# Journal of High Energy Physics

Journal of High Energy Physics > 2018 > 2018 > 6 > 1-70

Journal of High Energy Physics > 2018 > 2018 > 6 > 1-24

_{1}× U(3)

_{−1}ABJM theory and a theory consisting of the product between the (SU(2)

_{3}× SU(2)

_{− 3})/ℤ

_{2}BLG theory and a free N $$ \mathcal{N} $$ = 8 theory of eight real scalars and eight Majorana fermions. As evidence supporting this duality, we show that the moduli spaces, superconformal...

Journal of High Energy Physics > 2018 > 2018 > 6 > 1-57

Journal of High Energy Physics > 2018 > 2018 > 6 > 1-58

Journal of High Energy Physics > 2018 > 2018 > 6 > 1-98

_{3}backgrounds of F-theory and their holographic dual 2d superconformal field theories, which are dimensional reductions of theories with varying coupling. Imposing 2d N=02 $$ \mathcal{N}=\left(0,2\right) $$ supersymmetry,wederivethegeneralconditionsonthegeometryforTypeIIB AdS

_{3}solutions with varying axio-dilaton...

Journal of High Energy Physics > 2018 > 2018 > 6 > 1-32

Journal of High Energy Physics > 2018 > 2018 > 6 > 1-43

*q*= ±1

*,*±2 and no tensor multiplets, anomaly-free models match those models that can be realized from F-theory compactifications almost perfectly. For theories with tensor multiplets or with larger charges, the F-theory constraints are less well...

Journal of High Energy Physics > 2018 > 2018 > 6 > 1-34

*AdS*

_{2}space. More specifically, we consider the ratio of determinants between an operator in the presence of background fields with circular symmetry and the free operator in which the background fields are absent. By Fourier-transforming the angular dependence,...

Journal of High Energy Physics > 2018 > 2018 > 6 > 1-23

Journal of High Energy Physics > 2018 > 2018 > 6 > 1-54

*μτ*and e

*τ*decay modes is presented. The search is based on a data set corresponding to an integrated luminosity of 35.9 fb

^{−1}of proton-proton collisions collected with the CMS detector in 2016, at a centre-of-mass energy of 13 TeV. No significant excess over the standard model expectation is observed. The observed (expected)...

Journal of High Energy Physics > 2018 > 2018 > 6 > 1-27

Journal of High Energy Physics > 2018 > 2018 > 6 > 1-34

*M*

^{N}

*/S*(

*N*) where

*M*is T4 $$ {\mathbb{T}}^4 $$ or

*K*3. In this paper we consider correlation functions involving chiral operators constructed from twist fields: we find explicit expressions for processes involving a twist

*n*operator...

Journal of High Energy Physics > 2018 > 2018 > 6 > 1-16

*a*) improved Wilson fermions with tree-level improved gauge action. Employing a very robust strategy...

Journal of High Energy Physics > 2018 > 2018 > 6 > 1-32

*R*-matrix. We study a new recently proposed approach to construct on-shell Bethe vectors of these models. We prove that the vectors constructed by this method are semi-on-shell Bethe vectors for arbitrary values of Bethe parameters. They thus...

Journal of High Energy Physics > 2018 > 2018 > 6 > 1-35

Journal of High Energy Physics > 2018 > 2018 > 6 > 1-32

Journal of High Energy Physics > 2018 > 2018 > 6 > 1-23

*ξ*-gauge. It is demonstrated that for doing this calculation one should take into account...

Journal of High Energy Physics > 2018 > 2018 > 6 > 1-42

_{4}solutions of IIB string theory where the fields in overlapping patches are glued by elements of the S-duality group. We obtain them by suitable quotients of compact and non-compact geometric solutions. The quotient procedure suggests CFT duals as quiver theories with links involving the so-called

*T*[U(

*N*)] theory. We test the validity of the non-geometric solutions...

Journal of High Energy Physics > 2018 > 2018 > 6 > 1-22

Journal of High Energy Physics > 2018 > 2018 > 6 > 1-30

*C*(

*u*) of the monodromy matrix. In this work we provide a more complete mathematical...