, but its simple realization in interacting physical systems is rare. Here we report a simple non-mutual FES that depicts the particle-hole symmetry breaking in interacting Bose gases at a quantum critical point. We show that the FES distribution directly comes from particle-hole symmetry breaking. Based on exact solutions, quantum Monte Carlo simulations and experiments, we find that, over a wide range of interaction strengths, the macroscopic physical properties of these gases are determined by non-interacting quasi-particles that obey non-mutual FES of the same form in one and two dimensions. Whereas strongly interacting Bose gases reach full fermionization in one dimension, they exhibit incomplete fermionization in two dimensions. Our results provide a generic connection between interaction-induced particle-hole symmetry breaking (depicted by FES) and macroscopic properties of many-body systems in arbitrary dimensions. Our work lays the groundwork for using FES to explore quantum criticality and other novel many-body phenomena in strongly correlated quantum systems.
Transport properties of the multicomponent quantum many-body systems obeying Haldane's fractional exclusion statistics are studied in one dimension. By computing the finite-size spectrum under twisted boundary conditions, we explicitly express the conductivity and conductance in terms of statistical interactions. Through this analysis, the effective charge and effective mass for collective excitations are determined. We apply the results for l/r 2 quantum systems as well as for correlated electron systems.