Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Physics Today

Third dimension for anyons

Published Apr 1, 2010• 0 citations
Publisher
DOI
10.1063/pt.5.024208

Related papers

Another dimension for anyons

Chetan Nayak

Nature•Mar 30, 2010•10 citations

Anyons in 1 + 1 dimensions

J. Gamboa, J. Zanelli

arXiv:hep-th/9503126•Physics Letters B•Aug 1, 1995•6 citations

Effect of third dimension on the properties of phases with gauge flux (anyons)

I. E. Dzyaloshinskiǐ

JETPL•Dec 1, 1989•0 citations

Disordered Pinned Anyons in Two Dimensions

Chris R. Laumann, David A. Huse, Andreas Ludwig +3 more

Bulletin of the American Physical Society•Mar 23, 2011•0 citations

Interacting anyons in one dimension: The Fibonacci chain

Andreas W. W. Ludwig, Adrian E. Feiguin, Simon Trebst +4 more

Bulletin of the American Physical Society•Mar 6, 2007•0 citations

Spectrum of three anyons in a harmonic potential and the third virial coefficient

Diptiman Sen

We use supersymmetric quantum mechanics to show that the spectrum of three anyons in a harmonic potential exhibits an almost complete mirror symmetry about semions. Barring a subset of exactly solved states, all states come in pairs such that the energy of one state with the statistics parameter \ensuremath{\theta} is equal to the energy of its partner state at \ensuremath{\pi}-\ensuremath{\theta}. Bosons, semions, and fermions have \ensuremath{\theta}=0,\ensuremath{\pi}/2, and \ensuremath{\pi}, respectively. From this, we show that the third virial coefficient of an ideal anyon gas is exactly mirror symmetric about semions.

Physical Review Letters•May 18, 1992•31 citations
We use supersymmetric quantum mechanics to show that the spectrum of three anyons in a harmonic potential exhibits an almost complete mirror symmetry about semions. Barring a subset of exactly solved states, all states come in pairs such that the energy of one state with the statistics parameter \ensuremath{\theta} is equal to the energy of its partner state at \ensuremath{\pi}-\ensuremath{\theta}. Bosons, semions, and fermions have \ensuremath{\theta}=0,\ensuremath{\pi}/2, and \ensuremath{\pi}, respectively. From this, we show that the third virial coefficient of an ideal anyon gas is exactly mirror symmetric about semions.