Three-body forces and shell structure in calcium isotopes

Understanding and predicting the formation of shell structure from nuclear forces is a central challenge for nuclear physics. While the magic numbers N = 2, 8, 20 are generally well understood, N = 28 is the first standard magic number that is not reproduced in microscopic theories with two-nucleon forces. In this paper, we show that three-nucleon forces give rise to repulsive interactions between two valence neutrons that are key to explain 48Ca as a magic nucleus, with a high 2+ excitation energy and a concentrated magnetic dipole transition strength. The repulsive three-nucleon mechanism improves the agreement with experimental binding energies. Communicated by Professor Jacek Dobaczewski

[1]  G. Hagen,et al.  Ab initio coupled-cluster approach to nuclear structure with modern nucleon-nucleon interactions , 2010, 1005.2627.

[2]  D. R. Entem,et al.  Accurate charge dependent nucleon nucleon potential at fourth order of chiral perturbation theory , 2003 .

[3]  Low-momentum interactions with smooth cutoffs , 2006, nucl-th/0609003.

[4]  T. Duguet,et al.  Ab-initio approach to effective single-particle energies in doubly closed shell nuclei , 2011, 1110.2468.

[5]  Sabine Lee From nuclei to stars : festschrift in honor of Gerald E. Brown , 2011 .

[6]  A. Poves,et al.  Magnetic dipole response in nuclei at the N=28 shell closure: a new look 1 Work supported by the DFG , 1998 .

[7]  B. A. Brown,et al.  New effective interaction for pf-shell nuclei and its implications for the stability of the N = Z = 28 closed core , 2004, nucl-th/0402079.

[8]  F. Touchard,et al.  53K, 54K and 53Ca: Three new neutron rich isotopes , 1983 .

[9]  S. Quaglioni,et al.  Recent developments in no-core shell-model calculations , 2009, 0904.0463.

[10]  U. van Kolck,et al.  Few-nucleon forces from chiral Lagrangians. , 1994 .

[11]  Toshio Suzuki,et al.  Three-body forces and the limit of oxygen isotopes. , 2009, Physical review letters.

[12]  L. Tassan-Got,et al.  Discovery and cross-section measurement of 58 new fission products in projectile-fission of 750 · A MeV 238U , 1997 .

[13]  H. Hammer,et al.  Modern theory of nuclear forces , 2004, 0811.1338.

[14]  P. Piecuch,et al.  Coupled-Cluster Theory for Three-Body Hamiltonians , 2007, 0704.2854.

[15]  F. Nowacki,et al.  Shell model study of the isobaric chains A=50, A=51 and A=52 , 2000, nucl-th/0012077.

[16]  B. A. Brown,et al.  Magic numbers in exotic nuclei and spin-isospin properties of the NN interaction. , 2001, Physical review letters.

[17]  M. Hjorth-Jensen,et al.  Realistic effective interactions for nuclear systems , 1995 .

[18]  S. K. Bogner,et al.  From low-momentum interactions to nuclear structure , 2009, 0912.3688.

[19]  A. H. Wapstra,et al.  The AME2003 atomic mass evaluation . (II). Tables, graphs and references , 2003 .

[20]  H. Witała,et al.  Three-nucleon forces from chiral effective field theory , 2002, nucl-th/0208023.

[21]  F. Nowacki,et al.  The shell model as a unified view of nuclear structure , 2004, nucl-th/0402046.

[22]  K. Hebeler,et al.  Chiral three-nucleon forces and neutron matter , 2009, 0911.0483.

[23]  T. Kubo,et al.  Production of very neutron-rich nuclei with a Ge-76 beam , 2009, 0908.3852.

[24]  H. Miyazawa,et al.  Pion Theory of Three-Body Forces , 1957 .

[25]  Toshio Suzuki,et al.  Novel features of nuclear forces and shell evolution in exotic nuclei. , 2009, Physical review letters.

[26]  A. Zuker Three-body monopole corrections to realistic interactions. , 2002, Physical review letters.

[27]  A. Green Nucleon resonance in nuclei , 1976 .

[28]  A. Poves,et al.  Theoretical spectroscopy and the fp shell , 1981 .