Results 41 to 50 of about 388 (83)
We present a two-loop calculation of the supersymmetric circular Wilson loop in the N $$ \mathcal{N} $$ = 2* super Yang-Mills theory on the four-sphere. We develop an efficient framework for computing contributing Feynman graphs that relies on using the ...
A. V. Belitsky, G. P. Korchemsky
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Semi-Abelian gauge theories, non-invertible symmetries, and string tensions beyond N-ality
We study a 3d lattice gauge theory with gauge group U(1) N−1 ⋊ S N , which is obtained by gauging the S N global symmetry of a pure U(1) N−1 gauge theory, and we call it the semi-Abelian gauge theory.
Mendel Nguyen +2 more
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A path integral formulation for particle detectors: the Unruh-DeWitt model as a line defect
Particle detectors are an ubiquitous tool for probing quantum fields in the context of relativistic quantum information (RQI). We formulate the Unruh-DeWitt (UDW) particle detector model in terms of the path integral formalism. The formulation is able to
Ivan M. Burbano +2 more
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The crease is a surface operator folded by a finite angle along an infinite line. Several realisations of it in the 6d N $$ \mathcal{N} $$ = (2, 0) theory are studied here. It plays a role similar to the generalised quark-antiquark potential, or the cusp
Nadav Drukker, Maxime Trépanier
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Probing the dynamics of stringy flux tubes with large R-charge
We study the generalized cusp anomalous dimension, or quark-antiquark potential on the three-sphere, in the presence of a large R-charge L and at strong coupling.
Davide Bonomi +4 more
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The planar limit of N $$ \mathcal{N} $$ = 2 superconformal quiver theories
We compute the planar limit of both the free energy and the expectation value of the 1/2 BPS wilson loop for four dimensional N $$ \mathcal{N} $$ = 2 superconformal quiver theories, with a product of SU(N)s as gauge group and hi-fundamental matter ...
Bartomeu Fiol +2 more
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We construct new half-BPS line defects in 3d N = 2 $$ \mathcal{N}=2 $$ supersymmetric quiver gauge theories whose Higgs branches are complete flag manifolds X = Fl(n). Upon circle compactification, the bulk theory flows to a non-linear sigma model (NLSM)
Cyril Closset +5 more
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Solvable models of quantum black holes: a review on Jackiw-Teitelboim gravity. [PDF]
Mertens TG, Turiaci GJ.
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The analytic structure of the fixed charge expansion. [PDF]
Antipin O +3 more
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Schubert line defects in 3d GLSMs. Part II. Partial flag manifolds and parabolic quantum polynomials
We construct Schubert line defects in the 3d N = 2 $$ \mathcal{N}=2 $$ supersymmetric gauged linear sigma model (GLSM) with target space a partial flag manifold X = Fl(k; n), generalizing our construction for complete flag manifolds given in a companion ...
Cyril Closset +5 more
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