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Prompt J/psi production at e^+e^- colliders

Feng Yuan, Cong-Feng Qiao, Kuang-Ta Chao

TL;DR

The study analyzes prompt $J/\psi$ production at $e^+e^-$ colliders within NRQCD, contrasting color-singlet and color-octet mechanisms across energy scales. It finds color-octet channels overwhelmingly dominate singlet contributions, with distinct energy dependences and characteristic $J/\psi$ energy spectra for the two octet processes. The work also discusses strategies to extract color-octet matrix elements from $e^+e^-$ data at different energies, offering cleaner tests of NRQCD than hadroproduction. It highlights potential for precise NRQCD scaling tests and notes the need to incorporate $Z^0$ effects at high energies in future analyses.

Abstract

In this paper, we discuss the prompt j/psi production at e^+e^- colliders via color-singlet and color-octet production mechanisms. The color-singlet production processes include 1) e^+e^- to J/ψgg; 2) e^+e^- to J/ψc\bar{c}; 3) e^+e^- to q \bar q ggJ/ψand e^+e^- to q \bar q gχ_c followed by χ_c to J/ψγ. The color-octet production processes include 1) e^+e^- to J/ψg; 2) e^+e^- to j/psi q\bar q. Of all these production channels, we find that the color-octet contributions dominate over the color-singlet contributions at any energy scales. At low energies (\sqrt{s}< 20 GeV), the dominant channel is e^+e^- to J/ψg whereas at high energies e+e^- to j/psi q\bar q will take the leading part. We also find that the energy spectrum for the color-octet j/psi production in process e^+e^- to j/psi q\bar q is very soft, and the mean energy of the produced j/psi is only about 10 GeV~ 20 GeV even at very high energies (e.g. at 1000 GeV). The extraction of color-octet matrix elements from j/psi production in e^+e^- collisions is also discussed.

Prompt J/psi production at e^+e^- colliders

TL;DR

The study analyzes prompt production at colliders within NRQCD, contrasting color-singlet and color-octet mechanisms across energy scales. It finds color-octet channels overwhelmingly dominate singlet contributions, with distinct energy dependences and characteristic energy spectra for the two octet processes. The work also discusses strategies to extract color-octet matrix elements from data at different energies, offering cleaner tests of NRQCD than hadroproduction. It highlights potential for precise NRQCD scaling tests and notes the need to incorporate effects at high energies in future analyses.

Abstract

In this paper, we discuss the prompt j/psi production at e^+e^- colliders via color-singlet and color-octet production mechanisms. The color-singlet production processes include 1) e^+e^- to J/ψgg; 2) e^+e^- to J/ψc\bar{c}; 3) e^+e^- to q \bar q ggJ/ψand e^+e^- to q \bar q gχ_c followed by χ_c to J/ψγ. The color-octet production processes include 1) e^+e^- to J/ψg; 2) e^+e^- to j/psi q\bar q. Of all these production channels, we find that the color-octet contributions dominate over the color-singlet contributions at any energy scales. At low energies (\sqrt{s}< 20 GeV), the dominant channel is e^+e^- to J/ψg whereas at high energies e+e^- to j/psi q\bar q will take the leading part. We also find that the energy spectrum for the color-octet j/psi production in process e^+e^- to j/psi q\bar q is very soft, and the mean energy of the produced j/psi is only about 10 GeV~ 20 GeV even at very high energies (e.g. at 1000 GeV). The extraction of color-octet matrix elements from j/psi production in e^+e^- collisions is also discussed.

Paper Structure

This paper contains 5 sections, 35 equations.