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NSR database version of April 27, 2024.

Search: Author = J.Navarro

Found 62 matches.

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2023BA20      Eur.Phys.J. A 59, 173 (2023); Errarum Eur.Phys.J. A 59, 219 (2023)

L.Batail, D.Davesne, S.Peru, P.Becker, A.Pastore, J.Navarro

A three-ranged Gogny interaction in touch with pion exchange: promising results to improve infinite matter properties

doi: 10.1140/epja/s10050-023-01073-w
Citations: PlumX Metrics


2023DA14      Universe 9, 398 (2023)

D.Davesne, A.Pastore, J.Navarro

Hartree-Fock Calculations in Semi-Infinite Matter with Gogny Interactions

doi: 10.3390/universe9090398
Citations: PlumX Metrics


2023DA15      Phys.Rev. C 108, 034003 (2023)

D.Davesne, J.W.Holt, J.Navarro, A.Pastore

Landau sum rules with noncentral quasiparticle interactions

doi: 10.1103/PhysRevC.108.034003
Citations: PlumX Metrics


2022PA02      Ann.Nucl.Energy 165, 108629 (2022)

V.Patel, J.Navarro, W.Windes, P.Tsvetkov

An uncertainty quantification method relevant to material test reactors

doi: 10.1016/j.anucene.2021.108629
Citations: PlumX Metrics


2019DA15      Phys.Rev. C 100, 064301 (2019)

D.Davesne, A.Pastore, J.Navarro

Linear response theory in asymmetric nuclear matter for Skyrme functionals including spin-orbit and tensor terms. II. Charge exchange

doi: 10.1103/PhysRevC.100.064301
Citations: PlumX Metrics


2018BE22      Acta Phys.Pol. B49, 331 (2018)

P.Becker, D.Davesne, J.Meyer, J.Navarro, A.Pastore

Skyrme N2LO Pseudo-potential for Calculations of Properties of Atomic Nuclei

NUCLEAR STRUCTURE 132Sn; calculated isoscalar densities vs radius using N2LO extension of usual Skyrme pseudo-potential, neutron effective mass vs density and effective masses of neutrons and protons vs asymmetry parameter using Symmetric Nuclear Matter (SNM) and Pure Neutron Matter (PNM). 40,42,44,46,48,50,52,54Ca, 58,60,62,64,66,68Ni, 110,112,114,116,118,120,122,124,126,128,130,132,134Sn, 136,138,140,142,144,146,148,150,152,154,156,158.160,162,164,166,168,170,172,174,176,178,180,182,184,186,188,190,192,194,!96,198,200,202,204,206,208,210,212,214Pb; calculated average pairing gaps vs neutron number. Compared with data.

doi: 10.5506/aphyspolb.49.331
Citations: PlumX Metrics


2018DA05      Phys.Rev. C 97, 044304 (2018)

D.Davesne, J.Navarro, J.Meyer, K.Bennaceur, A.Pastore

Two-body contributions to the effective mass in nuclear effective interactions

doi: 10.1103/PhysRevC.97.044304
Citations: PlumX Metrics


2017BE28      Phys.Rev. C 96, 044330 (2017)

P.Becker, D.Davesne, J.Meyer, J.Navarro, A.Pastore

Solution of Hartree-Fock-Bogoliubov equations and fitting procedure using the N2LO Skyrme pseudopotential in spherical symmetry

NUCLEAR STRUCTURE 208Pb; calculated isoscalar densities, radial dependence of coefficients using the SN2LO1 and SLy5 interactions, for centrifugal and spin-orbit fields. 208Pb, 120Sn, 40Ca; calculated energies (total, kinetic, field, spin-orbit, Coulomb, and neutron pairing) using the WHISKY and LENTEUR codes with self-consistent HF calculations and the SLy5 interaction. 40Ca, 208Pb; calculated neutron single-particle energies around the Fermi energy for SLy5 and SN2LO1 parametrizations. 34,36,38,40,42,44,46,48,50,52,54,56Ca, 48,50,52,54,56,58,60,62,64,66,68,70,72,74,76,78Ni, 100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136Sn, 178,180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214Pb, 48Ca, 50Ti, 52Cr, 54Fe, 56Ni, 58Zn, 60Ge, 78Ni, 80Zn, 82Ge, 84Se, 86Kr, 88Sr, 90Zr, 92Mo, 94Ru, 96Pd, 98Cd, 100Sn, 130Cd, 132Sn, 134Te, 136Xe, 138Ba, 140Ce, 142Nd, 144Sm, 146Gd, 148Dy, 150Er, 152Yb, 206Hg, 208Pb, 210Po, 212Rn, 214Ra, 216Th, 218U; calculated binding energies and proton radii for isotopic and isotonic chains using extended Skyrme interaction SN2LO1, and compared with experimental values, as well as with calculations using the SLy5 parametrization.

