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      Polarization of Prompt J/psi at the Tevatron

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          Abstract

          The polarization of prompt J/psi at the Fermilab Tevatron is calculated within the nonrelativistic QCD factorization framework. The contribution from radiative decays of P-wave charmonium states decreases, but does not eliminate, the transverse polarization at large transverse momentum. The angular distribution parameter alpha for leptonic decays of the J/\psi is predicted to increase from near 0 at p_T = 5 GeV to about 0.5 at p_T = 20 GeV. The prediction is consistent with measurements by the CDF Collaboration at intermediate values of p_T, but disagrees by about 3 standard deviations at the largest values of p_T measured.

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          Color-Octet Fragmentation and the psi' Surplus at the Tevatron

          , (2009)
          The production rate of prompt \(\psi'\)'s at large transverse momentum at the Tevatron is larger than theoretical expectations by about a factor of 30. As a solution to this puzzle, we suggest that the dominant \(\psi'\) production mechanism is the fragmentation of a gluon into a \(c \bar c\) pair in a pointlike color-octet S-wave state, which subsequently evolves nonperturbatively into a \(\psi'\) plus light hadrons. The contribution to the fragmentation function from this process is enhanced by a short-distance factor of \(1/\alpha_s^2\) relative to the conventional color-singlet contribution. This may compensate for the suppression by \(v^4\), where \(v\) is the relative momentum of the charm quark in the \(\psi'\). If this is indeed the dominant production mechanism at large \(p_T\), then the prompt \(\psi'\)'s that are observed at the Tevatron should almost always be associated with a jet of light hadrons.
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            Color-octet quarkonia production II

            We calculate the lowest order hadronic cross sections for producing colored heavy quark-antiquark pairs in \(L=S=0\) and \(L=S=1\) configurations. Such \(Q\Qbar[{}^1S_0^{(8)}]\) and \(Q\Qbar[{}^3P_J^{(8)}]\) states hadronize into \(\psi_\Q\) quarkonia at the same order in the NRQCD velocity expansion as previously considered \(Q\Qbar[{}^3S_1^{(8)}]\) pairs. Their contributions to prompt Psi and Upsilon production at the Tevatron bring the shapes of theoretical transverse momentum distributions into line with recent CDF measurements. We find that the best fit values for the linear combinations of \(Q\Qbar[{}^1S_0^{(8)}]\) and \(Q\Qbar[{}^3P_J^{(8)}]\) long distance matrix elements which can be extracted from the data are generally consistent with NRQCD scaling rules.
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              Gluon Fragmentation into Heavy Quarkonium

              , (2010)
              The dominant production mechanism for heavy quark-antiquark bound states in very high energy processes is fragmentation, the splitting of a high energy parton into a quarkonium state and other partons. We show that the fragmentation functions \(D(z,\mu)\) describing these processes can be calculated using perturbative QCD. We calculate the fragmentation functions for a gluon to split into S-wave quarkonium states to leading order in the QCD coupling constant. The leading logarithms of \(\mu/m_Q\), where \(\mu\) is the factorization scale and \(m_Q\) is the heavy quark mass, are summed up using Altarelli-Parisi evolution equations.
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                Author and article information

                Journal
                22 November 1999
                2000-07-26
                Article
                10.1103/PhysRevD.62.094005
                hep-ph/9911436
                4b64bb35-f633-473b-b50d-3f31b714ff02
                History
                Custom metadata
                DESY 99-175
                Phys.Rev.D62:094005,2000
                4 pages, 2 figures, one reference added, accepted for publication in Phys. Rev. D
                hep-ph

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