Emergent properties of nuclei from ab initio coupled-cluster calculations

Hagen, G.; Hjorth-Jensen, M.; Jansen, G. R.; Papenbrock, T.

doi:10.1088/0031-8949/91/6/063006

Emergent properties of nuclei from ab initio coupled-cluster calculations

Journal Article · Tue May 17 00:00:00 EDT 2016 · Physica Scripta

DOI:https://doi.org/10.1088/0031-8949/91/6/063006· OSTI ID:1286964

Hagen, G. ^[1]; Hjorth-Jensen, M. ^[2]; Jansen, G. R. ^[3]; Papenbrock, T. ^[1]

Oak Ridge National Lab. (ORNL), Oak Ridge, TN (United States); Univ. of Tennessee, Knoxville, TN (United States)
Michigan State Univ., East Lansing, MI (United States); Univ. of Oslo (Norway)
Oak Ridge National Lab. (ORNL), Oak Ridge, TN (United States)

Emergent properties such as nuclear saturation and deformation, and the effects on shell structure due to the proximity of the scattering continuum and particle decay channels are fascinating phenomena in atomic nuclei. In recent years, ab initio approaches to nuclei have taken the first steps towards tackling the computational challenge of describing these phenomena from Hamiltonians with microscopic degrees of freedom. Our endeavor is now possible due to ideas from effective field theories, novel optimization strategies for nuclear interactions, ab initio methods exhibiting a soft scaling with mass number, and ever-increasing computational power. We review some of the recent accomplishments. We also present new results. The recently optimized chiral interaction NNLO$${}_{{\rm{sat}}}$$ is shown to provide an accurate description of both charge radii and binding energies in selected light- and medium-mass nuclei up to 56Ni. We derive an efficient scheme for including continuum effects in coupled-cluster computations of nuclei based on chiral nucleon–nucleon and three-nucleon forces, and present new results for unbound states in the neutron-rich isotopes of oxygen and calcium. Finally, the coupling to the continuum impacts the energies of the $${J}^{\pi }=1/{2}^{-},3/{2}^{-},7/{2}^{-},3/{2}^{+}$$ states in $${}^{\mathrm{17,23,25}}$$O, and—contrary to naive shell-model expectations—the level ordering of the $${J}^{\pi }=3/{2}^{+},5/{2}^{+},9/{2}^{+}$$ states in $${}^{\mathrm{53,55,61}}$$Ca.

View Accepted Manuscript (DOE)

Research Organization:: Oak Ridge National Laboratory (ORNL), Oak Ridge, TN (United States); Oak Ridge National Laboratory (ORNL), Oak Ridge, TN (United States). Oak Ridge Leadership Computing Facility (OLCF)

Sponsoring Organization:: USDOE Office of Science (SC), Nuclear Physics (NP); USDOE Office of Science (SC), Nuclear Physics (NP) (SC-26)

Grant/Contract Number:: AC05-00OR22725; FG02-96ER40963; SC0008499

OSTI ID:: 1286964

Alternate ID(s):: OSTI ID: 1253425
OSTI ID: 22874580

Journal Information:: Physica Scripta, Journal Name: Physica Scripta Journal Issue: 6 Vol. 91; ISSN 0031-8949

Publisher:: IOP PublishingCopyright Statement

Country of Publication:: United States

Language:: English

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