# Journal of High Energy Physics

Journal of High Energy Physics > 2019 > 2019 > 5 > 1-12

Journal of High Energy Physics > 2019 > 2019 > 5 > 1-36

Journal of High Energy Physics > 2019 > 2019 > 5 > 1-47

*K*3 ×

*T*

^{2}orbifolded by an order ℤ

_{N}freely acting orbifold

*g*′ including all CHL compactifications...

Journal of High Energy Physics > 2019 > 2019 > 5 > 1-31

Journal of High Energy Physics > 2019 > 2019 > 5 > 1-39

Journal of High Energy Physics > 2019 > 2019 > 5 > 1-33

Journal of High Energy Physics > 2019 > 2019 > 5 > 1-48

Journal of High Energy Physics > 2019 > 2019 > 5 > 1-29

Journal of High Energy Physics > 2019 > 2019 > 5 > 1-28

*AdS*

_{3}

*/CF T*

_{2}. This computation is done perturbatively to second order. We give a general result and discuss some of its properties. As operators generating such conformal transformations can be explicitly constructed in CFT terms, these results allow for a comparison...

Journal of High Energy Physics > 2019 > 2019 > 5 > 1-48

*E*≫

*T*) traveling through a quark-gluon plasma lose energy by splitting via bremsstrahlung and pair production. Regardless of whether or not the quark-gluon plasma itself is strongly coupled, an important question lying at the heart of philosophically different approaches to energy loss is whether the high-energy partons of an in-medium shower can be thought of as a...

Journal of High Energy Physics > 2019 > 2019 > 5 > 1-64

Journal of High Energy Physics > 2019 > 2019 > 5 > 1-37

Journal of High Energy Physics > 2019 > 2019 > 5 > 1-25

Journal of High Energy Physics > 2019 > 2019 > 5 > 1-25

Journal of High Energy Physics > 2019 > 2019 > 5 > 1-29

Journal of High Energy Physics > 2019 > 2019 > 5 > 1-43

Journal of High Energy Physics > 2019 > 2019 > 5 > 1-35

Journal of High Energy Physics > 2019 > 2019 > 5 > 1-25

*b*−

*τ*Yukawa unified Supersymmetric (SUSY) SU(5) GUTs, in which the asymptotic gaugino

*M*

_{1,2,3}masses are generated through the mirage mediated supersymmetry breaking, which is a combination of the gravity and anomaly mediation. Due to the contributions from the anomaly contribution,

*M*

_{3}is always lighter than

*M*

_{1}and

*M*

_{2}, and consequently for the range of asymptotic masses...

Journal of High Energy Physics > 2019 > 2019 > 5 > 1-31

*B*

^{0}→ (

*π*

^{+}

*π*

^{−})(

*K*

^{+}π

^{−}) decays is performed in the two-body invariant mass regions 300

*< m*(

*π*

^{+}

*π*

^{−})

*<*1100 MeV/

*c*

^{2}, accounting for the

*ρ*

^{0},

*ω*,

*f*

_{0}(500),

*f*

_{0}(980) and

*f*

_{0}(1370) resonances, and 750

*< m*(

*K*

^{+}

*π*

^{−})

*<*1200 MeV/

*c*

^{2}, which is dominated by the

*K*

^{*}(892)

^{0}meson. The analysis uses 3 fb

^{−1}of proton-proton collision data collected by the LHCb experiment at centre-of-mass...

Journal of High Energy Physics > 2019 > 2019 > 5 > 1-23