Matches in SemOpenAlex for { <https://semopenalex.org/work/W2891741477> ?p ?o ?g. }
- W2891741477 endingPage "559" @default.
- W2891741477 startingPage "507" @default.
- W2891741477 abstract "The supersymmetric reformulation of physical observables in the Chalker-Coddington model (CC) for the plateau transition in the integer quantum Hall effect leads to a reformulation of its critical properties in terms of a 2D non-compact loop model or a 1D non-compact $gl(2|2)$ spin chain. Following a proposal by Ikhlef, Fendley and Cardy, we define and study a series of truncations of these loop models and spin chains, involving a finite and growing number of degrees of freedom per site. The case of the first truncation is solved analytically using the Bethe-ansatz. It is shown to exhibit many of the qualitative features expected for the untruncated theory, including a quadratic spectrum of exponents with a continuous component, and a normalizable ground state below that continuum. Quantitative properties are however at odds with the results of simulations on the CC model. Higher truncations are studied only numerically. While their properties are found to get closer to those of the CC model, it is not clear whether this is a genuine effect, or the result of strong finite-size corrections." @default.
- W2891741477 created "2018-09-27" @default.
- W2891741477 creator A5001072764 @default.
- W2891741477 creator A5020505720 @default.
- W2891741477 creator A5027386297 @default.
- W2891741477 creator A5060806360 @default.
- W2891741477 date "2019-04-01" @default.
- W2891741477 modified "2023-10-16" @default.
- W2891741477 title "On truncations of the Chalker-Coddington model" @default.
- W2891741477 cites W1963861987 @default.
- W2891741477 cites W1964280100 @default.
- W2891741477 cites W1966336053 @default.
- W2891741477 cites W1970484418 @default.
- W2891741477 cites W1979736120 @default.
- W2891741477 cites W1980368780 @default.
- W2891741477 cites W1985147238 @default.
- W2891741477 cites W1986744105 @default.
- W2891741477 cites W1994120532 @default.
- W2891741477 cites W2000936432 @default.
- W2891741477 cites W2008972373 @default.
- W2891741477 cites W2009593131 @default.
- W2891741477 cites W2012341832 @default.
- W2891741477 cites W2012816531 @default.
- W2891741477 cites W2020614562 @default.
- W2891741477 cites W2033744434 @default.
- W2891741477 cites W2039450476 @default.
- W2891741477 cites W2041948597 @default.
- W2891741477 cites W2044078055 @default.
- W2891741477 cites W2046938841 @default.
- W2891741477 cites W2056216451 @default.
- W2891741477 cites W2063129650 @default.
- W2891741477 cites W2072243495 @default.
- W2891741477 cites W2089729930 @default.
- W2891741477 cites W2092233299 @default.
- W2891741477 cites W2104055252 @default.
- W2891741477 cites W2118840193 @default.
- W2891741477 cites W2123122881 @default.
- W2891741477 cites W2130517342 @default.
- W2891741477 cites W2144660969 @default.
- W2891741477 cites W2229825737 @default.
- W2891741477 cites W2566427550 @default.
- W2891741477 cites W2610279556 @default.
- W2891741477 cites W3098451938 @default.
- W2891741477 cites W3102077547 @default.
- W2891741477 cites W3104422899 @default.
- W2891741477 cites W3104850289 @default.
- W2891741477 cites W3150268706 @default.
- W2891741477 doi "https://doi.org/10.1016/j.nuclphysb.2019.02.015" @default.
- W2891741477 hasPublicationYear "2019" @default.
- W2891741477 type Work @default.
- W2891741477 sameAs 2891741477 @default.
- W2891741477 citedByCount "3" @default.
- W2891741477 countsByYear W28917414772019 @default.
- W2891741477 countsByYear W28917414772020 @default.
- W2891741477 crossrefType "journal-article" @default.
- W2891741477 hasAuthorship W2891741477A5001072764 @default.
- W2891741477 hasAuthorship W2891741477A5020505720 @default.
- W2891741477 hasAuthorship W2891741477A5027386297 @default.
- W2891741477 hasAuthorship W2891741477A5060806360 @default.
- W2891741477 hasBestOaLocation W28917414771 @default.
- W2891741477 hasConcept C105795698 @default.
- W2891741477 hasConcept C106195933 @default.
- W2891741477 hasConcept C121332964 @default.
- W2891741477 hasConcept C121864883 @default.
- W2891741477 hasConcept C129844170 @default.
- W2891741477 hasConcept C199360897 @default.
- W2891741477 hasConcept C208081375 @default.
- W2891741477 hasConcept C2524010 @default.
- W2891741477 hasConcept C32848918 @default.
- W2891741477 hasConcept C33923547 @default.
- W2891741477 hasConcept C37914503 @default.
- W2891741477 hasConcept C41008148 @default.
- W2891741477 hasConcept C42704618 @default.
- W2891741477 hasConcept C62520636 @default.
- W2891741477 hasConcept C69523127 @default.
- W2891741477 hasConcept C77843276 @default.
- W2891741477 hasConcept C84114770 @default.
- W2891741477 hasConcept C97137487 @default.
- W2891741477 hasConcept C97355855 @default.
- W2891741477 hasConceptScore W2891741477C105795698 @default.
- W2891741477 hasConceptScore W2891741477C106195933 @default.
- W2891741477 hasConceptScore W2891741477C121332964 @default.
- W2891741477 hasConceptScore W2891741477C121864883 @default.
- W2891741477 hasConceptScore W2891741477C129844170 @default.
- W2891741477 hasConceptScore W2891741477C199360897 @default.
- W2891741477 hasConceptScore W2891741477C208081375 @default.
- W2891741477 hasConceptScore W2891741477C2524010 @default.
- W2891741477 hasConceptScore W2891741477C32848918 @default.
- W2891741477 hasConceptScore W2891741477C33923547 @default.
- W2891741477 hasConceptScore W2891741477C37914503 @default.
- W2891741477 hasConceptScore W2891741477C41008148 @default.
- W2891741477 hasConceptScore W2891741477C42704618 @default.
- W2891741477 hasConceptScore W2891741477C62520636 @default.
- W2891741477 hasConceptScore W2891741477C69523127 @default.
- W2891741477 hasConceptScore W2891741477C77843276 @default.
- W2891741477 hasConceptScore W2891741477C84114770 @default.
- W2891741477 hasConceptScore W2891741477C97137487 @default.
- W2891741477 hasConceptScore W2891741477C97355855 @default.