Matches in SemOpenAlex for { <https://semopenalex.org/work/W2058725323> ?p ?o ?g. }
- W2058725323 endingPage "384" @default.
- W2058725323 startingPage "361" @default.
- W2058725323 abstract "We study the spectral properties of a chiral random banded matrix (chRBM) with elements decaying as a power-law ${{cal H}_{ij}}sim |i-j|^{-alpha}$. This model is equivalent to a chiral 1D Anderson Hamiltonian with long range power-law hopping. In the weak disorder limit we obtain explicit nonperturbative analytical results for the density of states and the two-level correlation function by mapping the chRBM onto a nonlinear sigma model. We also put forward, by exploiting the relation between the chRBM at $alpha=1$ and a generalized chiral random matrix model, an exact expression for the above correlation functions. We give compelling analytical and numerical evidence that for this value the chRBM reproduces all the features of an Anderson transition. Finally we discuss possible applications of our results to QCD." @default.
- W2058725323 created "2016-06-24" @default.
- W2058725323 creator A5007195436 @default.
- W2058725323 creator A5009976413 @default.
- W2058725323 date "2004-11-01" @default.
- W2058725323 modified "2023-10-02" @default.
- W2058725323 title "Long range disorder and Anderson transition in systems with chiral symmetry" @default.
- W2058725323 cites W1528946541 @default.
- W2058725323 cites W1534301718 @default.
- W2058725323 cites W1967992669 @default.
- W2058725323 cites W1969811169 @default.
- W2058725323 cites W1973122949 @default.
- W2058725323 cites W1981447860 @default.
- W2058725323 cites W1982170218 @default.
- W2058725323 cites W1985126950 @default.
- W2058725323 cites W1988102507 @default.
- W2058725323 cites W1990446578 @default.
- W2058725323 cites W1996945771 @default.
- W2058725323 cites W2003113244 @default.
- W2058725323 cites W2006141728 @default.
- W2058725323 cites W2006920602 @default.
- W2058725323 cites W2007398620 @default.
- W2058725323 cites W2018640768 @default.
- W2058725323 cites W2023023074 @default.
- W2058725323 cites W2023163263 @default.
- W2058725323 cites W2043932940 @default.
- W2058725323 cites W2045454519 @default.
- W2058725323 cites W2046921937 @default.
- W2058725323 cites W2048624782 @default.
- W2058725323 cites W2049587182 @default.
- W2058725323 cites W2049803877 @default.
- W2058725323 cites W2052382979 @default.
- W2058725323 cites W2052796696 @default.
- W2058725323 cites W2055288739 @default.
- W2058725323 cites W2058513304 @default.
- W2058725323 cites W2061035561 @default.
- W2058725323 cites W2062790565 @default.
- W2058725323 cites W2063987903 @default.
- W2058725323 cites W2064257524 @default.
- W2058725323 cites W2076740525 @default.
- W2058725323 cites W2080726719 @default.
- W2058725323 cites W2082398151 @default.
- W2058725323 cites W2083240980 @default.
- W2058725323 cites W2089663769 @default.
- W2058725323 cites W2111271983 @default.
- W2058725323 cites W2120855720 @default.
- W2058725323 cites W2160665252 @default.
- W2058725323 cites W2264002775 @default.
- W2058725323 cites W2601300439 @default.
- W2058725323 cites W3099968882 @default.
- W2058725323 cites W3100327175 @default.
- W2058725323 cites W3100772153 @default.
- W2058725323 cites W3101399646 @default.
- W2058725323 cites W3102852086 @default.
- W2058725323 cites W3105823421 @default.
- W2058725323 cites W3106532397 @default.
- W2058725323 doi "https://doi.org/10.1016/j.nuclphysb.2004.08.035" @default.
- W2058725323 hasPublicationYear "2004" @default.
- W2058725323 type Work @default.
- W2058725323 sameAs 2058725323 @default.
- W2058725323 citedByCount "12" @default.
- W2058725323 countsByYear W20587253232012 @default.
- W2058725323 countsByYear W20587253232017 @default.
- W2058725323 countsByYear W20587253232020 @default.
- W2058725323 countsByYear W20587253232021 @default.
- W2058725323 crossrefType "journal-article" @default.
- W2058725323 hasAuthorship W2058725323A5007195436 @default.
- W2058725323 hasAuthorship W2058725323A5009976413 @default.
- W2058725323 hasBestOaLocation W20587253233 @default.
- W2058725323 hasConcept C105795698 @default.
- W2058725323 hasConcept C121332964 @default.
- W2058725323 hasConcept C121864883 @default.
- W2058725323 hasConcept C126255220 @default.
- W2058725323 hasConcept C130787639 @default.
- W2058725323 hasConcept C133386390 @default.
- W2058725323 hasConcept C133654230 @default.
- W2058725323 hasConcept C147120987 @default.
- W2058725323 hasConcept C158622935 @default.
- W2058725323 hasConcept C158693339 @default.
- W2058725323 hasConcept C188234980 @default.
- W2058725323 hasConcept C2524010 @default.
- W2058725323 hasConcept C2778049214 @default.
- W2058725323 hasConcept C2779886137 @default.
- W2058725323 hasConcept C2781313195 @default.
- W2058725323 hasConcept C33923547 @default.
- W2058725323 hasConcept C37914503 @default.
- W2058725323 hasConcept C53622274 @default.
- W2058725323 hasConcept C62520636 @default.
- W2058725323 hasConcept C64812099 @default.
- W2058725323 hasConcept C87040749 @default.
- W2058725323 hasConceptScore W2058725323C105795698 @default.
- W2058725323 hasConceptScore W2058725323C121332964 @default.
- W2058725323 hasConceptScore W2058725323C121864883 @default.
- W2058725323 hasConceptScore W2058725323C126255220 @default.
- W2058725323 hasConceptScore W2058725323C130787639 @default.
- W2058725323 hasConceptScore W2058725323C133386390 @default.
- W2058725323 hasConceptScore W2058725323C133654230 @default.
- W2058725323 hasConceptScore W2058725323C147120987 @default.