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In the paper, the inclusive production of heavy quarkonium $eta_Q$ ($Q=b$ or $c$) via $Z$ boson decays within the framework of nonrelativistic QCD (NRQCD) effective theory are studied. The contributions from the leading color-singlet and color-octet Fock states are considered. Total and differential decay widths for the inclusive decays $Z to eta_c+X$ and $Z to eta_b+X$ are presented. It is found that the decay $Zto eta_Q +X$ is dominated by the $^3S_1^{[8]}$ component, so the decays can be inversely adopted to determine the values of the long-distance matrix elements $langle {cal O}^{eta_{c}}(^{3}S_{1}^{[8]})rangle$ and $langle {cal O}^{eta_{b}}(^{3}S_{1}^{[8]})rangle$ respectively. The numerical results show that at an $e^+e^-$ collider running at the $Z$ pole with a high luminosity around $10^{35}{rm cm}^{-2}{rm s}^{-1}$ (a super $Z$ factory), there are about $4.5times 10^7$ $eta_c$ meson events and $6.2times 10^5$ $eta_b$ meson events to be produced per operation year, and the inclusive decays may be used for clarifying some problems on the heavy quarkonium $eta_Q$ and NRQCD.
We compute the color-singlet and color-octet nonrelativistic QCD (NRQCD) long-distance matrix elements for inclusive production of $P$-wave quarkonia in the framework of potential NRQCD. In this way, the color-octet NRQCD long-distance matrix element
We consider a different power counting in potential NRQCD by incorporating the static potential exactly in the leading order Hamiltonian. We compute the leading relativistic corrections to the inclusive electromagnetic decay ratios in this new scheme
We study the $eta_c$ photoproduction in $ep$ collisions in this paper. The short-distance coefficients for $cbar{c}(^1S_0^{[1]})$, $cbar{c}(^1S_0^{[8]})$, $cbar{c}(^3S_1^{[8]})$, and $cbar{c}(^1P_1^{[8]})$ photoproductions are evaluated at leading or
The near threshold photo or electroproduction of heavy vector quarkonium off the proton is studied in quantum chromodynamics. Similar to the high-energy limit, the production amplitude can be factorized in terms of gluonic Generalized Parton Distribu
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