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Double parton interactions in $\gamma p, \gamma A$ collisions in the direct photon kinematics

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arxiv 1410.5064 v1 pith:WAG5TIIZ submitted 2014-10-19 hep-ph hep-exnucl-th

classification hep-phhep-exnucl-th
keywords collisionspartoncasecdotdoubleeventsgammainteractions
verification ladder T0 review T1 audit T2 compute T3 formal
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abstract

We derive expressions for the differential distributions and the total cross section of double- parton interaction in direct photon interaction with proton and nuclei. We demonstrate that in this case the cross section is more directly related to the nucleon generalized parton distribution than in the case of double parton interactions in the proton - proton collisions. We focus on the production of two dijets each containing charm (anticharm) quarks and carrying $x_1,x_2>0.2$ fractions of the photon momentum. Numerical results are presented for the case of $\gamma p$ collisions at LHeC, HERA and in the ultraperipheral $AA$ and $pA$ collisions at the LHC. We find that the events of this kind would be abundantly produced at the LHeC. For $\sqrt{s}=1.3$ TeV the expected rate is $2\cdot 10^8$ events for the luminosity $10^{34}$ cm$^{-2}s^{-1}$, the running time of $10^6$ s and the transverse cutoff of $p_t>5$ GeV. This would make it feasible to use these processes for the model independent determination of two parton GPDs in nucleon and in nuclei. For HERA the total accumulated number of the events is also high, but efficiency of the detection of charm seems too low to study the process. We also find that a significant number of such double parton interactions should be produced in $p - Pb$ and $Pb- Pb$ collisions at the LHC: $\sim 6\cdot 10^4$ for $Pb-Pb$, and $\sim 7 \cdot 10^3$ for $p-Pb$ collisions for the same transverse momentum cutoff.

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  1. Direct versus resolved photons in DPS in photoproduction on proton and nuclei

    hep-ph 2026-08 conditional novelty 6.0 of 10

    In photoproduction double parton scattering, the 1⊗2 parton-splitting mechanism boosts resolved-photon cross sections by up to a factor 1.6, and direct photons dominate charm final states for x_γ above 0.3-0.4.

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