Single-Pion Production in pp Collisions at 0.95 GeV/c (II)
| dc.creator | El-Samad, S. Abd | |
| dc.creator | Bilger, R. | |
| dc.creator | Brinkmann, K. Th. | |
| dc.creator | Clement, H. | |
| dc.creator | Dietrich, M. | |
| dc.creator | Doroshkevich, E. | |
| dc.creator | Dshemuchadse, S. | |
| dc.creator | Ehrhardt, K. | |
| dc.creator | Erhardt, A. | |
| dc.creator | Eyrich, W. | |
| dc.creator | Filippi, A. | |
| dc.creator | Freiesleben, H. | |
| dc.creator | Fritsch, M. | |
| dc.creator | Geyer, R. | |
| dc.creator | Gillitzer, A. | |
| dc.creator | Hauffe, J. | |
| dc.creator | Hesselbarth, D. | |
| dc.creator | Jaekel, R. | |
| dc.creator | Jakob, B. | |
| dc.creator | Karsch, L. | |
| dc.creator | Kilian, K. | |
| dc.creator | Kress, J. | |
| dc.creator | Kuhlmann, E. | |
| dc.creator | Marcello, S. | |
| dc.creator | Marwinski, S. | |
| dc.creator | Meier, R. | |
| dc.creator | Moeller, K. | |
| dc.creator | Morsch, H. P. | |
| dc.creator | Naumann, L. | |
| dc.creator | Ritman, J. | |
| dc.creator | Roderburg, E. | |
| dc.creator | Schoenmeier, P. | |
| dc.creator | Schulte-Wissermann, M. | |
| dc.creator | Schroeder, W. | |
| dc.creator | Stinzing, F. | |
| dc.creator | Sun, G. Y. | |
| dc.creator | Waechter, J. | |
| dc.creator | Wagner, G. J. | |
| dc.creator | Wagner, M. | |
| dc.creator | Weidlich, U. | |
| dc.creator | Wilms, A. | |
| dc.creator | Wirth, S. | |
| dc.creator | Zhang, G. | |
| dc.creator | Zupranski, P. | |
| dc.date | 2008-07-08 | |
| dc.date | 2009-01-15 | |
| dc.date.accessioned | 2026-07-07T13:04:37Z | |
| dc.date.available | 2026-07-07T13:04:37Z | |
| dc.description | The single-pion production reactions $pp\to dπ^+$, $pp\to npπ^+$ and $pp\to ppπ^0$ were measured at a beam momentum of 0.95 GeV/c ($T_p \approx$ 400 MeV) using the short version of the COSY-TOF spectrometer. The central calorimeter provided particle identification, energy determination and neutron detection in addition to time-of-flight and angle measurements from other detector parts. Thus all pion production channels were recorded with 1-4 overconstraints. Main emphasis is put on the presentation and discussion of the $npπ^+$ channel, since the results on the other channels have already been published previously. The total and differential cross sections obtained are compared to theoretical calculations. In contrast to the $ppπ^0$ channel we find in the $npπ^+$ channel a strong influence of the $Δ$ excitation already at this energy close to threshold. In particular we find a $(3 cos^2Θ+ 1)$ dependence in the pion angular distribution, typical for a pure s-channel $Δ$ excitation and identical to that observed in the $dπ^+$ channel. Since the latter is understood by a s-channel resonance in the $^1D_2$ $pn$ partial wave, we discuss an analogous scenario for the $pnπ^+$ channel. | |
| dc.identifier | https://arxiv.org/abs/0807.1189 | |
| dc.identifier | http://arxiv.org/abs/0807.1189 | |
| dc.identifier | Eur.Phys.J.A39:281-289,2009 | |
| dc.identifier | doi:10.1140/epja/i2008-10721-4 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/227226 | |
| dc.subject | Nuclear Experiment | |
| dc.title | Single-Pion Production in pp Collisions at 0.95 GeV/c (II) | |
| dc.type | text |