ABJM Theory with mass and FI deformations and Quantum Phase Transitions
arXiv:1502.06828 · doi:10.1007/JHEP05(2015)064
Abstract
The phase structure of ABJM theory with mass deformation and non-vanishing Fayet-Iliopoulos (FI) parameter, , is studied through the use of localisation on . The partition function of the theory then reduces to a matrix integral, which, in the large limit and at large sphere radius, is exactly computed by a saddle-point approximation. When the couplings are analytically continued to real values, the phase diagram of the model becomes immensely rich, with an infinite series of third-order phase transitions at vanishing FI-parameter. As the FI term is introduced, new effects appear. For any given , the number of phases is finite and for the theory does not have any phase transitions at all. Finally, we argue that ABJM theory with physical couplings does not undergo phase transitions and investigate the case of gauge group in detail by an explicit calculation of the partition function.
42 pages, 7 figures. Minor revisions of eq. (19) and section 6.2.2 to agree with JHEP-version
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Cited by in corpus (20)
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- Phase transitions and Wilson loops in antisymmetric representations in Chern-Simons-matter theory
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- Mordell integrals and Giveon-Kutasov duality
- More Large limits of 3d gauge theories
- Non-topological Vortex Configurations in the ABJM Model
- Aspects of Massive Gauge Theories on Three Sphere in Infinite Mass Limit
- Duality Cascades and Affine Weyl Groups
- BPS Wilson loops in mass-deformed ABJM theory: Fermi gas expansions and new defect CFT data
- Mass deformed ABJM and symmetry
- Mass-deformed ABJ and ABJM theory, Meixner-Pollaczek polynomials, and oscillators
- Dualities and loops on squashed