We study vacuum expectation values (VEVs) of circular half BPS Wilson loops in arbitrary representations in ABJM theory. We find that those in hook representations are reduced to elementary integrations thanks to the Fermi gas formalism, which are accessible from the numerical studies similar to the partition function in the previous studies. For non-hook representations, we show that the VEVs in the grand canonical formalism can be exactly expressed as determinants of those in the hook representations. Using these facts, we can study the instanton effects of the VEVs in various representations. Our results are consistent with the worldsheet instanton effects studied from the topological string and a prescription to include the membrane ins...
We study the Fermi gas quantum mechanics associated to the ABJM matrix model. We develop a method to...
arXiv The partition function of the ABJM theory receives non-perturbative corrections due to instant...
As holographic description of BPS Wilson loops in N = 3 $$ \mathcal{N}=3 $$ flavored ABJM theory wit...
We study vacuum expectation values (VEVs) of circular half BPS Wilson loops in arbitrary representat...
We study vacuum expectation values (VEVs) of circular half BPS Wilson loops in arbitrary representat...
We study instanton corrections to the vacuum expectation value (VEV) of 1/6 BPS Wilson loops in ABJM...
We present a new Fermi gas formalism for the ABJ matrix model. This formulation identifies the effec...
We study 1/2 BPS Wilson loops in 3d N = 4 U(N) Yang-Mills theory with one adjoint and N-f fundamenta...
The matrix model of the ABJM theory can be formulated in terms of an ideal Fermi gas with a non-triv...
The partition function of the ABJM theory receives non-perturbative corrections due to instanton eff...
We compute the exact vacuum expectation value of 1/2 BPS circular Wilson loops of $ \mathcal{N} $ = ...
We investigate the exact results for circular 1/4 and 1/2 BPS Wilson loops in the d = 3 N = 4 super ...
We study the instanton effects of the ABJM partition function using the Fermi gas formalism. We comp...
Recently, Kapustin, Willett and Yaakov have found, by using localization techniques, that vacuum exp...
We study the partition function of the ABJ theory, which is the N = 6 superconformal Chern-Simons ma...
We study the Fermi gas quantum mechanics associated to the ABJM matrix model. We develop a method to...
arXiv The partition function of the ABJM theory receives non-perturbative corrections due to instant...
As holographic description of BPS Wilson loops in N = 3 $$ \mathcal{N}=3 $$ flavored ABJM theory wit...
We study vacuum expectation values (VEVs) of circular half BPS Wilson loops in arbitrary representat...
We study vacuum expectation values (VEVs) of circular half BPS Wilson loops in arbitrary representat...
We study instanton corrections to the vacuum expectation value (VEV) of 1/6 BPS Wilson loops in ABJM...
We present a new Fermi gas formalism for the ABJ matrix model. This formulation identifies the effec...
We study 1/2 BPS Wilson loops in 3d N = 4 U(N) Yang-Mills theory with one adjoint and N-f fundamenta...
The matrix model of the ABJM theory can be formulated in terms of an ideal Fermi gas with a non-triv...
The partition function of the ABJM theory receives non-perturbative corrections due to instanton eff...
We compute the exact vacuum expectation value of 1/2 BPS circular Wilson loops of $ \mathcal{N} $ = ...
We investigate the exact results for circular 1/4 and 1/2 BPS Wilson loops in the d = 3 N = 4 super ...
We study the instanton effects of the ABJM partition function using the Fermi gas formalism. We comp...
Recently, Kapustin, Willett and Yaakov have found, by using localization techniques, that vacuum exp...
We study the partition function of the ABJ theory, which is the N = 6 superconformal Chern-Simons ma...
We study the Fermi gas quantum mechanics associated to the ABJM matrix model. We develop a method to...
arXiv The partition function of the ABJM theory receives non-perturbative corrections due to instant...
As holographic description of BPS Wilson loops in N = 3 $$ \mathcal{N}=3 $$ flavored ABJM theory wit...