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We optimize $��$-full nuclear interactions from chiral effective field theory. The low-energy constants of the contact potentials are constrained by two-body scattering phase shifts, and by properties of bound-state of $A=2$ to $4$ nucleon system
Externí odkaz:
https://explore.openaire.eu/search/publication?articleId=doi_________::d8b4a11e4a59cea5880295e60f814530
Autor:
Hagen, G., Ekstr��m, A., Forss��n, C., Jansen, G. R., Nazarewicz, W., Papenbrock, T., Wendt, K. A., Bacca, S., Barnea, N., Carlsson, B., Drischler, C., Hebeler, K., Hjorth-Jensen, M., Miorelli, M., Orlandini, G., Schwenk, A., Simonis, J.
What is the size of the atomic nucleus? This deceivably simple question is difficult to answer. While the electric charge distributions in atomic nuclei were measured accurately already half a century ago, our knowledge of the distribution of neutron
Externí odkaz:
https://explore.openaire.eu/search/publication?articleId=doi_dedup___::f880ebef7dedf38819dd00e842071d12
http://arxiv.org/abs/1509.07169
http://arxiv.org/abs/1509.07169
Autor:
Carlsson, B. D., Ekstr��m, A., Forss��n, C., Str��mberg, D. Fahlin, Jansen, G. R., Lilja, O., Lindby, M., Mattsson, B. A., Wendt, K. A.
Publikováno v:
Physical Review X, Vol 6, Iss 1, p 011019 (2016)
Physical Review X
Physical Review X (2160-3308) vol.6(2016)
Physical Review X
Physical Review X (2160-3308) vol.6(2016)
Chiral effective field theory (chiEFT) provides a systematic approach to describe low-energy nuclear forces. Moreover, chiEFT is able to provide well-founded estimates of statistical and systematic uncertainties -- although this unique advantage has
Externí odkaz:
https://explore.openaire.eu/search/publication?articleId=doi_dedup___::9531c05d27176323113713deee8a454e
http://arxiv.org/abs/1506.02466
http://arxiv.org/abs/1506.02466