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Dimensional reduction for a system of 2D anyons

Nicolas Rougerie, Qiyun Yang

Abstract

Anyons with a statistical phase parameter $α\in(0,2)$ are a kind of quasi-particles that, for topological reasons, only exist in a 1D or 2D world. We consider the dimensional reduction for a 2D system of anyons in a tight wave-guide. More specifically, we study the 2D magnetic-gauge picture model with an imposed anisotropic harmonic potential that traps particles much stronger in the $y$-direction than in the $x$-direction. We prove that both the eigenenergies and the eigenfunctions are asymptotically decoupled into the loose confining direction and the tight confining direction during this reduction. The limit 1D system for the $x$-direction is given by the impenetrable Tonks-Girardeau Bose gas, which has no dependency on $α$, and no trace left of the long-range interactions of the 2D model.

Dimensional reduction for a system of 2D anyons

Abstract

Anyons with a statistical phase parameter are a kind of quasi-particles that, for topological reasons, only exist in a 1D or 2D world. We consider the dimensional reduction for a 2D system of anyons in a tight wave-guide. More specifically, we study the 2D magnetic-gauge picture model with an imposed anisotropic harmonic potential that traps particles much stronger in the -direction than in the -direction. We prove that both the eigenenergies and the eigenfunctions are asymptotically decoupled into the loose confining direction and the tight confining direction during this reduction. The limit 1D system for the -direction is given by the impenetrable Tonks-Girardeau Bose gas, which has no dependency on , and no trace left of the long-range interactions of the 2D model.
Paper Structure (15 sections, 21 theorems, 215 equations)

This paper contains 15 sections, 21 theorems, 215 equations.

Key Result

Theorem 1.1

Let $\lambda^{\mathrm{2D}}_{k}$ and $\lambda^{1\mathrm{D}}_k$ be the $k$-th eigenvalues of $H^{\mathrm{2D}}_{\varepsilon}$ and $H^{1\mathrm{D}}$ respectively (counting the multiplicity), and let $e_{\varepsilon}$ be the ground energy of $H^{\mathrm{HO}}_{\varepsilon}$. For any fixed $k$, we have, in

Theorems & Definitions (38)

  • Theorem 1.1: Relation between energies
  • Theorem 1.2: Relation between eigenfunctions
  • Theorem 2.1: Isolated two-anyon Hardy
  • proof
  • Lemma 2.2: Three-particle Hardy
  • Remark 2.3: Three-particle Hardy for anyons
  • Theorem 2.4: Many-anyon Hardy for $\alpha \in (0,2)$
  • proof
  • Corollary 2.5: $H^1$-regularity
  • proof
  • ...and 28 more