2016
DOI: 10.1007/jhep02(2016)170
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Little strings and T-duality

Abstract: We study the 2d N = 4 gauge theory descriptions of little strings on type II NS5-branes. The IIB strings on N NS5-branes are described by the N = (4, 4) gauge theories, whose Higgs branch CFTs on U(N ) instanton moduli spaces are relevant. The IIA strings are described by N = (4, 4)Â N −1 quiver theories, whose Coulomb branch CFTs are relevant. We study new N = (0, 4) quiver gauge theories for the IIA strings, which make it easier to study some infrared observables. In particular, we show that the supersymmetr… Show more

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Cited by 47 publications
(53 citation statements)
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“…As a byproduct, our result also verifies the 5d/6d dualities involving D n singularities, discussed in [26][27][28]. Similar studies on T-duality of LSTs were already made in [25,[29][30][31] for the (2, 0) LSTs and the (1, 0) LSTs found from NS5-branes on A n singularities.…”
Section: Jhep10(2017)045supporting
confidence: 89%
See 1 more Smart Citation
“…As a byproduct, our result also verifies the 5d/6d dualities involving D n singularities, discussed in [26][27][28]. Similar studies on T-duality of LSTs were already made in [25,[29][30][31] for the (2, 0) LSTs and the (1, 0) LSTs found from NS5-branes on A n singularities.…”
Section: Jhep10(2017)045supporting
confidence: 89%
“…Each winding sector has a fixed winding number along the circle, which we interpret as a number of 6d little strings. When the circle radius is taken be large, the Hilbert space of 6d BPS states is factorized into numerous winding sectors being decoupled from one another at low energy regime [25]. Such decoupling occurs as the ground energy gap between distinct winding sectors is proportional to the circle radius R, dominating the momentum excitation proportional to the inverse of the circle radius R −1 .…”
Section: Jhep10(2017)045mentioning
confidence: 99%
“…[14][15][16][17][18]. The equivariant elliptic genus turns out to be equal to the refined topological string partition function of the dual Calabi-Yau threefold [10,14,17,18]. Without these insertions, the elliptic genus diverges which is the case for ϵ 1;2 ↦ 0 and this matches the divergence of the refined topological string partition function for ϵ 1;2 ↦ 0.…”
Section: Introductionmentioning
confidence: 63%
“…The regularized partition function is the equivariant (2,0) elliptic genus with the equivariant action on the instaton moduli spaces being given by lifting ðz 1 ; z 2 Þ ∈ C 2 ↦ ðe iϵ 1 z 1 ; e iϵ 2 z 2 Þ with ϵ 1 , ϵ 2 as the equivariant parameters. [14][15][16][17][18]. The equivariant elliptic genus turns out to be equal to the refined topological string partition function of the dual Calabi-Yau threefold [10,14,17,18].…”
Section: Introductionmentioning
confidence: 97%
“…It is amusing to note that we can also obtain a theory in 4d of A-type class S with no punctures by considering the little string theory [37,38] of the above setup [20] (see also [39]). In this case the toric geometry is doubly periodic and we end up periodically identifying horizontal space as well.…”
Section: Jhep11(2015)123mentioning
confidence: 99%