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| 017 | _ | _ | |a This version is available at the following Publisher URL: http://prc.aps.org |
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| 041 | _ | _ | |a eng |
| 082 | _ | _ | |a 530 |
| 084 | _ | _ | |2 WoS |a Physics, Nuclear |
| 100 | 1 | _ | |a Elster, C. |0 P:(DE-Juel1)VDB345 |b 0 |u FZJ |
| 245 | _ | _ | |a Nucleon-nucleon scattering in a three dimensional approach |
| 260 | _ | _ | |a Woodbury, NY |b Inst. |c 2000 |
| 300 | _ | _ | |a 044002-1 |
| 336 | 7 | _ | |a Journal Article |0 PUB:(DE-HGF)16 |2 PUB:(DE-HGF) |
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| 440 | _ | 0 | |a Physical Review C |x 0556-2813 |0 4921 |v 62 |
| 500 | _ | _ | |a Record converted from VDB: 12.11.2012 |
| 520 | _ | _ | |a The nucleon-nucleon (NN) t matrix is calculated directly as function of two vector momenta for different realistic NN potentials. To facilitate this a formalism is developed for solving the two-nucleon Lippmann-Schwinger equation in momentum space without employing a partial wave decomposition. The total spin is heated in a helicity representation. Two different realistic NN interactions, one defined in momentum space and one in coordinate space, are presented in a form suited for this formulation. The angular and momentum dependence of the full amplitude is studied and displayed. A partial wave decomposition of the full amplitude it carried out to compare the presented results with the well-known phase shifts provided by those interactions. |
| 536 | _ | _ | |a Theoretische Kernphysik |c 20.80.0 |2 G:(DE-HGF) |0 G:(DE-Juel1)FUEK39 |x 0 |
| 588 | _ | _ | |a Dataset connected to Web of Science |
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| 700 | 1 | _ | |a Fachruddin, I. |0 P:(DE-HGF)0 |b 1 |
| 700 | 1 | _ | |a Glöckle, W. |0 P:(DE-HGF)0 |b 2 |
| 773 | _ | _ | |g Vol. 62, p. 044002-1 |p 044002-1 |q 62<044002-1 |0 PERI:(DE-600)2844098-5 |t Physical review / C |v 62 |y 2000 |x 0556-2813 |
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| 913 | 1 | _ | |k 20.80.0 |v Theoretische Kernphysik |l Kernphysik |b Struktur der Materie und Materialforschung |0 G:(DE-Juel1)FUEK39 |x 0 |
| 914 | 1 | _ | |y 2000 |
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| 920 | 1 | _ | |k IKP |l Institut für Kernphysik |d 31.12.2000 |g IKP |0 I:(DE-Juel1)VDB301 |x 0 |
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