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Double charmed meson production at the LHC: Single- versus double-parton scattering mechanism

29 Apr 2014, 16:10
20m
F (BUW)

F

BUW

Oral presentation WG4: QCD and Hadronic Final States WG4: QCD and Hadronic Final States

Speakers

Antoni Szczurek (Institute of Nuclear Physics) Rafal Maciula (Institute of Nuclear Physics PAN)

Description

We compare results of exact calculations of single-parton scattering (SPS) and double-parton scattering (DPS) for production of $c \bar c c \bar c$ and for $D-D$ meson correlations [1]. Each step of DPS is calculated within $k_t$-factorization approach, i.e. effectively including next-to-leading order corrections. The SPS calculations are performed in collinear approximation with exact matrix element for $g g \to c \bar c c \bar c$ subprocess. The new results are compared with results of previous calculation with approximate matrix elements in high-energy approximation. The cross section for the exact calculation is bigger only at small invariant masses and small rapidity difference between two $c$ quarks (or two $\bar c$ antiquarks). We compare correlations in rapidities of two $c$ (or two $\bar c$) for DPS and SPS contributions. Finally we compare our predictions for $DD$ meson pairs with recent results of the LHCb collaboration for invariant mass, rapidity distance between mesons and dimeson invariant mass. The predicted shapes are similar to the measured ones, however, some strength seems to be lacking. Possible missing contribution within the framework of DPS mechanism is suggested. Our new calulations clearly confirm the dominance of DPS in the production of events with double charm. [1] A. van Hameren, R. Maciula and A. Szczurek, arXiv:1402.6972 [hep-ph].

Primary authors

Antoni Szczurek (Institute of Nuclear Physics) Rafal Maciula (Institute of Nuclear Physics PAN)

Presentation materials