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Anna Cisek

Publications and source records attributed to Anna Cisek.

23 records · Page 2Linked to original sources

Exclusive photoproduction of charmonia in $γp \to V p$ and $p p \to p V p$ reactions within $k_t$-factorization approach

The amplitude for $γp \to J/ψp$ ($γp \to ψ' p$) is calculated in a pQCD $k_{T}$-factorization approach. The total cross section for this process is calculated for different unintegrated gluon distributions and compared with the HERA data and the data extracted recently by the LHCb collaboration. The amplitude for $γp \to J/ψp$ ($γp \to ψ' p$) is used to predict the cross section for exclusive photoproduction of $J/ψ$ ($ψ'$) meson in proton-proton collisions. Compared to earlier calculations we include both Dirac and Pauli electromagnetic form factors. The effect of Pauli form factor is quantified. Absorption effects are taken into account and their role is discussed in detail. Different differential distributions e.g. in $J/ψ$ ($ψ'$) rapidity and transverse momentum are presented and compared with existing experimental data. The UGDF with nonlinear effects built in better describe recent experimental data of the LHCb collaboration but no definite conclusion on onset of saturation can be drawn. We present our results also for the Tevatron. A good agreement with the CDF experimental data points at the midrapidity for both $J/ψ$ and $ψ'$ is achieved.

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The $γγ\to J/ψJ/ψ$ reaction and the $J/ψJ/ψ$ pair production in exclusive ultraperipheral ultrarelativistic heavy ion collisions

We calculate the cross section for the $γγ\to J/ψJ/ψ$ process. Two mechanisms are considered: box (two-loop) diagrams of the order of $O(α_{em}^2 α_s^2)$ and two-gluon exchange of the order of $O(α_{em}^2 α_s^4)$. The first mechanism is calculated in the heavy-quark non-relativistic approximation while the second case we also include the effects of quantum motion of quarks in the bound state. The box contribution dominates at energies close to the threshold ($W <$ 15 GeV) while the two-gluon mechanism takes over at $W >$ 15 GeV. Including the bound-state wave function effects for the two-gluon exchange mechanism gives a cross section 0.1 - 0.4 pb, substantially smaller than that in the non-relativistic limit (0.4 - 1.6 pb). We also find a strong infrared sensitivity which manifests itself in a rather strong dependence on the mass for the $t$-channel gluons. The elementary cross section is then used in the Equivalent Photon Approximation (EPA) in the impact parameter space to calculate the cross section for $^{208}Pb+^{208}Pb \to ^{208}Pb + J/ψJ/ψ+ ^{208}Pb$ reaction. Distributions in rapidity of the $J/ψJ/ψ$ pair and invariant mass of the pair are shown.

hep-ph↗

Exclusive production of vector mesons in $γp$ and $p p$ collisions

The dominant mechanism for the central exclusive production of vector meson in $p p$ and $p \bar p$ collisions is the $γ$ $I P$ fusion. As a building block for the pp reaction, the amplitude for photoproduction $ γp \to V p $ is calculated in a pQCD $k_{T}$- factorization approach. We will present results for several vector mesons: $ρ$, $ω$, $ϕ$, $J/Ψ$ and $Υ$. The total cross section for diffractive mesons production as a function of energy and photon virtuality is calculated. We will present dependence on the mass of the quark for light mesons. The results for $ γp \to V p $ photoproduction depend on the model of the meson wave function. We compare our results with a HERA data for photon-proton collisions. Finally we turn to pp collisions, and we present distribution in rapidity, transverse momentum of vector mesons and azimuthal angle between outgoing protons for Tevatron and LHC energies. The absorption effects will be discussed.

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Exclusive production of $ω$ meson in proton-proton collisions at high energies

First we calculate cross section for the $γp \to ωp$ reaction from the threshold to very large energies. At low energies the pion exchange is the dominant mechanism. At large energies the experimental cross section can be well described within the $k_{t}$-factorization approach by adjusting light-quark constituent mass. Next we calculate differential distributions for the $p p \to p p ω$ reaction at RHIC, Tevatron and LHC energies for the first time in the literature. We consider photon-pomeron (pomeron-photon), photon-pion (pion-photon) as well as diffractive hadronic bremsstrahlung mechanisms. The latter are included in the meson/reggeon exchange picture with parameters fixed from the known phenomenology. Interesting rapidity distributions are predicted. The hadronic bremsstrahlung contributions dominate at large (forward, backward) rapidities. At small energies the photon-pomeron contribution is negligible compared to the bremsstrahlung contributions. It could be, however, easily identified at large energies at midrapidities. Absorptions effects are included and discussed. Our predictions are ready for verification at RHIC and LHC.

hep-ph↗

Exclusive photoproduction of $ϕ$ meson in $γp \to ϕp$ and $p p \to p ϕp$ reactions

The amplitude for $γp \to ϕp$ is calculated in a pQCD $k_{T}$ - factorization approach. The total cross section for this process is compared with HERA data. Total cross section, as a function of photon-proton energy and photon virtuality, is calculated. We also discuss the ratio of $σ_{L}$ / $σ_{T}$ and the dependence on the mass of the strange quark. The amplitude for $γp \to ϕp$ is used to predict the cross section for exclusive photoproduction of $ϕ$ meson in proton-proton collisions. Absorption effects are included. The results for RHIC, Tevatron and LHC energies are presented.

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