Measurement of the Rate of Muon Capture in Hydrogen Gas and Determination of the Proton's Pseudoscalar Coupling $g_P$
| dc.creator | Andreev, V. A. | |
| dc.creator | Banks, T. I. | |
| dc.creator | Case, T. A. | |
| dc.creator | Chitwood, D. B. | |
| dc.creator | Clayton, S. M. | |
| dc.creator | Crowe, K. M. | |
| dc.creator | Deutsch, J. | |
| dc.creator | Egger, J. | |
| dc.creator | Freedman, S. J. | |
| dc.creator | Ganzha, V. A. | |
| dc.creator | Gorringe, T. | |
| dc.creator | Gray, F. E. | |
| dc.creator | Hertzog, D. W. | |
| dc.creator | Hildebrandt, M. | |
| dc.creator | Kammel, P. | |
| dc.creator | Kiburg, B. | |
| dc.creator | Knaack, S. | |
| dc.creator | Kravtsov, P. A. | |
| dc.creator | Krivshich, A. G. | |
| dc.creator | Lauss, B. | |
| dc.creator | Lynch, K. L. | |
| dc.creator | Maev, E. M. | |
| dc.creator | Maev, O. E. | |
| dc.creator | Mulhauser, F. | |
| dc.creator | Özben, C. S. | |
| dc.creator | Petitjean, C. | |
| dc.creator | Petrov, G. E. | |
| dc.creator | Prieels, R. | |
| dc.creator | Schapkin, G. N. | |
| dc.creator | Semenchuk, G. G. | |
| dc.creator | Soroka, M. A. | |
| dc.creator | Tishchenko, V. | |
| dc.creator | Vasilyev, A. A. | |
| dc.creator | Vorobyov, A. A. | |
| dc.creator | Vznuzdaev, M. E. | |
| dc.creator | Winter, P. | |
| dc.date | 2007-04-16 | |
| dc.date.accessioned | 2026-07-07T10:59:36Z | |
| dc.date.available | 2026-07-07T10:59:36Z | |
| dc.description | The rate of nuclear muon capture by the proton has been measured using a new experimental technique based on a time projection chamber operating in ultra-clean, deuterium-depleted hydrogen gas at 1 MPa pressure. The capture rate was obtained from the difference between the measured $μ^-$ disappearance rate in hydrogen and the world average for the $μ^+$ decay rate. The target's low gas density of 1% compared to liquid hydrogen is key to avoiding uncertainties that arise from the formation of muonic molecules. The capture rate from the hyperfine singlet ground state of the $μp$ atom is measured to be $Λ_S=725.0 \pm 17.4 s^{-1}$, from which the induced pseudoscalar coupling of the nucleon, $g_P(q^2=-0.88 m_μ^2)=7.3 \pm 1.1$, is extracted. This result is consistent with theoretical predictions for $g_P$ that are based on the approximate chiral symmetry of QCD. | |
| dc.description | submitted to Phys.Rev.Lett | |
| dc.identifier | https://arxiv.org/abs/0704.2072 | |
| dc.identifier | http://arxiv.org/abs/0704.2072 | |
| dc.identifier | Phys.Rev.Lett.99:032002,2007 | |
| dc.identifier | doi:10.1103/PhysRevLett.99.032002 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/187457 | |
| dc.subject | Nuclear Experiment | |
| dc.title | Measurement of the Rate of Muon Capture in Hydrogen Gas and Determination of the Proton's Pseudoscalar Coupling $g_P$ | |
| dc.type | text |