Precise Measurement of Muon Capture on the Proton
| dc.creator | Kammel, P. | |
| dc.creator | Andreev, V. A. | |
| dc.creator | Balin, D. V. | |
| dc.creator | Carey, R. M. | |
| dc.creator | Case, T. | |
| dc.creator | Chitwood, D. B. | |
| dc.creator | Clayton, S. M. | |
| dc.creator | Crowe, K. M. | |
| dc.creator | Deutsch, J. | |
| dc.creator | Debevec, P. T. | |
| dc.creator | Dick, P. U. | |
| dc.creator | Dijksman, A. | |
| dc.creator | Egger, J. | |
| dc.creator | Fahrni, D. | |
| dc.creator | Fetisov, A. A. | |
| dc.creator | Freedman, S. J. | |
| dc.creator | Ganzha, V. A. | |
| dc.creator | Gartner, B. | |
| dc.creator | Govaerts, J. | |
| dc.creator | Gray, F. E. | |
| dc.creator | Hartmann, F. J. | |
| dc.creator | Herold, W. D. | |
| dc.creator | Hertzog, D. W. | |
| dc.creator | Jatsoura, V. I. | |
| dc.creator | Krivshich, A. G. | |
| dc.creator | Lauss, B. | |
| dc.creator | Maev, E. M. | |
| dc.creator | Maev, O. E. | |
| dc.creator | Markushin, V. E. | |
| dc.creator | Onderwater, C. J. G. | |
| dc.creator | Petitjean, C. | |
| dc.creator | Petrov, G. E. | |
| dc.creator | Polly, C. C. | |
| dc.creator | Prieels, R. | |
| dc.creator | Sadetsky, S. M. | |
| dc.creator | Schapkin, G. N. | |
| dc.creator | Schmidt, R. | |
| dc.creator | Semenchuk, G. G. | |
| dc.creator | Soroka, M. | |
| dc.creator | Vorobyov, A. A. | |
| dc.creator | Voropaev, N. I. | |
| dc.date | 2002-02-12 | |
| dc.date.accessioned | 2026-07-07T05:36:53Z | |
| dc.date.available | 2026-07-07T05:36:53Z | |
| dc.description | The aim of the MuCap experiment is a 1% measurement of the singlet capture rate Lambda_S for the basic electro-weak reaction mu + p -> n + nu_mu. This observable is sensitive to the weak form-factors of the nucleon, in particular to the induced pseudoscalar coupling constant g_P. It will provide a rigorous test of theoretical predictions based on the Standard Model and effective theories of QCD. The present method is based on high precision lifetime measurements of mu^- in hydrogen gas and the comparison with the free mu^+ lifetime. The mu^- experiment will be performed in ultra-clean, deuterium-depleted H_2 gas at 10 bar. Low density compared to liquid H_2 is chosen to avoid uncertainties due to ppmu formation. A time projection chamber acts as a pure hydrogen active target. It defines the muon stop position in 3-D and detects rare background reactions. Decay electrons are tracked in cylindrical wire-chambers and a scintillator array covering 75% of 4 pi. | |
| dc.description | Int. RIKEN Conf. on Muon Catalyzed Fusion and Related Exotic Atoms, April 2001, Shimoda, Japan, to be published in Hyperfine Interactions | |
| dc.identifier | https://arxiv.org/abs/nucl-ex/0202011 | |
| dc.identifier | http://arxiv.org/abs/nucl-ex/0202011 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/81142 | |
| dc.subject | Nuclear Experiment | |
| dc.title | Precise Measurement of Muon Capture on the Proton | |
| dc.type | text |