Quantum Phase Transitions in Mass-Deformed ABJM Matrix Model
arXiv:1406.3366 · doi:10.1007/JHEP09(2014)021
Abstract
When mass-deformed ABJM theory is considered on S(3), the partition function of the theory localises and is given by a matrix model. We solve this model at large-N in the decompactification limit, where the radius of the three-sphere is taken to infinity. In this limit, the theory exhibits a rich phase structure with an infinite number of third-order quantum phase transitions accumulating at strong coupling.
25 pages, 9 figures; v2: references added; v3: comment on massless model added
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Cited by in corpus (23)
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- Instanton effects in ABJM theory with general R-charge assignments
- Partition Functions of Superconformal Chern-Simons Theories from Fermi Gas Approach
- N=2* Super-Yang-Mills Theory at Strong Coupling
- Supersymmetric Chern-Simons-matter theory and phase transitions
- Large N behavior of mass deformed ABJM theory
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- N = 2* Phase Transitions and Holography
- Phases of planar 5-dimensional supersymmetric Chern-Simons theory
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- Exact Holography of the Mass-deformed M2-brane Theory
- Phases of five-dimensional supersymmetric gauge theories
- Matrix models for 5d super Yang-Mills
- Mass-deformed ABJM Theory and LLM Geometries: Exact Holography
- Phase transitions and Wilson loops in antisymmetric representations in Chern-Simons-matter theory
- Exact partition function in ABJM theory deformed by mass and Fayet-Iliopoulos terms
- Identification of Bulk coupling constant in Higher Spin/ABJ correspondence
- More Large limits of 3d gauge theories
- Aspects of Massive Gauge Theories on Three Sphere in Infinite Mass Limit
- Duality Cascades and Affine Weyl Groups
- Mass deformed ABJM and symmetry
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- Mass-deformed ABJ and ABJM theory, Meixner-Pollaczek polynomials, and oscillators