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

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 $\sigma (\gamma + p \rightarrow J/\psi +X)$ 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 $B \rightarrow J/\psi + X$ 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 $\langle 0 | {\cal O}_{8}^{\psi} ({^1S_0}) | 0 \rangle$ and $\langle 0 | {\cal O}_{8}^{\psi} ({^3P_J}) | 0 \rangle$, might have been overestimated by an order of magnitude.