doi: 10.1103/PhysRevC.96.044330
Citations: PlumX Metrics


2017DA08      Acta Phys.Pol. B48, 265 (2017)

D.Davesne, P.Becker, A.Pastore, J.Navarro

Does the Gogny Interaction Need a Third Gaussian?

doi: 10.5506/APhysPolB.48.265
Citations: PlumX Metrics


2016DA02      Phys.Rev. C 93, 064001 (2016)

D.Davesne, P.Becker, A.Pastore, J.Navarro

Partial-wave decomposition of the finite-range effective tensor interaction

doi: 10.1103/PhysRevC.93.064001
Citations: PlumX Metrics


2015DA02      Phys.Rev. C 91, 014323 (2015)

D.Davesne, J.W.Holt, A.Pastore, J.Navarro

Effect of three-body forces on response functions in infinite neutron matter

doi: 10.1103/PhysRevC.91.014323
Citations: PlumX Metrics


2015DA06      Phys.Rev. C 91, 064303 (2015)

D.Davesne, J.Navarro, P.Becker, R.Jodon, J.Meyer, A.Pastore

Extended Skyrme pseudopotential deduced from infinite nuclear matter properties

doi: 10.1103/PhysRevC.91.064303
Citations: PlumX Metrics


2015DA15      Phys.Scr. 90, 114002 (2015)

D.Davesne, J.Meyer, A.Pastore, J.Navarro

Partial wave decomposition of the N3LO equation of state

doi: 10.1088/0031-8949/90/11/114002
Citations: PlumX Metrics


2015PA34      Phys.Rev. C 92, 024305 (2015)

A.Pastore, D.Tarpanov, D.Davesne, J.Navarro

Spurious finite-size instabilities in nuclear energy density functionals: Spin channel

NUCLEAR STRUCTURE 40Ca, 56Ni, 132Sn, 208Pb; calculated finite-size instabilities in the ground state properties of atomic nuclei and vibrational excited states. Skyrme functionals non-converging results in atomic nuclei. Discussed quantitative stability criterion to detect finite-size instabilities. Systematic fully-self consistent Random Phase Approximation (RPA) calculations in spherical doubly-magic nuclei. Comparison of RPA calculations in atomic nuclei with Linear Response in Symmetric Nuclear Matter.

doi: 10.1103/PhysRevC.92.024305
Citations: PlumX Metrics


2014DA06      Phys.Rev. C 89, 044302 (2014)

D.Davesne, A.Pastore, J.Navarro

Linear response theory in asymmetric nuclear matter for Skyrme functionals including spin-orbit and tensor terms

doi: 10.1103/PhysRevC.89.044302
Citations: PlumX Metrics


2014NA33      Nucl.Data Sheets 118, 571 (2014)

J.Navarro, T.A.Ring, D.W.Nigg

A Feasibility and Optimization Study to Design a Nondestructive ATR Fuel Permanent Scanning System to Determine Fuel Burnup

doi: 10.1016/j.nds.2014.04.138
Citations: PlumX Metrics


2014PA11      J.Phys.(London) G41, 055103 (2014)

A.Pastore, D.Davesne, J.Navarro

Nuclear matter response function with a central plus tensor Landau interaction

doi: 10.1088/0954-3899/41/5/055103
Citations: PlumX Metrics


2014PA42      Phys.Rev. C 90, 025804 (2014)

A.Pastore, M.Martini, D.Davesne, J.Navarro, S.Goriely, N.Chamel

Linear response theory and neutrino mean free path using Brussels-Montreal Skyrme functionals

doi: 10.1103/PhysRevC.90.025804
Citations: PlumX Metrics


2013NA07      Phys.Rev. C 87, 044329 (2013)

J.Navarro, A.Polls

Spin instabilities of infinite nuclear matter and effective tensor interactions

doi: 10.1103/PhysRevC.87.044329
Citations: PlumX Metrics


2009PE16      Phys.Rev. C 80, 025802 (2009)

