Issue |
EPJ Web Conf.
Volume 113, 2016
21st International Conference on Few-Body Problems in Physics
|
|
---|---|---|
Article Number | 06009 | |
Number of page(s) | 4 | |
Section | Nuclear Structure and Reactions | |
DOI | https://doi.org/10.1051/epjconf/201611306009 | |
Published online | 25 March 2016 |
https://doi.org/10.1051/epjconf/201611306009
Contributions of chiral two- and three-nucleon interactions to closed shell nuclei
1 Institute of Physics, Academia Sinica, Taipei, 11529, Taiwan, ROC
2 Dept. of Electro-Optical Engineering, National Taipei University of Technology, Taipei, 10608, Taiwan, ROC
3 Department of Physics, State University New York at Stony Brook, Stony Brook, New York 11794, USA
a e-mail: phtzengyh@sinica.edu.tw
b e-mail: sytsay@mail.ntut.edu.tw
c e-mail: kuo@tonic.physics.sunysb.edu
Published online: 25 March 2016
Using two-nucleon force alone is usually inadequate to interpret nuclear systems’ experimental data. We adopt a chiral N3LO two-nucleon potential V2N with the inclusion of an in-medium three-nucleon (NNN) force V̄3N to calculate binding energies of closed-shell nuclei. The matrix elements of low momentum nucleon-nucleon potential Vlow−k obtained from integrating the high momentum part of a realistic potentials is inputted in the particle-particle hole-hole ring diagram calculation to study nuclear properties. Nuclear binding energies are accurately reproduced. Without this three-nucleon force, the nuclear binding energy is too weak, as already known. The correction from ring diagrams of order higher than 1 can not be ignored.
© Owned by the authors, published by EDP Sciences, 2016
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