The exact \(S\)-matrix for an \(\text{osp}(2| 2)\) disordered system.

From MaRDI portal
Revision as of 00:41, 30 January 2024 by Import240129110155 (talk | contribs) (Created automatically from import240129110155)
(diff) ← Older revision | Latest revision (diff) | Newer revision → (diff)

Publication:5934865

DOI10.1016/S0550-3213(00)00173-5zbMATH Open1037.82521arXivhep-th/9911105OpenAlexW2027186169MaRDI QIDQ5934865

Author name not available (Why is that?)

Publication date: 14 May 2001

Published in: (Search for Journal in Brave)

Abstract: We study a two-dimensional disordered system consisting of Dirac fermions coupled to a scalar potential. This model is closely related to a more general disordered system that has been introduced in conjunction with the integer quantum Hall transition. After disorder averaging, the interaction can be written as a marginal osp(2|2) current-current perturbation. The osp(2|2) current-current model in turn can be viewed as the fully renormalized version of an osp(2|2)^(1) Toda-type system (at the marginal point). We build non-local charges for the Toda system satisfying the U_q[osp(2|2)^(1)] quantum superalgebra. The corresponding quantum group symmetry is used to construct a Toda S-matrix for the vector representation. We argue that in the marginal (or rational) limit, this S-matrix gives the exact (Yangian symmetric) physical S-matrix for the fundamental "solitons" of the osp(2|2) current-current model.


Full work available at URL: https://arxiv.org/abs/hep-th/9911105




No records found.








This page was built for publication: The exact \(S\)-matrix for an \(\text{osp}(2| 2)\) disordered system.

Report a bug (only for logged in users!)Click here to report a bug for this page (MaRDI item Q5934865)