M.A.Perez-Garcia, J.Navarro, A.Polls

Neutron Fermi liquids under the presence of a strong magnetic field with effective nuclear forces

doi: 10.1103/PhysRevC.80.025802
Citations: PlumX Metrics


2008MA20      Phys.Rev. C 77, 064306 (2008)

J.Margueron, J.Navarro, Nguyen Van Giai, P.Schuck

Continued fraction approximation for the nuclear matter response function

doi: 10.1103/PhysRevC.77.064306
Citations: PlumX Metrics


2006MA42      Phys.Rev. C 74, 015805 (2006)

J.Margueron, N.Van Giai, J.Navarro

Effects of spin-orbit interaction on nuclear response and neutrino mean free path

doi: 10.1103/PhysRevC.74.015805
Citations: PlumX Metrics


2006NA36      Eur.Phys.J. A 30, 333 (2006)

J.Navarro, P.-G.Reinhard, E.Suraud

Small fermionic systems: The common methods and challenges

doi: 10.1140/epja/i2006-10127-4
Citations: PlumX Metrics


2005MA74      Phys.Rev. C 72, 034311 (2005)

J.Margueron, N.Van Giai, J.Navarro

Nuclear response functions in homogeneous matter with finite range effective interactions

doi: 10.1103/PhysRevC.72.034311
Citations: PlumX Metrics


2004MA73      Phys.Rev. C 70, 028801 (2004)

J.Margueron, J.Navarro, P.Blottiau

Nuclear liquid-gas phase transition and supernovae evolution

doi: 10.1103/PhysRevC.70.028801
Citations: PlumX Metrics


2003MA49      Nucl.Phys. A719, 169c (2003)

J.Margueron, J.Navarro, N.Van Giai

Neutrino mean free path and in-medium nuclear interaction

doi: 10.1016/S0375-9474(03)00987-4
Citations: PlumX Metrics


2002MA49      Phys.Rev. C66, 014303 (2002)

J.Margueron, J.Navarro, V.G.Nguyen

Instabilities of Infinite Matter with Effective Skyrme-Type Interactions

doi: 10.1103/PhysRevC.66.014303
Citations: PlumX Metrics


2001GU19      Nucl.Phys. A689, 499c (2001)

R.Guardiola, J.Navarro

Description of Strongly Interacting Systems by Means of Jastrow and Configuration Interaction Correlated Wave Functions

doi: 10.1016/S0375-9474(01)00890-9
Citations: PlumX Metrics


2000MO11      Phys.Lett. 480B, 61 (2000)

I.Moliner, R.F.Bishop, N.R.Walet, R.Guardiola, J.Navarro, M.Portesi

The Translationally-Invariant Coupled Cluster Method in Coordinate Space

doi: 10.1016/S0370-2693(00)00368-3
Citations: PlumX Metrics


1999BI13      J.Phys.(London) G25, 945 (1999)

R.F.Bishop, R.Guardiola, P.I.Moliner, J.Navarro, M.Portesi, N.R.Walet

Microscopic and Translationally-Invariant Calculations with Tensor Forces and Tensor Correlations

NUCLEAR STRUCTURE 4He; calculated binding energy. Several interactions compared.

doi: 10.1088/0954-3899/25/4/076
Citations: PlumX Metrics


1999HE35      Nucl.Phys. A658, 327 (1999)

E.S.Hernandez, J.Navarro, A.Polls

Response of Asymmetric Nuclear Matter to Isospin-Flip Probes

doi: 10.1016/S0375-9474(99)00363-2
Citations: PlumX Metrics


1999NA35      Phys.Rev. C60, 045801 (1999)

J.Navarro, E.S.Hernandez, D.Vautherin

Neutrino Propagation and Spin Zero Sound in Hot Neutron Matter with Skyrme Interactions

doi: 10.1103/PhysRevC.60.045801
Citations: PlumX Metrics


1999NA45      Nucl.Phys. (Supplement) A654, 912c (1999)

J.Navarro, E.S.Hernandez, D.Vautherin

Neutrino Mean Free Path in Hot Neutron Matter with Skyrme Interactions

doi: 10.1016/S0375-9474(00)88571-1
Citations: PlumX Metrics


1998BI16      Nucl.Phys. A643, 243 (1998)

