Color-octet mechanism in $γ+ p \to J/ψ+ X$

Details Color-octet mechanism in $γ+ p \to J/ψ+ X$ Color-octet mechanism in $γ+ p \to J/ψ+ X$

1996-02-05

arxiv.org/abs/hep-ph/9602223v2

Phys.Rev. D54 (1996) 4312-4325; Erratum-ibid. D60 (1999) 119902

Physics

High Energy Physics

High Energy Physics - Phenomenology

22 pages, with 12 figures(merged into one postscript file), uses eqsecnum.sty, Eqs. (A1)-(A4) are corrected

Scientific paper

10.1103/PhysRevD.54.4312

Photoproduction of $J/\psi$ is considered including the color-octet contributions from the various partial wave states, $^{2S+1}L_J$ = $^1S_0$, $^3S_1$ and $^3P_J$. The production cross section depends on three new nonperturbative parameters defined in NRQCD, called the color-octet matrix elements. Using the color-octet matrix elements determined by fitting the $J/\psi$ production at the Tevatron, we find that the color-octet($c\bar{c}) _{8}({^1S_0}~{\rm and~}~{^3P_J})$ contributions to the $J/\psi$ photoproductions at the fixed target experiments and HERA are too large compared to the data on $\sigma (\gamma + p \to J/\psi +X)$ in the forward direction, the $z$ distribution of $J/\psi$. The $P_T^2$ distribution of $J/\psi$ and the total inelastic $J/\psi$ production rate as a function of $\sqrt{s_ {\gamma p}}$ are predicted including color-octet contributions. We also briefly digress on the $B \to J/\psi + X$ and observe the similar situation. This may be an indication that the color-octet matrix elements determined from the $J/\psi$ production at the Tevatron, especially $<0 | {\cal O}_{8}^{\psi} ({^1S_0}) | 0>$ and $<0 | {\cal O}_{8}^{\psi} ({^3P_J}) | 0>$, might have been overestimated by an order of magnitude.

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