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
Abstract: The partition function of N = 6 supersymmetric Chern–Simons-matter theory (known as ABJM t...
We study the quantum mechanical model obtained as a dimensional reduction of Image super Yang–Mills ...
The partition function and expectation values of certain BPS observables of N>=2 Chern-Simons-matter...
When mass-deformed ABJM theory is considered on S-3, the partition function of the theory localises,...
When mass-deformed ABJM theory is considered on S3, the par-tition function of the theory localises,...
When mass-deformed ABJM theory is considered on S(3), the partition function of the theory localises...
When mass-deformed ABJM theory is considered on S 3 , the partition function of the theory localises...
The phase structure of ABJM theory with mass m deformation and non-vanishing Fayet-Iliopoulos (FI) p...
The phase structure of ABJM theory with mass m deformation and non-vanishing Fayet-Iliopoulos (FI) p...
Abstract: We exactly compute the partition function for U(2)k × U(2)− k ABJM theory on S3 deformed b...
The partition function on the three-sphere of many supersymmetric Chern-Simons-matter theories reduc...
Abstract We study phase structure of a three dimensional N $$ \mathcal{N} $$ = 6 superconformal theo...
ABSTRACT: We present quantum phase transitions and critical phenomena at the large-dimension (D) lim...
In this paper we study a phase structure of 5D N=1 super Yang-Mills theory with massive matter multi...
The N=2* theory (mass deformation of the N=4 super-Yang-Mills theory) undergoes an infinite number o...
Abstract: The partition function of N = 6 supersymmetric Chern–Simons-matter theory (known as ABJM t...
We study the quantum mechanical model obtained as a dimensional reduction of Image super Yang–Mills ...
The partition function and expectation values of certain BPS observables of N>=2 Chern-Simons-matter...
When mass-deformed ABJM theory is considered on S-3, the partition function of the theory localises,...
When mass-deformed ABJM theory is considered on S3, the par-tition function of the theory localises,...
When mass-deformed ABJM theory is considered on S(3), the partition function of the theory localises...
When mass-deformed ABJM theory is considered on S 3 , the partition function of the theory localises...
The phase structure of ABJM theory with mass m deformation and non-vanishing Fayet-Iliopoulos (FI) p...
The phase structure of ABJM theory with mass m deformation and non-vanishing Fayet-Iliopoulos (FI) p...
Abstract: We exactly compute the partition function for U(2)k × U(2)− k ABJM theory on S3 deformed b...
The partition function on the three-sphere of many supersymmetric Chern-Simons-matter theories reduc...
Abstract We study phase structure of a three dimensional N $$ \mathcal{N} $$ = 6 superconformal theo...
ABSTRACT: We present quantum phase transitions and critical phenomena at the large-dimension (D) lim...
In this paper we study a phase structure of 5D N=1 super Yang-Mills theory with massive matter multi...
The N=2* theory (mass deformation of the N=4 super-Yang-Mills theory) undergoes an infinite number o...
Abstract: The partition function of N = 6 supersymmetric Chern–Simons-matter theory (known as ABJM t...
We study the quantum mechanical model obtained as a dimensional reduction of Image super Yang–Mills ...
The partition function and expectation values of certain BPS observables of N>=2 Chern-Simons-matter...