R.F.Bishop, R.Guardiola, I.Moliner, J.Navarro, M.Portesi, A.Puente, N.R.Walet

Translationally Invariant Treatment of Pair Correlations in Nuclei II. Tensor Correlations

NUCLEAR STRUCTURE 4He, 8Be, 12C, 16O; calculated binding energies; deduced tensor correlations contributions. Realistic V6 interactions, several potentials compared, translational invariance.

doi: 10.1016/S0375-9474(98)00562-4
Citations: PlumX Metrics


1998GU02      Nucl.Phys. A628, 187 (1998)

R.Guardiola, I.Moliner, J.Navarro, M.Portesi

Translationally-Invariant Coupled-Cluster Method for Finite Systems

doi: 10.1016/S0375-9474(97)00627-1
Citations: PlumX Metrics


1997HE20      Phys.Lett. 413B, 1 (1997)

E.S.Hernandez, J.Navarro, A.Polls

Disappearance of Zero Sound in Asymmetric Nuclear Matter

NUCLEAR STRUCTURE 208Pb; calculated asymmetry parameter Y vs energy, temperature; deduced zero sound related features. Thermal RPA response, Skyrme interaction.

doi: 10.1016/S0370-2693(97)01173-8
Citations: PlumX Metrics


1997HE25      Nucl.Phys. A627, 460 (1997)

E.S.Hernandez, J.Navarro, A.Polls

RPA Susceptibility of Asymmetric Nuclear Matter at Finite Temperatures with Skyrme Interactions

doi: 10.1016/S0375-9474(97)00506-X
Citations: PlumX Metrics


1996BA41      Z.Phys. A355, 23 (1996)

M.Barranco, E.S.Hernandez, J.Navarro

Two Quasiparticle Scattering and Pairing in Neutron Matter with Skyrme Interactions

doi: 10.1007/s002180050073
Citations: PlumX Metrics


1996GU16      Phys.Lett. 383B, 243 (1996)

R.Guardiola, P.I.Moliner, J.Navarro

Two-Body and Hyperradial Correlations in the Description of Many-Body Systems

NUCLEAR STRUCTURE A=4; A=16; A=40; calculated bosonic systems binding energies variational upperbound; deduced hyperradial correlations role. Different approaches used.

doi: 10.1016/0370-2693(96)00765-4
Citations: PlumX Metrics


1996GU19      Nucl.Phys. A609, 218 (1996)

R.Guardiola, P.I.Moliner, J.Navarro, R.F.Bishop, A.Puente, N.R.Walet

Translationally Invariant Treatment of Pair Correlations in Nuclei: I. Spin and isospin dependent correlations

NUCLEAR STRUCTURE 4He, 8Be, 12C, 16O; calculated binding energy. Translationally invariant pair correlations treatment, spin, isospin dependent correlations.

doi: 10.1016/S0375-9474(96)00315-6
Citations: PlumX Metrics


1996HE03      Nucl.Phys. A597, 1 (1996)

E.S.Hernandez, J.Navarro, A.Polls, J.Ventura

Finite Temperature RPA in Symmetric Nuclear Matter with Skyrme Interactions

doi: 10.1016/0375-9474(95)00426-2
Citations: PlumX Metrics


1996NA20      J.Phys.(London) G22, 1363 (1996)

J.Navarro, X.Vinas

Extended Thomas-Fermi Expansion from Nuclear Linear Response

doi: 10.1088/0954-3899/22/9/009
Citations: PlumX Metrics


1993GU14      Acta Phys.Pol. B24, 525 (1993)

R.Guardiola, J.Navarro

Microscopic Calculations of the Hypernucleus (Λ)5He


1993OS07      Phys.Rev. C48, 2395 (1993)

E.Oset, D.Strottman, H.Toki, J.Navarro

Core Polarization Phenomena in Pion-Nucleus Charge-Exchange Reactions Above the Delta Resonance

NUCLEAR REACTIONS 14C(π+, π0), E=250-650 MeV; calculated σ(θ)=0°. 14C, 42Ca, 18O(π+, π-), E=400 MeV; calculated σ(θ). Microscopic, parameter free Glauber approach.

doi: 10.1103/PhysRevC.48.2395
Citations: PlumX Metrics


1992GO16      Nucl.Phys. A549, 125 (1992)

