Matches in SemOpenAlex for { <https://semopenalex.org/work/W1996403735> ?p ?o ?g. }
- W1996403735 abstract "Exact expressions for correlation functions are known for the large-$N$ (planar) limit of the $(1+1)$-dimensional ${rm SU}(N)times {rm SU}(N)$ principal chiral sigma model. These were obtained with the form-factor bootstrap, an entirely nonperturbative method. The large-$N$ solution of this asymptotically-free model is far less trivial than that of O($N$) sigma model (or other isovector models). Here we study the Euclidean two-point correlation function $N^{-1}< {rm Tr},Phi(0)^{dagger} Phi(x)>$, where $Phi(x)sim Z^{-1/2}U(x)$ is the scaling field and $U(x)in SU(N)$ is the bare field. We express the two-point function in terms of the spectrum of the operator $sqrt{-d^{2}/du^{2}}$, where $uin (-1,1)$. At short distances, this expression perfectly matches the result from the perturbative renormalization group." @default.
- W1996403735 created "2016-06-24" @default.
- W1996403735 creator A5071239762 @default.
- W1996403735 date "2014-12-30" @default.
- W1996403735 modified "2023-09-27" @default.
- W1996403735 title "Seeing asymptotic freedom in an exact correlator of a large-Nmatrix field theory" @default.
- W1996403735 cites W1499968416 @default.
- W1996403735 cites W1560118662 @default.
- W1996403735 cites W1674379328 @default.
- W1996403735 cites W1796810754 @default.
- W1996403735 cites W1967999171 @default.
- W1996403735 cites W1969552299 @default.
- W1996403735 cites W1973079440 @default.
- W1996403735 cites W1973601304 @default.
- W1996403735 cites W1984667414 @default.
- W1996403735 cites W1986022323 @default.
- W1996403735 cites W1989001108 @default.
- W1996403735 cites W1994200639 @default.
- W1996403735 cites W2003008637 @default.
- W1996403735 cites W2003750725 @default.
- W1996403735 cites W2011012401 @default.
- W1996403735 cites W2016813357 @default.
- W1996403735 cites W2026653284 @default.
- W1996403735 cites W2033441375 @default.
- W1996403735 cites W2036466157 @default.
- W1996403735 cites W2043941454 @default.
- W1996403735 cites W2049361188 @default.
- W1996403735 cites W2055374620 @default.
- W1996403735 cites W2056037153 @default.
- W1996403735 cites W2066686577 @default.
- W1996403735 cites W2068046593 @default.
- W1996403735 cites W2071644227 @default.
- W1996403735 cites W2083764481 @default.
- W1996403735 cites W2090081354 @default.
- W1996403735 cites W2090153618 @default.
- W1996403735 cites W2090250666 @default.
- W1996403735 cites W2151880873 @default.
- W1996403735 cites W2906328270 @default.
- W1996403735 cites W3099535368 @default.
- W1996403735 cites W3101278528 @default.
- W1996403735 cites W3104662511 @default.
- W1996403735 cites W4237798076 @default.
- W1996403735 cites W4299550612 @default.
- W1996403735 cites W2045499355 @default.
- W1996403735 doi "https://doi.org/10.1103/physrevd.90.125038" @default.
- W1996403735 hasPublicationYear "2014" @default.
- W1996403735 type Work @default.
- W1996403735 sameAs 1996403735 @default.
- W1996403735 citedByCount "6" @default.
- W1996403735 countsByYear W19964037352014 @default.
- W1996403735 countsByYear W19964037352015 @default.
- W1996403735 countsByYear W19964037352016 @default.
- W1996403735 countsByYear W19964037352017 @default.
- W1996403735 countsByYear W19964037352020 @default.
- W1996403735 crossrefType "journal-article" @default.
- W1996403735 hasAuthorship W1996403735A5071239762 @default.
- W1996403735 hasBestOaLocation W19964037352 @default.
- W1996403735 hasConcept C114614502 @default.
- W1996403735 hasConcept C121332964 @default.
- W1996403735 hasConcept C133386390 @default.
- W1996403735 hasConcept C14036430 @default.
- W1996403735 hasConcept C149374227 @default.
- W1996403735 hasConcept C156778621 @default.
- W1996403735 hasConcept C166124518 @default.
- W1996403735 hasConcept C181830111 @default.
- W1996403735 hasConcept C187268509 @default.
- W1996403735 hasConcept C202444582 @default.
- W1996403735 hasConcept C2524010 @default.
- W1996403735 hasConcept C33923547 @default.
- W1996403735 hasConcept C37914503 @default.
- W1996403735 hasConcept C53622274 @default.
- W1996403735 hasConcept C62520636 @default.
- W1996403735 hasConcept C78458016 @default.
- W1996403735 hasConcept C86803240 @default.
- W1996403735 hasConcept C9652623 @default.
- W1996403735 hasConcept C99844830 @default.
- W1996403735 hasConceptScore W1996403735C114614502 @default.
- W1996403735 hasConceptScore W1996403735C121332964 @default.
- W1996403735 hasConceptScore W1996403735C133386390 @default.
- W1996403735 hasConceptScore W1996403735C14036430 @default.
- W1996403735 hasConceptScore W1996403735C149374227 @default.
- W1996403735 hasConceptScore W1996403735C156778621 @default.
- W1996403735 hasConceptScore W1996403735C166124518 @default.
- W1996403735 hasConceptScore W1996403735C181830111 @default.
- W1996403735 hasConceptScore W1996403735C187268509 @default.
- W1996403735 hasConceptScore W1996403735C202444582 @default.
- W1996403735 hasConceptScore W1996403735C2524010 @default.
- W1996403735 hasConceptScore W1996403735C33923547 @default.
- W1996403735 hasConceptScore W1996403735C37914503 @default.
- W1996403735 hasConceptScore W1996403735C53622274 @default.
- W1996403735 hasConceptScore W1996403735C62520636 @default.
- W1996403735 hasConceptScore W1996403735C78458016 @default.
- W1996403735 hasConceptScore W1996403735C86803240 @default.
- W1996403735 hasConceptScore W1996403735C9652623 @default.
- W1996403735 hasConceptScore W1996403735C99844830 @default.
- W1996403735 hasIssue "12" @default.
- W1996403735 hasLocation W19964037351 @default.
- W1996403735 hasLocation W19964037352 @default.
- W1996403735 hasOpenAccess W1996403735 @default.
- W1996403735 hasPrimaryLocation W19964037351 @default.