NSR Query Results
Output year order : Descending NSR database version of May 3, 2024. Search: Author = J.Navarro Found 62 matches. 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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
2014NA33 Nucl.Data Sheets 118, 571 (2014) 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
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
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
2013NA07 Phys.Rev. C 87, 044329 (2013) Spin instabilities of infinite nuclear matter and effective tensor interactions
doi: 10.1103/PhysRevC.87.044329
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
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
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
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
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
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
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
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
2001GU19 Nucl.Phys. A689, 499c (2001) Description of Strongly Interacting Systems by Means of Jastrow and Configuration Interaction Correlated Wave Functions
doi: 10.1016/S0375-9474(01)00890-9
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
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
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
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
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
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
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
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
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
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
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
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
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
1996NA20 J.Phys.(London) G22, 1363 (1996) Extended Thomas-Fermi Expansion from Nuclear Linear Response
doi: 10.1088/0954-3899/22/9/009
1993GU14 Acta Phys.Pol. B24, 525 (1993) 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
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
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
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
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) 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
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
1989NA01 Phys.Rev. C39, 302 (1989) 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
1989NA22 Nucl.Phys. A505, 173 (1989) 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
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
1987NA04 Nucl.Phys. A465, 628 (1987) 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
1986KR06 Phys.Lett. 171B, 331 (1986) 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
1986NA14 Nucl.Phys. A457, 731 (1986) 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
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
1985RO17 Nucl.Phys. A440, 659 (1985) 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
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
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
1979RI16 Ann.Phys.(New York) 123, 185 (1979) 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
1976NA10 Phys.Lett. 62B, 22 (1976) 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
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