J.M.G.Gomez, C.Prieto, J.Navarro

Improved Skyrme Forces for Hartree-Fock Seniority Calculations

NUCLEAR STRUCTURE 16O, 40,48Ca, 90Zr, 208Pb; calculated Hartree-Fock binding energies, proton radii. 41,42,43,44,45,46,47,48Ca; calculated neutron separation energies. Hartree-Fock seniority calculations, improved Skyrme forces.

doi: 10.1016/0375-9474(92)90070-Z
Citations: PlumX Metrics


1990CH12      Nucl.Phys. A510, 573 (1990); Errata Nucl.Phys. A514, 749 (1990)

H.C.Chiang, E.Oset, R.C.Carrasco, J.Nieves, J.Navarro

Inclusive Radiative Pion Capture in Nuclei

NUCLEAR STRUCTURE A=6-209; calculated radiative pion capture widths. 6,7Li, 9Be, 10,11B, 12,13C, 14N, 16,18O, 19F, 40Ca, 209Bi; calculated radiative pion capture branching ratios. Many-body approach, Pauli blocking, medium polarization.

ATOMIC PHYSICS, Mesic-Atoms A=6-209; calculated radiative pion capture widths. 6,7Li, 9Be, 10,11B, 12,13C, 14N, 16,18O, 19F, 40Ca, 209Bi; calculated radiative pion capture branching ratios. Many-body approach, Pauli blocking, medium polarization.

doi: 10.1016/0375-9474(90)90349-Q
Citations: PlumX Metrics


1990GA04      Nucl.Phys. A507, 385 (1990)

C.Garcia-Recio, H.Krivine, V.G.Nguyen, J.Navarro

The Thomas-Fermi Method and Polarizability of Nuclei

NUCLEAR STRUCTURE 12C, 48,40Ca, 56Fe; calculated M1 sum rule. Constrained Thomas-Fermi method.

doi: 10.1016/0375-9474(90)90299-2
Citations: PlumX Metrics


1990GA25      Z.Phys. A337, 261 (1990)

F.Garcias, M.Barranco, J.Navarro, E.Suraud

High Temperature Giant Dipole and Isoscalar Resonances

NUCLEAR STRUCTURE 63Cu, 90Zr, 114Sn, 140Ce, 160Er, 208Pb; calculated GDR energy vs temperature. Semi-classical approximation, RPA sum rules.


1990RO04      Phys.Lett. 236B, 393 (1990)

F.Roig, J.Navarro

Radiative Muon Capture and the Value of g(P) in Nuclei

NUCLEAR REACTIONS 12C, 16O, 40Ca(μ-, γ), E at rest; analyzed γ yield data; deduced g(P). RPA sum rules.

doi: 10.1016/0370-2693(90)90371-C
Citations: PlumX Metrics


1989GA09      Phys.Lett. 222B, 329 (1989)

C.Garcia-Recio, M.J.Lopez, J.Navarro, F.Roig

Pionic Distortion Factors for Radiative Pion Capture Studies

NUCLEAR REACTIONS 6Li, 10B, 12C, 14N, 16O, 40Ca(π, γ), E at rest; calculated total branching ratio distortion factors.

ATOMIC PHYSICS, Mesic-Atoms 6Li, 10B, 12C, 14N, 16O, 40Ca(π, γ), E at rest; calculated pionic atom distortion factors.

doi: 10.1016/0370-2693(89)90317-1
Citations: PlumX Metrics


1989NA01      Phys.Rev. C39, 302 (1989)

J.Navarro, F.Roig

Some Relations for Radiative-Pion-Capture and Muon-Capture Rates

NUCLEAR REACTIONS 6Li, 10B, 12C, 14N, 16O(μ-, γ), (π, γ), E at rest; calculated radiative capture rate ratios.

doi: 10.1103/PhysRevC.39.302
Citations: PlumX Metrics


1989NA22      Nucl.Phys. A505, 173 (1989)

J.Navarro, M.Barranco

The Dipole Isovector M3 Sum Rule in the Random Phase Approximation

NUCLEAR STRUCTURE 16O, 40Ca, 60Ni, 90Zr, 114Sn, 140Ce, 208Pb; calculated M3 dipole isovector sum rule contributions. RPA, Skyrme interactions.

doi: 10.1016/0375-9474(89)90369-2
Citations: PlumX Metrics


1988KR09      Nucl.Phys. A481, 781 (1988)

