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000033608 0247_ $$2arXiv$$aarXiv:nucl-th/0307011$$cnucl-th
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000033608 035__ $$9arXiv$$aoai:arXiv.org:nucl-th/0307011$$zoai:arXiv.org:nucl-th/0307011
000033608 035__ $$9SPIRESTeX$$zFachuddin:2003ps
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000033608 084__ $$2WoS$$aPhysics, Nuclear
000033608 084__ $$2PACS$$a21.45.+v
000033608 084__ $$2PACS$$a13.75.Cs
000033608 084__ $$2PACS$$a25.40.Kv
000033608 1001_ $$0P:(DE-HGF)0$$aFachruddin, I.$$b0
000033608 245__ $$aThe Nd Break-Up Process in Leading Order in a Three-Dimensional Approach
000033608 260__ $$aWoodbury, NY$$bInst.$$c2003
000033608 264_1 $$2Crossref$$3online$$bAmerican Physical Society (APS)$$c2003-11-21
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000033608 440_0 $$04921$$aPhysical Review C$$v68$$x0556-2813
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000033608 500__ $$9arXiv$$a31 pages + 9 figures, revtex Journal-ref: Phys. Rev. C68, 054003 (2003)
000033608 520__ $$aA three-dimensional approach based on momentum vectors as variables for solving the three-nucleon Faddeev equation in first order is presented. The nucleon-deuteron breakup amplitude is evaluated in leading order in the nucleon-nucleon (NN) T matrix, which is also generated directly in three dimensions avoiding a summation of partial wave contributions. A comparison of semiexclusive observables in the d(p,n)pp reaction calculated in this scheme with those generated by a traditional partial wave expansion shows perfect agreement at lower energies. At about 200 MeV nucleon laboratory energies deviations in the peak of the cross section appear, which may indicate that special care is required in a partial wave approach for energies at and higher than 200 MeV . The role of higher order rescattering processes beyond the leading order in the NN T matrix is investigated with the result that at 200 MeV rescattering still provides important contributions to the cross section and certain spin observables. The influence of a relativistic treatment of the kinematics is investigated. It is found that relativistic effects become important at projectile energies higher than 200 MeV .
000033608 536__ $$0G:(DE-Juel1)FUEK241$$2G:(DE-HGF)$$aPhysik der Hadronen$$cM01$$x0
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000033608 7001_ $$0P:(DE-Juel1)VDB345$$aElster, C.$$b1$$uFZJ
000033608 7001_ $$0P:(DE-HGF)0$$aGlöckle, W.$$b2
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000033608 8567_ $$uhttp://hdl.handle.net/2128/1685$$uhttp://dx.doi.org/10.1103/PhysRevC.68.054003
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000033608 999C5 $$1L. D. Faddeev$$2Crossref$$oL. D. Faddeev 1960$$y1960
000033608 999C5 $$1L. D. Faddeev$$2Crossref$$oL. D. Faddeev 1961$$y1961
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000033608 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevC.66.044010
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000033608 999C5 $$1M. E. Rose$$2Crossref$$oM. E. Rose Elementary Theory of Angular Momentum 1957$$tElementary Theory of Angular Momentum$$y1957
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000033608 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevC.33.709
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000033608 999C5 $$1R. Machleidt$$2Crossref$$oR. Machleidt 1989$$y1989
000033608 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevC.51.38
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