# Journal of High Energy Physics

Journal of High Energy Physics > 2015 > 2015 > 2 > 1-12

*θ*

_{23}may not be maximal (45°). Two nearly degenerate solutions are possible, one in the lower octant (LO) where

*θ*

_{23}< 45°, and one in the higher octant (HO) where

*θ*

_{23}> 45°. Long baseline experiments measuring the...

Journal of High Energy Physics > 2015 > 2015 > 2 > 1-31

*e*

^{+}

*e*

^{−}collider commissioned as a Higgs factory. We perform a detailed analysis of such potential of a collider operating at 250 − 300 GeV. Mostly using higher dimensional operators in a gauge-invariant framework, we show that...

Journal of High Energy Physics > 2015 > 2015 > 2 > 1-51

Journal of High Energy Physics > 2015 > 2015 > 2 > 1-16

Journal of High Energy Physics > 2015 > 2015 > 2 > 1-21

*T*

_{ n }theories. The conjecture is motivated by making manifest the critical affine module structure in...

Journal of High Energy Physics > 2015 > 2015 > 2 > 1-27

*W*

^{+}

*W*

^{−}production is one of the golden channels for testing the Standard Model as well for searches beyond the Standard Model. We discuss many new subleading processes for inclusive production of

*W*

^{+}

*W*

^{−}pairs generally not included in the literature so far. We focus on photon-photon induced processes. We include elastic-elastic,...

Journal of High Energy Physics > 2015 > 2015 > 2 > 1-28

Journal of High Energy Physics > 2015 > 2015 > 2 > 1-31

Journal of High Energy Physics > 2015 > 2015 > 2 > 1-68

Journal of High Energy Physics > 2015 > 2015 > 2 > 1-48

*A*

_{ N − 1 }Toda CFT and the connection to supersymmetric loop operators in N = 2 $$ \mathcal{N}=2 $$ theories of class S $$ \mathcal{S} $$ on a four-sphere. Correlation functions in the presence of topological defect networks are computed by exploiting the monodromy...

Journal of High Energy Physics > 2015 > 2015 > 2 > 1-44

Journal of High Energy Physics > 2015 > 2015 > 2 > 1-51

_{4}of disjoint spatial domains in the boundary which are delimited by smooth closed curves. A numerical method which approximates a local minimum of the area functional through triangulated surfaces is employed. After some checks of the method against existing analytic results for the holographic entanglement entropy, we compute the holographic...

Journal of High Energy Physics > 2015 > 2015 > 2 > 1-27

Journal of High Energy Physics > 2015 > 2015 > 2 > 1-30

Journal of High Energy Physics > 2015 > 2015 > 2 > 1-62

*q*-form global symmetry is a global symmetry for which the charged operators are of space-time dimension

*q*; e.g. Wilson lines, surface defects, etc., and the charged excitations have

*q*spatial dimensions; e.g. strings, membranes, etc. Many of the properties of ordinary global symmetries (

*q*= 0) apply here. They lead to Ward identities...

Journal of High Energy Physics > 2015 > 2015 > 2 > 1-13

Journal of High Energy Physics > 2015 > 2015 > 2 > 1-17

*B*

^{+}→

*K*

^{+}

*ll*) decay and the CMS analysis in the context of right handed

*W*-boson (

*W*

_{ R }) search show a 2

*.*6

*σ*and a 2

*.*8

*σ*deviations from the Standard Model expectations respectively. In...

Journal of High Energy Physics > 2015 > 2015 > 2 > 1-22

Journal of High Energy Physics > 2015 > 2015 > 2 > 1-22

*C*

_{1}

^{1}+

*A*) in the curved background are explicitly solved by the super Poisson-Lie T-duality. To find the solution of the flat model we use the transformation of supercoordinates, transforming the metric into a constant one, which is shown to be a supercanonical transformation. Then, using the super...

Journal of High Energy Physics > 2015 > 2015 > 2 > 1-22