# Journal of High Energy Physics

Journal of High Energy Physics > 2018 > 2018 > 4 > 1-45

Journal of High Energy Physics > 2018 > 2018 > 4 > 1-28

*S*

^{4}. We study a probe fundamental string in this background which is dual to a supersymmetric Wilson loop in the N=2∗ $$ \mathcal{N}={2}^{\ast } $$ theory. Using holography we calculate...

Journal of High Energy Physics > 2018 > 2018 > 4 > 1-81

*q*

_{T}spectra of gauge bosons (

*γ*

^{∗}, Higgs) in

*pp*collisions in the regime of low (but perturbative) transverse momentum

*q*

_{T}as a specific example. First we introduce a scheme to choose the factorization scale for virtuality in momentum space instead of in impact parameter...

Journal of High Energy Physics > 2018 > 2018 > 4 > 1-43

*q*-body Sachdev-Ye-Kitaev (SYK) model, and obtain order 1

*/N*

^{2}corrections for all moments, where

*N*is the total number of Majorana fermions. To order 1

*/N*, moments are given by those of the weight function of the Q-Hermite polynomials. Representing Wick contractions by rooted chord diagrams, we show that the 1

*/N*

^{2}correction...

Journal of High Energy Physics > 2018 > 2018 > 4 > 1-47

Journal of High Energy Physics > 2018 > 2018 > 4 > 1-58

Journal of High Energy Physics > 2018 > 2018 > 4 > 1-40

Journal of High Energy Physics > 2018 > 2018 > 4 > 1-29

Journal of High Energy Physics > 2018 > 2018 > 4 > 1-15

Journal of High Energy Physics > 2018 > 2018 > 4 > 1-23

Journal of High Energy Physics > 2018 > 2018 > 4 > 1-16

*S*

^{1}fibration leads to D4-branes intersecting with D6-branes. D-braneology shows that there are additional charged chiral fermions from the open strings which stretch between the D4-branes and D6-branes. From the M-theory point of view the appearance of these charged states is mysterious as the...

Journal of High Energy Physics > 2018 > 2018 > 4 > 1-32

*D*= 4, N=2 $$ \mathcal{N}=2 $$ gauged supergravity with an electromagnetic Fayet-Iliopoulos term. We restrict to the uncharged, single dilaton consistent truncation and point out that the bulk Lagrangian is self-dual under electromagnetic duality. Within this truncation, we construct two families of exact hairy black hole solutions, which are asymptotically

*AdS*

_{4}. When a duality...

Journal of High Energy Physics > 2018 > 2018 > 4 > 1-18

*α*′, which are at the core of the FZZ duality, render the region just behind the horizon of the SL(2, ℝ)

_{k}/U(1) black hole singular already at the classical level (

*g*

_{s}= 0). We argue that the 2D

*classical*SL(2, ℝ)

_{k}/U(1) black hole could shed some light on

*quantum*black holes in higher dimensions including large black holes...

Journal of High Energy Physics > 2018 > 2018 > 4 > 1-39

Journal of High Energy Physics > 2018 > 2018 > 4 > 1-54

Journal of High Energy Physics > 2018 > 2018 > 4 > 1-54

_{5}×

*S*

^{5}. Our approach relies entirely on general consistency conditions and maximal supersymmetry. We discuss two related methods, one in position space and the other in Mellin space. The position space method is based on the observation that the holographic...

Journal of High Energy Physics > 2018 > 2018 > 4 > 1-23

Journal of High Energy Physics > 2018 > 2018 > 4 > 1-27

*D*= 5 holographic models we construct boomerang RG flow solutions that start in the UV at an

*AdS*

_{5}vacuum and end up at the same vacuum in the IR. The RG flows are driven by deformations by relevant operators that explicitly break translation invariance. For specific models, such that they admit another

*AdS*

_{5}solution,

*AdS*

_{5}

^{c}, we show that for large enough deformations the RG...

Journal of High Energy Physics > 2018 > 2018 > 4 > 1-23

Journal of High Energy Physics > 2018 > 2018 > 4 > 1-34