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A Search for the LHCb Charmed 'Pentaquark' using Photo-Production of \(J/{\psi}\) at Threshold in Hall C at Jefferson Lab
We propose to measure the photo-production cross section of \(J/{\psi}\) near threshold, in search of the recently observed LHCb hidden-charm resonances \(P_c\)(4380) and \(P_c\)(4450) consistent with 'pentaquarks'. The observation of these resonances in photo-production will provide stron...
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Published in: | arXiv.org 2016-09 |
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Main Authors: | , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , |
Format: | Article |
Language: | English |
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Online Access: | Get full text |
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Summary: | We propose to measure the photo-production cross section of \(J/{\psi}\) near threshold, in search of the recently observed LHCb hidden-charm resonances \(P_c\)(4380) and \(P_c\)(4450) consistent with 'pentaquarks'. The observation of these resonances in photo-production will provide strong evidence of the true resonance nature of the LHCb states, distinguishing them from kinematic enhancements. A bremsstrahlung photon beam produced with an 11 GeV electron beam at CEBAF covers the energy range of \(J/{\psi}\) production from the threshold photo-production energy of 8.2 GeV, to an energy beyond the presumed \(P_c\)(4450) resonance. The experiment will be carried out in Hall C at Jefferson Lab using a 50{\mu}A electron beam incident on a 9% copper radiator. The resulting photon beam passes through a 15 cm liquid hydrogen target, producing \(J/{\psi}\) mesons through a diffractive process in the \(t\)-channel, or through a resonant process in the \(s\)- and \(u\)-channel. The decay \(e^+e^-\) pair of the \(J/{\psi}\) will be detected in coincidence using the two high-momentum spectrometers of Hall C. The spectrometer settings have been optimized to distinguish the resonant \(s\)- and \(u\)-channel production from the diffractive \(t\)-channel \(J/{\psi}\) production. The \(s\)- and \(u\)-channel production of the charmed 5-quark resonance dominates the \(t\)-distribution at large \(t\). The momentum and angular resolution of the spectrometers is sufficient to observe a clear resonance enhancement in the total cross section and \(t\)-distribution. We request a total of 11 days of beam time with 9 days to carry the main experiment and 2 days to acquire the needed \(t\)-channel elastic \(J/{\psi}\) production data for a calibration measurement. This calibration measurement in itself will greatly enhance our knowledge of \(t\)-channel elastic \(J/{\psi}\) production near threshold. |
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ISSN: | 2331-8422 |