This title appears in the Scientific Report :
2006
Please use the identifier:
http://dx.doi.org/10.1103/PhysRevC.73.044004 in citations.
Please use the identifier: http://hdl.handle.net/2128/10595 in citations.
Testing nuclear forces by polarization transfer coefficients in d(polarized-p, polarized-p)d and d(polarized-p, polarized-d)p reactions E(p,lab) = 22.7-MeV
Testing nuclear forces by polarization transfer coefficients in d(polarized-p, polarized-p)d and d(polarized-p, polarized-d)p reactions E(p,lab) = 22.7-MeV
The proton to proton polarization transfer coefficients K-x(x'),K-y(y'), and K-z(x'), and the proton to deuteron polarization transfer coefficients K-x(x'),K-y(y'),K-z(x'), K(x)(y')z('),K(y)(z')z('),K(z)(y')z('),K(y)(x')z('), and...
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Personal Name(s): | Witala, H. |
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Golak, J. / Skibinski, R. / Glöckle, W. / Nogga, A. / Epelbaum, E. / Kamada, H. / Kievsky, A. / Viviani, M. | |
Contributing Institute: |
Institut 3 (Theoretische Kernphysik); IKP-TH |
Published in: | Physical Review C Physical review / C, 73 73 (2006 2006) 4 4, S. 044004 044004 |
Imprint: |
Woodbury, NY
Inst.
2006
2006-04-12 2006-04-01 |
Physical Description: |
044004 |
DOI: |
10.1103/PhysRevC.73.044004 |
Document Type: |
Journal Article |
Research Program: |
Physik der Hadronen und Kerne |
Series Title: |
Physical Review C
73 |
Subject (ZB): | |
Link: |
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Publikationsportal JuSER |
Please use the identifier: http://hdl.handle.net/2128/10595 in citations.
The proton to proton polarization transfer coefficients K-x(x'),K-y(y'), and K-z(x'), and the proton to deuteron polarization transfer coefficients K-x(x'),K-y(y'),K-z(x'), K(x)(y')z('),K(y)(z')z('),K(z)(y')z('),K(y)(x')z('), and K(y)(x')x(')-y(')y(') were measured in d(p,p)d and d(p,d)p reactions, respectively, at E-p(lab)=22.7 MeV. The data were compared to predictions of modern nuclear forces obtained by solving the three-nucleon Faddeev equations in momentum space. Realistic (semi)phenomenological nucleon-nucleon potentials combined with model three-nucleon forces and modern chiral nuclear forces were used. The AV18, CD Bonn, and Nijm I and II nucleon-nucleon interactions were applied alone or combined with the Tucson-Melbourne 99 three-nucleon force, adjusted separately for each potential to reproduce the triton binding energy. For the AV18 potential, the Urbana IX three-nucleon force was also used. In addition, chiral NN potentials in the next-to-leading order and chiral two- and three-nucleon forces in the next-to-next-to-leading order were applied. Only when three-nucleon forces are included does a satisfactory description of all data result. For the chiral approach, the restriction to the forces in the next-to-leading order is insufficient. Only when going over to the next-to-next-to-leading order does one get a satisfactory description of the data, similar to the one obtained with the (semi)phenomenological forces. |