# Journal of High Energy Physics

Journal of High Energy Physics > 2017 > 2017 > 1 > 1-102

*g*, the NS quantization scheme leads to

*g*quantization conditions for the corresponding integrable system. The exact NS quantization conditions enjoy a self S-duality with...

Journal of High Energy Physics > 2017 > 2017 > 1 > 1-31

Journal of High Energy Physics > 2017 > 2017 > 1 > 1-46

*AdS*

_{5}×

*S*

^{5}background. The pre-potential appears as part of the vielbeins, without derivatives. In both subspaces (

*AdS*

_{5}and

*S*

^{5}) we used Poincaré coordinates. We picked one bulk coordinate in

*AdS*

_{5}and one bulk coordinate in

*S*

^{5}to define the space-cone gauge. Such space-cone gauge destroys the bulk Lorentz covariance. However, it still preserves...

Journal of High Energy Physics > 2017 > 2017 > 1 > 1-26

*KLT*) factorization method. The amplitude in the chiral bosonic case is identical to a field theory amplitude corresponding to the spin-2 tachyon, massless gravitational sector and massive spin-2 tardyon states of the spectrum. Chiral type II superstrings...

Journal of High Energy Physics > 2017 > 2017 > 1 > 1-51

Journal of High Energy Physics > 2017 > 2017 > 1 > 1-19

*F*

_{1}and

*F*

_{2}in the large-

*N*

_{c}limit. The analytic results are expressed in terms of Goncharov polylogarithms. This allows for a straightforward numerical evaluation. We also derive series expansions, including power suppressed terms, for three kinematic regions corresponding to small and large invariant...

Journal of High Energy Physics > 2017 > 2017 > 1 > 1-13

*y*

_{N}between the Higgs and...

Journal of High Energy Physics > 2017 > 2017 > 1 > 1-10

*D*= 3 of four maximal-rank super-gravities which preserve minimal supersymmetry in

*D*= 11, 7, 5 and 4. Such “

*curious*” theories were investigated some time ago, and the four-dimensional one corresponds to an N = 1 $$ \mathcal{N}=1 $$ supergravity with 7 chiral multiplets spanning the seven-disk manifold. Recently, this latter theory provided...

Journal of High Energy Physics > 2017 > 2017 > 1 > 1-15

*ℤ*

_{2}cosets to the pure spinor description of the superstring in the

*AdS*

_{5}×

*S*

^{5}background.

Journal of High Energy Physics > 2017 > 2017 > 1 > 1-36

*Z*gauge boson as a concrete example for the intermediary state, we utilize a “merged jet” defined by a large jet size to capture the...

Journal of High Energy Physics > 2017 > 2017 > 1 > 1-33

^{−1}, respectively. The Z bosons are reconstructed from opposite-sign electron...

Journal of High Energy Physics > 2017 > 2017 > 1 > 1-39

*a*

_{μ}and present the complete two-loop result, particularly for the bosonic contribution. We focus on the Aligned 2HDM, which has general Yukawa couplings and contains the type I, II, X, Y models as special cases. The result is expressed with physical parameters: three Higgs boson masses, Yukawa couplings, two mixing angles,...

Journal of High Energy Physics > 2017 > 2017 > 1 > 1-24

*pp*scattering at the LHC at S $$ \sqrt{S} $$ = 14 TeV is considered. We analyze the Drell-Yan structure functions assuming the dominance of a Compton-like emission of a virtual photon from a fast quark scattering off the small

*x*gluons. The color dipole framework is applied to perform quantitatively the twist decomposition of all the Drell-Yan...

Journal of High Energy Physics > 2017 > 2017 > 1 > 1-41

Journal of High Energy Physics > 2017 > 2017 > 1 > 1-24

Journal of High Energy Physics > 2017 > 2017 > 1 > 1-20

*n*

^{2}order. It was conjectured that in the critical regime this model is dual to a higher-spin gauge theory on

*AdS*

_{4}. The

*AdS*/

*CFT*correspondence predicts that the masses of higher-spin fields correspond to the scaling dimensions of the singlet currents in the Gross-Neveu...

Journal of High Energy Physics > 2017 > 2017 > 1 > 1-38

*μ*-parameter is positive, the wino mass is also bounded from above. These constraints relax significantly...

Journal of High Energy Physics > 2017 > 2017 > 1 > 1-30

Journal of High Energy Physics > 2017 > 2017 > 1 > 1-33

Journal of High Energy Physics > 2017 > 2017 > 1 > 1-28

*P N*,

*P V*,

*V N*and

*N N*scattering, where

*P*,

*V*and

*N*denote pseudoscalar, vector and nucleon. Explicit expressions for operators are given for all irreducible representations at lowest two relative momenta. Each hadron has a good helicity...