Little strings and T-duality

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Little strings and T-duality Jungmin Kim (Seoul National University) January 28, 2015 Talk based on [JK., Seok Kim, Kimyeong Lee] in progress.

6d N=(1,1) Little strings Outline NS5-branes in IIB string theory in 10d flat space Supersymmetric index of 6d N=(1,1) Little strings on R4 X T2 2d N=(4,4) ADHM GLSM for N=(1,1) little strings 6d N=(2,0) Little strings NS5-branes in IIA string theory in 10d flat space T-duality between N=(1,1) and N=(2,0) LSTs 2d N=(0,4) quiver gauge theory for N=(2,0) little strings T-duality T-duality between rank N theories T-duality between rank 1 theories

6d N= (1,1) Little string theory NS5-branes in IIB string theory in 10d flat space World-volume theory : 6d N=(1,1) Maximally supersymmetric Yang-Mills. NS5-branes : S-dual of D5-branes with the gauge coupling BPS Degrees of freedom In Coulomb branch, D1-branes : W-bosons Fundamental strings form BPS bound state on NS5s : Instanton strings Instanton action : : Tension of the F1.

Little string theory limit 6d N= (1,1) Little string theory The gauge coupling of the NS5-branes : gs independent limit The gravitational modes are decoupled The perturbative field theory description is totally broken. At this energy scale, Strongly coupled 6d non-gravitational string theory 6d N=(1,1) Little string theory Little strings : Fundamental strings bound to IIB NS5-branes

6d N= (1,1) Little string theory on R 1,4 x S 1 6d N=(1,1) Little string theory on circle Motivation : T-dual to 6d N=(2,0) Little string theory of IIA NS5-branes. T-Duality : KK-momentum Winding number, with Wilson line along the circle : KK-Momenta along the circle are fractionalized : Form the charge space of root space.

6d N= (1,1) Little string theory on R 4 x T 2 Supersymmetric Index for 6d N=(1,1) LST on R 4 X T 2 Global symmetry : Isometry on NS5-branes worldvolume : Isometry on NS5-branes transverse direction : : Winding number of little Strings : Wilson line expectation value counting fractional momentum Result : the elliptic genus of k instanton strings

6d N= (1,1) Little string theory on R 4 x T 2 Gauge theory description of IIB Little strings Worldsheet description : 2d NLSM with the target space of the instanton moduli space As UV-theory : 2d U(k) N=(4,4) ADHM gauged linear sigma model The elliptic genus of k IIB little strings Computed by Jeffrey-Kirwan residues [F.Benini, R.Eager, K. Hori, and Y. Tachikawa]

NS5-branes in IIA string theory World-volume theory : 6d N= (2,0) Little string theory 6d N=(2,0) Non-abelian tensor multiplet with one compact scalar on. Mass scale of In Tensor branch, Self-dual strings D2-branes NS5 F1 BPS bound states limit. 6d N=(2,0) Little string theory T-dual to 6d N=(1,1) Little string theory Little strings : M2-branes wrapping on

6d N= (2,0) Little string theory on R 4 x T 2 T-duality between 6d N=(1,1) and N=(2,0) Little strings. Wilson line in 6d N=(1,1) Separation of NS5s along Winding # of IIB Little strings KK-momentum along Fractional momentum Fractionalized IIA Little strings Winding M2-branes wrapping on Exchange. Obtain M5-branes circle-compactified abelian tensor branch. Fractional IIA Little strings Self-dual strings with type.

6d N= (2,0) Little string theory on R 4 x T 2 Supersymmetric Index for 6d N=(2,0) LST on R 4 X T 2 Result Field theory KK-momentum : Fractional IIA Little strings M2-branes contribution :

6d N= (1,1) Little string theory on R 4 x T 2 Fractional IIA Little strings Self-dual strings on the circle compactified abelian tensor branch Self-dual strings charged under [B.Haghighat, A. Iqbal, C. Kozcaz, G. Lockhart, C. Vafa] 2d N=(0,4) circular quiver gauge theory case The Elliptic genus of IIA Little strings

Rank N Little strings T-duality in Rank N Little string theories 6d N=(1,1) Little string theory 6d N=(2,0) Little string theory T-duality T-duality : Checked to highly nontrivial order of in SU(2) gauge theory, [in progress]

Rank 1 Little strings T-duality for Rank 1 Little string theories 6d N=(1,1) Little string theory 6d N=(2,0) Little string theory T-duality T-duality : Checked to highly nontrivial order of Self-T-duality and Extension of T-duality 2d N=(0,4) quiver gauge theory for rank 1 IIA Little strings Enhanced N=(4,4) GLSM for IIA Little strings = GLSM for IIB Little strings T-duality is extended to Sp(4,Z) duality group, [T.J.Hollowood, A. Iqbal, C. Vafa]

Summary Type II Little string theories share T-duality exchanging KK-momentum and Winding strings with all fractional quantities. There are useful 2d gauge theory descriptions of Little strings world-sheet. For the rank 1 little string theories, T-duality is extended to larger duality symmetry group.