This title appears in the Scientific Report :
2016
Please use the identifier:
http://dx.doi.org/10.1007/s00601-016-1156-3 in citations.
Please use the identifier: http://hdl.handle.net/2128/13496 in citations.
Role of the Total Isospin 3/2 Component in Three-Nucleon Reactions
Role of the Total Isospin 3/2 Component in Three-Nucleon Reactions
We discuss the role of the three-nucleon isospin T=3/2 amplitude in elastic neutron–deuteron scattering and in the deuteron breakup reaction. The contribution of this amplitude originates from charge-independence breaking of the nucleon–nucleon potential and is driven by the difference between neutr...
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Personal Name(s): | Witała, H. (Corresponding author) |
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Golak, J. / Skibiński, R. / Topolnicki, K. / Epelbaum, E. / Hebeler, K. / Kamada, H. / Krebs, H. / Meißner, U.-G. / Nogga, A. | |
Contributing Institute: |
Theorie der starken Wechselwirkung; IKP-3 Theorie der Starken Wechselwirkung; IAS-4 |
Published in: | Few-body systems, 57 (2016) 12, S. 1213 - 1225 |
Imprint: |
Wien [u.a.]
Springer
2016
|
DOI: |
10.1007/s00601-016-1156-3 |
Document Type: |
Journal Article |
Research Program: |
The Strong Interaction at Neutron-Rich Extremes Computational Science and Mathematical Methods |
Link: |
OpenAccess OpenAccess |
Publikationsportal JuSER |
Please use the identifier: http://hdl.handle.net/2128/13496 in citations.
We discuss the role of the three-nucleon isospin T=3/2 amplitude in elastic neutron–deuteron scattering and in the deuteron breakup reaction. The contribution of this amplitude originates from charge-independence breaking of the nucleon–nucleon potential and is driven by the difference between neutron–neutron (proton–proton) and neutron–proton forces. We study the magnitude of that contribution to the elastic scattering and breakup observables, taking the locally regularized chiral N4LO nucleon–nucleon potential supplemented by the chiral N2LO three-nucleon force. For comparison we employ also the Av18 nucleon–nucleon potential combined with the Urbana IX three-nucleon force. We find that the isospin T=3/2 component is important for the breakup reaction and the proper treatment of charge-independence breaking in this case requires the inclusion of the 1S0 state with isospin T=3/2. For neutron–deuteron elastic scattering the T=3/2 contributions are insignificant and charge-independence breaking can be accounted for by using the effective t-matrix generated with the so-called ‘‘2/3−1/3" rule. |