Abstract
We calculate the production of pairs of $\chi_c(J)$ mesons with all possible combinations of $J=0,1,2$. The leading order production mechanism is the crossed-channel gluon exchange in the gluon-gluon fusion reaction. The building blocks are the vertices $g^* g^* \to \chi_c(J)$ for off shell gluons. We stick to the color-singlet model and calculate the gluon fusion vertices in the limit of heavy quarks with nonrelativistic motion in the bound state. These vertices are used to construct the $g^* g^* \to \chi_c(J_1) \chi_c(J_2)$ amplitudes. We then calculate hadron-level cross sections using the $k_T$-factorization approach. In our numerical predictions, we use the KMR-type unintegrated gluon distributions. Several differential distributions at the $pp$ center of mass energy $\sqrt{s} = 8 \, {\rm TeV}$ are shown. The salient feature of the $t$ and $u$-channel gluon exchange are the broad distributions in rapidity difference $\Delta y$ between $\chi_c$ mesons.
Highlights
Cross sections for the production of J=ψ-pairs were measured at the Tevatron [1] and the LHC [2,3,4,5]
For reference we show some distributions for production of χcJ1 χcJ2 pairs in double parton scattering
It is an open issue at the moment whether this points to a nonuniversality of σeff or whether there are additional single parton scattering mechanisms which can alleviate the tension
Summary
Cross sections for the production of J=ψ-pairs were measured at the Tevatron [1] and the LHC [2,3,4,5]. From the many diagrams which can contribute to the χ-pair production, we single out the gauge invariant subset which contains the crossed-channel gluon exchange. Due to the vector exchange, the Feynman amplitude will be ∝ s, which leads to cross sections which are flat at large s This implies broad distributions in the rapidity distance Δy between the produced χc-mesons. There has been recently a calculation for χcχb production [24] using collinear gluon distributions Notice that in the latter case, within the color-singlet model the gluon exchange mechanism is even the exact leading order in this channel. The χcJ1χcJ2 cross section is calculated within the kT-factorization approach including off-shell matrix elements for the gÃgà → χcJ1 χcJ2 subprocess and modern unintegrated gluon distributions. The longitudinal momentum fractions x1 apndffiffiffixffiffiffi2ffiffiffiaffiffirffiffieffiffifficffiffiffialculated from χc’s transverse masses mTi 1⁄4 M2 þ p⃗ 2iT and rapidities y1;2 of mesons in the pp center-of-mass: x1
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