Convergence in the no-core shell model with low-momentum two-nucleon interactions

Abstract The convergence of no-core shell model (NCSM) calculations using renormalization group evolved low-momentum two-nucleon interactions is studied for light nuclei up to 7 Li. Because no additional transformation was used in applying the NCSM framework, the energy calculations satisfy the variational principle for a given Hamiltonian. Dramatic improvements in convergence are found as the cutoffs are lowered. The renormalization group equations are truncated at two-body interactions, so the evolution is only approximately unitary and converged energies for A ⩾ 3 vary with the cutoff. This approximation is systematic, however, and for useful cutoff ranges the energy variation is comparable to natural-size truncation errors inherent from the initial chiral effective field theory potential.

[1]  P. Navrátil,et al.  Spectra and Binding Energy Predictions of Chiral Interactions for 7Li , 2005, nucl-th/0511082.

[2]  The Similarity renormalization group , 2000, hep-ph/0009071.

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

[4]  J P Vary,et al.  Properties of 12C in the Ab initio nuclear shell model. , 2000, Physical review letters.

[5]  K. Wilson,et al.  Perturbative renormalization group for Hamiltonians. , 1994, Physical review. D, Particles and fields.

[6]  R. Furnstahl,et al.  Similarity renormalization group for nucleon-nucleon interactions , 2006, nucl-th/0611045.

[7]  Variational calculations of nuclei with low-momentum potentials , 2005, nucl-th/0508022.

[8]  A. I. Mazur,et al.  Realistic Nuclear Hamiltonian: Ab exitu approach , 2005, nucl-th/0512105.

[9]  Effective Operators Within the Ab Initio No-Core Shell Model , 2004, nucl-th/0412004.

[10]  Is nuclear matter perturbative with low-momentum interactions? , 2005, nucl-th/0504043.

[11]  P. Navrátil,et al.  Few-nucleon systems in a translationally invariant harmonic oscillator basis , 1999, nucl-th/9907054.

[12]  Wilson,et al.  Renormalization of Hamiltonians. , 1993, Physical review. D, Particles and fields.

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

[14]  R. Furnstahl,et al.  Three-body forces produced by a similarity renormalization group transformation in a simple model , 2007, 0708.1602.

[15]  H. Hergert,et al.  Unitary correlation operator method from a similarity renormalization group perspective , 2007, nucl-th/0703006.

[16]  Ab initio shell model with a genuine three-nucleon force for the p-shell nuclei , 2003, nucl-th/0305090.

[17]  Franz Wegner Flow‐equations for Hamiltonians , 1994 .

[18]  G. Hagen,et al.  Benchmark calculations for 3H, 4He, 16O and 40Ca with ab-initio coupled-cluster theory , 2007, 0707.1516.

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

[20]  Modern nuclear force predictions for the alpha particle , 2000, Physical review letters.

[21]  F. Wilczek Quantum Field Theory , 1998, hep-th/9803075.

[22]  Petr Navratil,et al.  Large-basis ab initio no-core shell model and its application to 12 C , 2000 .

[23]  Ericka Stricklin-Parker,et al.  Ann , 2005 .

[24]  A. I. Mazur,et al.  Nucleon–Nucleon Interaction in the J-Matrix Inverse Scattering Approach and Few-Nucleon Systems , 2003, nucl-th/0312029.

[25]  P. Navrátil,et al.  Ab initio shell model calculations with three-body effective interactions for p-shell nuclei. , 2002, Physical review letters.

[26]  E. Epelbaum,et al.  The Two-nucleon system at next-to-next-to-next-to-leading order , 2004, nucl-th/0405048.

[27]  H. Hergert,et al.  Matrix elements and few-body calculations within the unitary correlation operator method , 2005, nucl-th/0505080.

[28]  S. Bogner,et al.  Model independent low momentum nucleon interaction from phase shift equivalence , 2003, nucl-th/0305035.

[29]  A. I. Mazur,et al.  Novel NN interaction and the spectroscopy of light nuclei [rapid communication] , 2004, nucl-th/0407018.

[30]  Nuclear structure with accurate chiral perturbation theory nucleon-nucleon potential: Application to 6Li and 10B , 2003, nucl-th/0311036.

[31]  R. Furnstahl,et al.  Decoupling in the similarity renormalization group for nucleon-nucleon forces , 2007, 0711.4252.

[32]  R. Wiringa,et al.  Accurate nucleon-nucleon potential with charge-independence breaking. , 1995, Physical review. C, Nuclear physics.

[33]  A Nogga,et al.  Structure of A=10-13 nuclei with two- plus three-nucleon interactions from chiral effective field theory. , 2007, Physical review letters.