# Journal of High Energy Physics

Journal of High Energy Physics > 2019 > 2019 > 10 > 1-95

*a priori*are not manifest. These modular structures include: mock modular forms, SL(2

*,*ℤ) Weil representations, quantum modular forms, non-semisimple modular tensor categories, and chiral algebras...

Journal of High Energy Physics > 2019 > 2019 > 10 > 1-19

Journal of High Energy Physics > 2019 > 2019 > 10 > 1-42

*priori*coordinate dependent, and may not be well-motivated in full, covariant general relativity; however, the fact that physically...

Journal of High Energy Physics > 2019 > 2019 > 10 > 1-27

*α*

^{′}expansion for the charges of a bound system of heterotic strings, solitonic 5-branes and, optionally, a Kaluza-Klein monopole. The expressions, which differ from those of the zeroth-order supergravity approximation, coincide with the values obtained when only the corrections of quadratic order in curvature are included. Our computation relies...

Journal of High Energy Physics > 2019 > 2019 > 10 > 1-30

*e*

^{+}

*e*

^{−}

*→*ϒ(

*nS*)

*π*

^{+}

*π*

^{−}(

*n*= 1

*,*2

*,*3) cross sections at energies from 10

*.*52 to 11

*.*02 GeV using data collected with the Belle detector at the KEKB asymmetric-energy

*e*

^{+}

*e*

^{−}collider. We observe a new structure in the energy dependence of the cross sections; if described by a Breit-Wigner function its mass and width are found to be M = 10752.7 ± 5.9 − 1.1 +...

Journal of High Energy Physics > 2019 > 2019 > 10 > 1-19

_{3}with a product flavor group of the form U(

*f*)

*×*U(

*F*). We find interesting structures emerge when

*f*+

*F > k*depending on the relative sizes of

*f*,

*F*and

*k*. In particular, there exists phase transitions in which a Grassmannian phase will disappear and reappear in a different part of the phase diagram.

Journal of High Energy Physics > 2019 > 2019 > 10 > 1-59

Journal of High Energy Physics > 2019 > 2019 > 10 > 1-30

*X*extensions of the Standard Model whose quantum anomalies are canceled per generation. Similarly to other versions, the theory consists of a Two-Higgs-Doublet Model plus a scalar singlet embedded into the SM ⊗ U (1)

_{X}gauge group, and introduces small modifications to the

*Z*-boson interactions. These changes can be minimized by exclusively charging...

Journal of High Energy Physics > 2019 > 2019 > 10 > 1-61

^{−1}, representing essentially the full LHC Run 2 data sample. The...

Journal of High Energy Physics > 2019 > 2019 > 10 > 1-49

Journal of High Energy Physics > 2019 > 2019 > 10 > 1-19

Journal of High Energy Physics > 2019 > 2019 > 10 > 1-53

*αs*studies, parton distribution function extractions, and many other applications. Numerous machine learning analyses have attacked the problem, demonstrating that...

Journal of High Energy Physics > 2019 > 2019 > 10 > 1-33

Journal of High Energy Physics > 2019 > 2019 > 10 > 1-38

_{3}or warped AdS

_{3}spacetimes under Dirichlet-Neumann boundary conditions...

Journal of High Energy Physics > 2019 > 2019 > 10 > 1-28

Journal of High Energy Physics > 2019 > 2019 > 10 > 1-31

*ϕ*

_{3}using

*B*

^{±}

*→ D*( K S 0 $$ {K}_{\mathrm{S}}^0 $$

*π*

^{+}

*π*

^{−}

*π*

^{0})

*K*

^{±}decays, where

*D*indicates either a

*D*

^{0}or D ¯ $$ \overline{D} $$

^{0}meson. Measurements of the strong-phase difference of the

*D →*K S 0 $$ {K}_{\mathrm{S}}^0 $$

*π*

^{+}

*π*

^{−}

*π*

^{0}amplitude obtained from CLEO-c data are used as input. This...

Journal of High Energy Physics > 2019 > 2019 > 10 > 1-51

*pp*collisions is measured at a centre-of-mass energy of 13 TeV with the ATLAS detector at the LHC using an integrated luminosity of 36

*.*1 fb

^{−1}. The differential cross section is presented as a function of the photon transverse energy in different regions of photon pseudorapidity. The differential cross section as a function...

Journal of High Energy Physics > 2019 > 2019 > 10 > 1-42

*N*corrections of the index are reproduced by D3-branes wrapped on three particular three-cycles in the internal space Y $$ \mathcal{Y} $$ , the abelian orbifold of

**S**^{5}. We first establish the...

Journal of High Energy Physics > 2019 > 2019 > 10 > 1-25

*O*(1

*/G*). We argue that semiclassical states prepared by a Euclidean path integral have the property that projecting them onto a subspace in which the Ryu-Takayanagi or Hubeny-Rangamani-Takayanagi surface has definite area gives a state with a flat entanglement spectrum at this...

Journal of High Energy Physics > 2019 > 2019 > 10 > 1-35

*S → A*1

*A*2

*Z*

^{t}and two scalar singlets, plus extra matter required to cancel the U(1)

^{t}anomalies...