000028823 001__ 28823 000028823 005__ 20230217124255.0 000028823 017__ $$aThis version is available at the following Publisher URL: http://prc.aps.org 000028823 0247_ $$2WOS$$aWOS:000089866000013 000028823 0247_ $$2Handle$$a2128/2382 000028823 037__ $$aPreJuSER-28823 000028823 041__ $$aeng 000028823 082__ $$a530 000028823 084__ $$2WoS$$aPhysics, Nuclear 000028823 1001_ $$0P:(DE-Juel1)VDB345$$aElster, C.$$b0$$uFZJ 000028823 245__ $$aNucleon-nucleon scattering in a three dimensional approach 000028823 260__ $$aWoodbury, NY$$bInst.$$c2000 000028823 300__ $$a044002-1 000028823 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article 000028823 3367_ $$2DataCite$$aOutput Types/Journal article 000028823 3367_ $$00$$2EndNote$$aJournal Article 000028823 3367_ $$2BibTeX$$aARTICLE 000028823 3367_ $$2ORCID$$aJOURNAL_ARTICLE 000028823 3367_ $$2DRIVER$$aarticle 000028823 440_0 $$04921$$aPhysical Review C$$v62$$x0556-2813 000028823 500__ $$aRecord converted from VDB: 12.11.2012 000028823 520__ $$aThe nucleon-nucleon (NN) t matrix is calculated directly as function of two vector momenta for different realistic NN potentials. To facilitate this a formalism is developed for solving the two-nucleon Lippmann-Schwinger equation in momentum space without employing a partial wave decomposition. The total spin is heated in a helicity representation. Two different realistic NN interactions, one defined in momentum space and one in coordinate space, are presented in a form suited for this formulation. The angular and momentum dependence of the full amplitude is studied and displayed. A partial wave decomposition of the full amplitude it carried out to compare the presented results with the well-known phase shifts provided by those interactions. 000028823 536__ $$0G:(DE-Juel1)FUEK39$$2G:(DE-HGF)$$aTheoretische Kernphysik$$c20.80.0$$x0 000028823 588__ $$aDataset connected to Web of Science 000028823 650_7 $$2WoSType$$aJ 000028823 7001_ $$0P:(DE-HGF)0$$aFachruddin, I.$$b1 000028823 7001_ $$0P:(DE-HGF)0$$aGlöckle, W.$$b2 000028823 773__ $$0PERI:(DE-600)2844098-5$$gVol. 62, p. 044002-1$$p044002-1$$q62<044002-1$$tPhysical review / C$$v62$$x0556-2813$$y2000 000028823 8564_ $$uhttps://juser.fz-juelich.de/record/28823/files/23640.pdf$$yOpenAccess 000028823 8564_ $$uhttps://juser.fz-juelich.de/record/28823/files/23640.jpg?subformat=icon-1440$$xicon-1440$$yOpenAccess 000028823 8564_ $$uhttps://juser.fz-juelich.de/record/28823/files/23640.jpg?subformat=icon-180$$xicon-180$$yOpenAccess 000028823 8564_ $$uhttps://juser.fz-juelich.de/record/28823/files/23640.jpg?subformat=icon-640$$xicon-640$$yOpenAccess 000028823 909CO $$ooai:juser.fz-juelich.de:28823$$pdnbdelivery$$pdriver$$pVDB$$popen_access$$popenaire 000028823 9131_ $$0G:(DE-Juel1)FUEK39$$bStruktur der Materie und Materialforschung$$k20.80.0$$lKernphysik$$vTheoretische Kernphysik$$x0 000028823 9141_ $$y2000 000028823 915__ $$0StatID:(DE-HGF)0010$$aJCR/ISI refereed 000028823 915__ $$0StatID:(DE-HGF)0510$$2StatID$$aOpenAccess 000028823 9201_ $$0I:(DE-Juel1)VDB301$$d31.12.2000$$gIKP$$kIKP$$lInstitut für Kernphysik$$x0 000028823 970__ $$aVDB:(DE-Juel1)23640 000028823 980__ $$aVDB 000028823 980__ $$aJUWEL 000028823 980__ $$aConvertedRecord 000028823 980__ $$ajournal 000028823 980__ $$aI:(DE-Juel1)VDB301 000028823 980__ $$aUNRESTRICTED 000028823 980__ $$aFullTexts 000028823 9801_ $$aFullTexts