# Journal of High Energy Physics

Journal of High Energy Physics > 2018 > 2018 > 11 > 1-15

*β*-deformed ABJM theory can be obtained by a TsT transformation of AdS

_{4}×

*ℂ*ℙ

^{3}. We present a supercoset construction of

*ℂ*ℙ

^{3}to obtain this gravity dual theory as a Yang-Baxter deformation. This is done by selecting a convenient combination of Cartan generators in order to get an Abelian

*r*-matrix satisfying the classical Yang-Baxter equation. Our results provide another...

Journal of High Energy Physics > 2018 > 2018 > 11 > 1-12

Journal of High Energy Physics > 2018 > 2018 > 11 > 1-25

Journal of High Energy Physics > 2018 > 2018 > 11 > 1-30

Journal of High Energy Physics > 2018 > 2018 > 11 > 1-25

*d*-dimensional Minkowski space. Depending on the value of the real parameter the system describes either helicity fields or continuous spin fields. Starting with the unified formulation we derive a number of equivalent descriptions including the triplet formulation, Fang-Fronsdal-Labastida...

Journal of High Energy Physics > 2018 > 2018 > 11 > 1-27

*τ*

^{−}→

*π*

^{−}

*π*

^{0}

*ν*

_{τ}decays, that includes the most general interactions between Standard Model fields up to dimension six, assuming left-handed neutrinos. We constrain as much as possible the necessary Standard Model hadronic input using chiral symmetry, dispersion relations, data and asymptotic QCD properties. As a result, we show that it is...

Journal of High Energy Physics > 2018 > 2018 > 11 > 1-36

*viz. Mellin*representation of the conformal blocks. The Mellin space is advantageous over the position space not only in allowing to write expressions agnostic...

Journal of High Energy Physics > 2018 > 2018 > 11 > 1-22

*N*expansion. We identify a (negative energy squared) bound state in its spectrum about the large

*N*conformal background. At the critical point...

Journal of High Energy Physics > 2018 > 2018 > 11 > 1-38

Journal of High Energy Physics > 2018 > 2018 > 11 > 1-52

_{3}×

*S*

^{3}×

*K*3, whereas the other four examples give new counting formulas. Their crucial feature...

Journal of High Energy Physics > 2018 > 2018 > 11 > 1-48

Journal of High Energy Physics > 2018 > 2018 > 11 > 1-44

*W*-annihilation and Pauli interference. Spectator effects originating from dimension-7 four-quark operators are derived. Hadronic matrix elements of four-quark operators are parameterized in a model-independent...

Journal of High Energy Physics > 2018 > 2018 > 11 > 1-39

Journal of High Energy Physics > 2018 > 2018 > 11 > 1-127

*N*), SO(

*N*) and Sp(

*N*) gauge groups. The construction leads to bases for the operators, labelled by Young diagrams and associated group theory data, which have been shown to be orthogonal under the inner product defined by the free field two-point...

Journal of High Energy Physics > 2018 > 2018 > 11 > 1-35

Journal of High Energy Physics > 2018 > 2018 > 11 > 1-24

Journal of High Energy Physics > 2018 > 2018 > 11 > 1-32

*W*/

*Z*bosons can appear in several extensions of the SM. The focus of collider studies for such a scalar is often on its direct production, where the scalar is typically only mildly boosted. The observed

*W*/

*Z*are therefore well-separated, allowing analyses for the scalar resonance in a standard fashion...

Journal of High Energy Physics > 2018 > 2018 > 11 > 1-24

Journal of High Energy Physics > 2018 > 2018 > 11 > 1-23

Journal of High Energy Physics > 2018 > 2018 > 11 > 1-26