2010
DOI: 10.1143/ptp.124.227
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Five-Dimensional AGT Relation and the Deformed  -Ensemble

Abstract: We discuss an analog of the AGT relation in five dimensions. We define a q-deformation of the β-ensemble which satisfies q-W N constraint. We also show a relation with the Nekrasov partition function of 5D SU(N ) gauge theory with N f = 2N .

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Cited by 122 publications
(149 citation statements)
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“…This corresponds to a composite vertex operator having two parts: the Virasoro part depending onã n and the Heisenberg part depending on the orthogonal linear combination of the oscillators,ā n . This is exactly as prescribed by the AGT relation [175][176][177][178][179][180][181][183][184][185], where the Nekrasov functions for the gauge group U(N ) correspond to the conformal block of the algebra Vir q,t ⊗ Heis q,t .…”
Section: Jhep07(2016)103mentioning
confidence: 85%
See 2 more Smart Citations
“…This corresponds to a composite vertex operator having two parts: the Virasoro part depending onã n and the Heisenberg part depending on the orthogonal linear combination of the oscillators,ā n . This is exactly as prescribed by the AGT relation [175][176][177][178][179][180][181][183][184][185], where the Nekrasov functions for the gauge group U(N ) correspond to the conformal block of the algebra Vir q,t ⊗ Heis q,t .…”
Section: Jhep07(2016)103mentioning
confidence: 85%
“…In fact, one could repeat this matrix model consideration in the deformed case with non-unit q, following the lines of [175][176][177][178][179][180][181]. However, the actual symmetry in this case becomes much larger than the Virasoro algebra: it is the DIM algebra, and we start its general description in the next section.…”
Section: Jhep07(2016)103mentioning
confidence: 99%
See 1 more Smart Citation
“…The spectral dual interpretation of the resulting amplitude is the partition function of a 6d linear quiver gauge theory compactified on a two-dimensional torus. The AGT relations in this case [121][122][123][124][125][126][127][128][129][130][131][132][133][134] give the conformal block of the q-deformed W -algebras on torus, or the spherical conformal block of the affine W -algebra [98,99].…”
Section: Jhep10(2016)047mentioning
confidence: 99%
“…The second famous example comes from the gauge theory: the equivariant cohomology of the instanton moduli spaces (captured by Nakajima quiver varieties [12][13][14] and the corresponding Nekrasov partition functions [15][16][17][18][19][20][21][22]) is acted on by a certain vertex operator algebra, which turns out to be the W N -algebra of two dimensional conformal field theory. This correspondence between the geometric (moduli space) and algebraic (W N -algebra) objects is known as the AGT relation [23][24][25] and has many known implications and generalizations [26][27][28][29][30][31][32][33][34][35][36]. These two examples are in fact directly related to each other and their relation can be understood on both sides of the algebro-geometric correspondence.…”
Section: Introductionmentioning
confidence: 99%