ﻻ يوجد ملخص باللغة العربية
Neutral meson cross-section and direct photon HBT measurements in high energy pp, pA, and AA collisions rely on either subtracting or dividing out the background underlying the $M_mathrm{inv}$ or $Q_mathrm{inv}$ distributions. In this paper we investigate the photon pair distributions for simulated proton-proton collisions at $sqrt{s}=13~$TeV, and show that the correlated part of the background in $M_mathrm{inv}$ gets poorly described by the conventional event-mixing method implemented in experimental analyses. We show that it fails to describe the background as it gives a qualitatively different shape especially at invariant masses around the $pi^{0}$ and $eta$ meson mass. We show that this is caused by the correlations originating from parton fragmentation, and discuss a new method that attempts to describe the correlated part of the combinatorial background by only pairing photons when the parton ancestors are close in $eta$ and $varphi$.
The collinear factorization framework allows to describe the exclusive photoproduction of a $gamma,rho$ pair in the generalized Bjorken regime in terms of a perturbatively calculable coefficient function and universal generalized parton distributions
We propose and study the photoproduction of a $gamma,rho$ pair with a large invariant mass and a small transverse momentum of the final nucleon, as a way to access generalized parton distributions. In the kinematics of JLab 12-GeV, we demonstrate the feasibility of this measurement.
We investigate top quark pair production near the threshold where the pair invariant mass $M_{tbar{t}}$ approaches $2m_t$, which provides sensitive observables to extract the top quark mass $m_t$. Using the effective field theory methods, we derive a
We compute the leading order (LO) $qgto q gamma$ and next-to-leading order (NLO) $ggto q{bar q} gamma$ contributions to inclusive photon production in proton-proton (p+p) collisions at the LHC. These channels provide the dominant contribution at LO a