The Nuclear Many-Body Problem

By P. Ring, P. Schuck, M. Strayer. 2004

5,005 citations recorded by the source corpus.

View Paper: https://www.semanticscholar.org/paper/1e7ec3f193b4b49681fbdb9d49e72e419d8a04ac

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Citations in the corpus

• Equations of state for supernovae and compact stars (2016, background): “, the textbooks of Fetter and Walecka (1971); Ring and Schuck (1980); Greiner and Maruhn (1996) for more details.”
• Microscopic approach of fission dynamics applied to fragment kinetic energy and mass distributions in U 238 (2005, background): “The exact form of the collective Hamiltonian Ĥcoll deduced from the GOA can be found in [14, 15].”
• Relativistic continuum Hartree Bogoliubov theory for ground-state properties of exotic nuclei (2005, methodology): “The continuum effect is commonly taken into account in the Hartree-Fock-Bogoliubov (HFB) [35] or relativistic-Hartree-Bogoliubov (RHB) [21] approaches.”
• Microscopic HFB+QRPA predictions of dipole strength for astrophysics applications (2003, methodology): “The QRPA response is obtained from the time-dependent HFB equations [16]: i~ ∂R ∂t = [H(t) + F(t),R(t)] (3) where R, H are the time-dependent generalized density and HFB Hamiltonian respectively, and F the external oscillating field.”
• QUASIPARTICLE RANDOM PHASE APPROXIMATION BASED ON THE RELATIVISTIC HARTREE-BOGOLIUBOV MODEL. II. NUCLEAR SPIN AND ISOSPIN EXCITATIONS (2004, background): “The matrices A and B are defined in the canonical basis [35]”
• Nuclear magic numbers: New features far from stability (2008, background): “This was attributed to the hard-core part of the NN interaction [35].”
• A Guided Tour of ab initio Nuclear Many-Body Theory (2020, methodology): “In this basis, one can then solve the generalized eigenvalue problem, known as the Griffin-Hill-Wheeler equation [147] in the RGM context:”
• Nuclear quantum many-body dynamics (2012, unknown): “In fact, in its linearised version, TDHF is equivalent to the Random Phase Approximation (RPA) [142] which is the basic tool to understand the collective vibrations in terms of independent phonons.”
• Quantum phase transitions in the interacting boson model (2008, background): “ng boson model that will be opened in the next section. One can nd extensive literature investigating various properties of the Lipkin model, including its phase transitional behavior, see e.g. Refs. [7,10,27,134{138]. The model is formulated in terms of pseudospin operators fJ z;J +;J gthat form th”
• The BCS–BEC crossover: From ultra-cold Fermi gases to nuclear systems (2018, methodology): “In this case, the NSR approach corresponds to what in nuclear physics is known as the particleparticle random-phase approximation (pp-RPA) [59].”
• Nuclear equation of state from ground and collective excited state properties of nuclei (2018, methodology): “The latter inequality is very easy to prove [20].”
• Transverse polarisation of quarks in hadrons (2001, methodology): “1 Centre-of-mass motion A problem arising in many model calculations is the removal of spurious contributions to physical observables due to the centre-of-mass motion (for a comprehensive discussion of this matter, see the book by Ring and Schuck [203]).”