2016/05/09 by Stefan Hohenegger, Amer Iqbal, Soo-Jong Rey
Mathematics · Physics and Astronomy · #Black Holes and Theoretical Physics #Brane #Combinatorics #Cosmology and Gravitation Theories #Duality (order theory) #Geometry #Homogeneous space #Mathematical analysis #Mathematical physics #Mathematics #Moduli space #Nonlinear Waves and Solitons #Partition function (quantum field theory) #Physics #Pure mathematics #Quantum mechanics #Relationship between string theory and quantum field theory #Sigma #Singularity #String (physics) #String duality #hep-th #math.AG
paper · pdf · doi:10.1103/physrevd.94.046006
published as Phys. Rev. D 94, 046006 (2016) · 49 pages, 4 figures
arxiv created 2016/05/09 · openalex publication_date 2016/08/19 · arxiv updated 2016/08/24 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
We study a class of N=(1,0) little string theories obtained from orbifolds of M-brane configurations. These are realized in two different ways that are dual to each other: either as M parallel M5-branes probing a transverse A_N\ensuremath-1 singularity or N M5-branes probing an A_M\ensuremath-1 singularity. These backgrounds can further be dualized into toric, noncompact Calabi-Yau threefolds XN,M which have double elliptic fibrations and thus give a natural geometric description of T-duality of the little string theories. The little string partition functions are captured by the topological string partition function of XN,M. We analyze in detail the free energies \mathrm\ensuremathΣN,M associated with the latter in a special region in the K"ahler moduli space of XN,M and discover a remarkable property: in the Nekrasov-Shatashvili limit, \mathrm\ensuremathΣN,M is identical to NM times \mathrm\ensuremathΣ1,1. This entails that the Bogomol'nyi-Prasad-Sommerfield (BPS) degeneracies for any (N,M) can uniquely be reconstructed from the (N,M)=(1,1) configuration, a property we refer to as self-similarity. Moreover, as \mathrm\ensuremathΣ1,1 is known to display a number of recursive structures, BPS degeneracies of little string configurations for arbitrary (N,M) as well acquire additional symmetries. These symmetries suggest that in this special region the two little string theories described above are self-dual under T-duality.