2004
DOI: 10.1016/j.nuclphysb.2004.08.029
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Correlators of matrix models on homogeneous spaces

Abstract: We investigate the correlators of T rA µ A ν in matrix models on homogeneous spaces: S 2 and S 2 × S 2 . Their expectation value is a good order parameter to measure the geometry of the space on which non-commutative gauge theory is realized. They also serve as the Wilson lines which carry the minimum momentum. We develop an efficient procedure to calculate them through 1PI diagrams. We determine the large N scaling behavior of the correlators. The order parameter shows that fuzzy S 2 × S 2 acquires a 4 dimens… Show more

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Cited by 13 publications
(29 citation statements)
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“…[35] in the present model, we find that the bosonic contribution and the fermionic contribution cancel each other even at finite N . We also find that à 4 = 0 to all orders in perturbation theory due to parity invariance A 4 → −A 4 .…”
Section: C1 Propagators and The Tadpolesupporting
confidence: 47%
See 1 more Smart Citation
“…[35] in the present model, we find that the bosonic contribution and the fermionic contribution cancel each other even at finite N . We also find that à 4 = 0 to all orders in perturbation theory due to parity invariance A 4 → −A 4 .…”
Section: C1 Propagators and The Tadpolesupporting
confidence: 47%
“…[27][28][29][30][31][32][33][34][35][36][37][38][39]. This provides a matrix description of the so-called Myers effect in string theory [40].…”
Section: Introductionmentioning
confidence: 99%
“…Quantum corrections in gauge theories on these spaces are investigated in [24,25,26,27,28]. The symmetric trace of the operators on a compact space is defined as…”
Section: Wilson Line Correlators In Noncommutative Gauge Theorymentioning
confidence: 99%
“…We list the studies for those based on low dimensional gauge theories: i) dynamical generation of space-times in IIB matrix model [18,19,20], ii) critical phenomena in strongly coupled 1D large-N gauge theories using Gaussian expansion method [21,22], iii) stabilities of fuzzy spaces in IIB matrix model [23,24,25,26,27,28,29], iv) phase structures of low dimensional gauge theories [16,30,31,32,33,34,35,36], v) correspondence between superstring theory and IIB matrix model [37,38,39], vi) phase structures of low dimensional gauge theories by 1/D expansion; [1,40,41], vii) descriptions of black holes in real-time using BFSS matrix model [42,43,44,45], viii) linear responses in D0-branes [46], ix) covariant matrix theory for D-particles [47].…”
Section: Introductionmentioning
confidence: 99%