H.Krivine, E.Lipparini, J.Navarro, F.Roig

RPA Correlation Effects in Radiative Pion Capture

NUCLEAR REACTIONS 16O, 40Ca(π, γ), E at rest; calculated radiative capture rates, γ-branching ratios.

doi: 10.1016/0375-9474(88)90725-7
Citations: PlumX Metrics


1987NA04      Nucl.Phys. A465, 628 (1987)

J.Navarro, F.Roig

Sum Rule Approach to Radiative Pion Capture: A full hamiltonian calculation for 1p shell nuclei

NUCLEAR REACTIONS 6Li, 10B, 12C, 14N, 16O(π, γ), E at rest; calculated radiative capture rates, branching ratios. Sum rule approach.

doi: 10.1016/0375-9474(87)90558-6
Citations: PlumX Metrics


1986KR06      Phys.Lett. 171B, 331 (1986)

H.Krivine, J.Navarro

Calculation of the Nuclear Electric Polarizability

NUCLEAR STRUCTURE 16O, 40Ca, 90Zr, 208Pb; calculated electric polarizability. Hydrodynamical hamiltonian.

doi: 10.1016/0370-2693(86)91414-0
Citations: PlumX Metrics


1986NA14      Nucl.Phys. A457, 731 (1986)

J.Navarro, H.Krivine

A Sum Rule Approach to Total Muon Capture Rates

NUCLEAR STRUCTURE 16O, 40Ca; calculated total muon capture rate. Sum rule approach.

doi: 10.1016/0375-9474(86)90477-X
Citations: PlumX Metrics


1985BA15      Phys.Lett. 154B, 96 (1985)

M.Barranco, A.Polls, S.Marcos, J.Navarro, J.Treiner

The Excited Dipole Resonance: A finite-temperature sum rule approach

NUCLEAR STRUCTURE 40Ca, 78Kr, 127Cs, 144Gd, 208Pb; calculated GDR energy, width evolution vs excitation energy. Finite temperature sum rule approach.

doi: 10.1016/0370-2693(85)90565-9
Citations: PlumX Metrics


1985RO17      Nucl.Phys. A440, 659 (1985)

F.Roig, J.Navarro

Inclusive Radiative Pion Capture by N = Z Nuclei in the 1p Shell

NUCLEAR REACTIONS 6Li(π, γX), E at rest; calculated inclusive radiative pion capture rate; deduced total branching ratios, mean Eγ. Sum rule technique.

doi: 10.1016/0375-9474(85)90401-4
Citations: PlumX Metrics


1984BA41      Phys.Lett. 143B, 19 (1984)

J.L.Ballot, M.Fabre de la Ripelle, J.Navarro

Contribution of Two-Body Correlation to the Wave Function of Many-Body Systems

NUCLEAR STRUCTURE 4He, 16O, 40Ca; calculated levels, binding energy; deduced two-body correlation role. Polynomial expansion technique.

doi: 10.1016/0370-2693(84)90796-2
Citations: PlumX Metrics


1982NA01      Nucl.Phys. A375, 361 (1982)

J.Navarro, J.Bernabeu, J.M.G.Gomez, J.Martorell

Total Muon Capture Rates for N = Z Nuclei in the 1p Shell

NUCLEAR STRUCTURE 6Li, 10B, 12C, 14N, 16O; calculated levels, total muon capture rates. Sum rule techniques, Cohen-Kurath effective interactions.

doi: 10.1016/0375-9474(82)90019-7
Citations: PlumX Metrics


1979RI16      Ann.Phys.(New York) 123, 185 (1979)

M.F.de la Ripelle, J.Navarro

The First Order of the Hyperspherical Harmonic Expansion Method

NUCLEAR STRUCTURE 4He, 16O, 40Ca, 56Ni, 90Zr, 208Pb; calculated ground state energies, charge radii. Hyperspherical harmonic expansion method.

doi: 10.1016/0003-4916(79)90270-7
Citations: PlumX Metrics


1976NA10      Phys.Lett. 62B, 22 (1976)

J.Navarro

Hyperspherical Calculations with Skyrme-Like Forces

NUCLEAR STRUCTURE 4He, 16O, 40Ca, 56Ni, 90Zr, 208Pb; calculated ground state, breathing modes.

doi: 10.1016/0370-2693(76)90037-X
Citations: PlumX Metrics


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