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| 024 | 7 | _ | |a 10.1140/epja/i2008-10721-4 |2 DOI |
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| 024 | 7 | _ | |a arXiv:0807.1189 |c nucl-ex |2 arXiv |
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| 024 | 7 | _ | |a 2128/10455 |2 Handle |
| 035 | _ | _ | |9 arXiv |a arXiv:0807.1189 |c nucl-ex |
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| 035 | _ | _ | |9 DESY |z D08-06624 |
| 035 | _ | _ | |9 SPIRESTeX |z ElSamad:2008yf |
| 037 | _ | _ | |a PreJuSER-8500 |
| 041 | _ | _ | |a eng |
| 082 | _ | _ | |a 530 |
| 084 | _ | _ | |2 WoS |a Physics, Nuclear |
| 084 | _ | _ | |2 WoS |a Physics, Particles & Fields |
| 084 | _ | _ | |2 PACS |a 13.75.Cs |
| 084 | _ | _ | |2 PACS |a 14.20.Gk |
| 084 | _ | _ | |2 PACS |a 14.20.Pt |
| 084 | _ | _ | |2 PACS |a 25.10.+s |
| 100 | 1 | _ | |0 P:(DE-HGF)0 |a Abdel-Samad, S. |b 0 |
| 245 | _ | _ | |a Single-pion production in pp collisions at 0.95 GeV/c (II) |
| 260 | _ | _ | |a Berlin |b Springer |c 2009 |
| 300 | _ | _ | |a 281 - 289 |
| 336 | 7 | _ | |a Journal Article |0 PUB:(DE-HGF)16 |2 PUB:(DE-HGF) |
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| 440 | _ | 0 | |0 1981 |a European Physical Journal A |v 39 |x 1434-6001 |y 3 |
| 500 | _ | _ | |a This work has been supported by BMBF, DFG (Europ. Graduiertenkolleg 683) and COSY-FFE. We acknowledge valuable discussions with R. A. Arndt, L. Alvarez-Ruso, D. Bugg, C. Hanhart, M. Kaskulov, V. Kukulin, E. Oset, I. Strakovsky, W. Weise and C. Wilkin. |
| 520 | _ | _ | |a The single-pion production reactions pp -> d pi(+), pp -> np pi(+) and pp -> pp pi(0) were measured at a beam momentum of 0.95 GeV/c (T-p approximate to 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. The main emphasis is put on the presentation and discussion of the npp+ 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 pp pi(0) channel we observe in the np pi(+) channel a strong influence of the Delta excitation. In particular, the pion angular distribution exhibits a (3cos(2) circle minus + 1)-dependence, typical for a pure s-channel Delta excitation and identical to that observed in the dp+ channel. Since the latter is understood by a s-channel resonance in the D-1(2) pn partial wave, we discuss an analogous scenario for the pn pi(+) channel. |
| 536 | _ | _ | |0 G:(DE-Juel1)FUEK413 |2 G:(DE-HGF) |a Physik der Hadronen und Kerne |c P53 |x 0 |
| 588 | _ | _ | |a Dataset connected to Web of Science |
| 650 | _ | 7 | |2 INSPIRE |a p p: exclusive reaction |
| 650 | _ | 7 | |2 INSPIRE |a pi+: hadroproduction |
| 650 | _ | 7 | |2 INSPIRE |a pi0: hadroproduction |
| 650 | _ | 7 | |2 INSPIRE |a cross section: energy dependence |
| 650 | _ | 7 | |2 INSPIRE |a p: angular distribution |
| 650 | _ | 7 | |2 INSPIRE |a Delta(1232) |
| 650 | _ | 7 | |2 INSPIRE |a impulse approximation: plane wave |
| 650 | _ | 7 | |2 INSPIRE |a spectrometer: time-of-flight |
| 650 | _ | 7 | |2 INSPIRE |a experimental results |
| 650 | _ | 7 | |2 INSPIRE |a Juelich COSY PS |
| 650 | _ | 7 | |2 INSPIRE |a p p --> 2 nucleon pi |
| 650 | _ | 7 | |2 INSPIRE |a p p --> deuteron pi+ |
| 650 | _ | 7 | |2 INSPIRE |a 0.95 GeV/c |
| 700 | 1 | _ | |0 P:(DE-HGF)0 |a Bilger, R. |b 1 |
| 700 | 1 | _ | |0 P:(DE-HGF)0 |a Brinkmann, K. |b 2 |
| 700 | 1 | _ | |0 P:(DE-Juel1)VDB73156 |a et, al |b 3 |u FZJ |
| 773 | _ | _ | |0 PERI:(DE-600)1459066-9 |a 10.1140/epja/i2008-10721-4 |g Vol. 39, p. 281 - 289 |p 281 - 289 |q 39<281 - 289 |t The @European physical journal / A |v 39 |x 1434-6001 |y 2009 |
| 856 | 7 | _ | |u http://dx.doi.org/10.1140/epja/i2008-10721-4 |
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