NSR Query Results
Output year order : Descending NSR database version of May 3, 2024. Search: Author = X.Campi Found 23 matches. 2005CA21 Phys.Rev. C 71, 041601 (2005) X.Campi, H.Krivine, E.Plagnol, N.Sator Partial energy fluctuations and negative heat capacities
doi: 10.1103/PhysRevC.71.041601
2005CA49 Phys.Rev. C 72, 057602 (2005) Zipf's law in multifragmentation
doi: 10.1103/PhysRevC.72.057602
2003CA15 Phys.Rev. C 67, 044610 (2003) X.Campi, H.Krivine, E.Plagnol, N.Sator "Little big bang" scenario of multifragmentation
doi: 10.1103/PhysRevC.67.044610
2001CA08 Nucl.Phys. A681, 458c (2001) Clustering and Thermodynamics in Small Systems
doi: 10.1016/S0375-9474(00)00553-4
1997CA24 Nucl.Phys. A620, 46 (1997) Clustering in Supercritical Nuclear Matter: A lattice-gas approach
doi: 10.1016/S0375-9474(97)00162-0
1996CA37 Phys.Lett. 385B, 1 (1996) Examining Some Aspects of the Nuclear Caloric Curve NUCLEAR STRUCTURE 6,7Li; analyzed caloric curve for these fragments; deduced liquid-gas phase transition observation related features.
doi: 10.1016/0370-2693(96)00839-8
1995CA17 Nucl.Phys. A589, 505 (1995) Fluctuations and Intermittency in Fragment Size Distributions
doi: 10.1016/0375-9474(95)00190-C
1994CA30 Phys.Rev. C50, R2680 (1994) Size and Excitation Energy Distributions of Projectile Spectators in Multifragmentation Data NUCLEAR REACTIONS Cu(197Au, X), E=600 MeV/nucleon; analyzed data; deduced spectators size, energy distributions characteristics correct interpretation. Abrasion, BUU models.
doi: 10.1103/PhysRevC.50.R2680
1989CA12 Nucl.Phys. A495, 259c (1989) Finite Size Scaling in Nuclear Fragmentation NUCLEAR REACTIONS Ag, Cu, C, 27Al, 197Au(p, X), E not given; calculated fragment production σ vs mass; deduced finite size scaling role.
doi: 10.1016/0375-9474(89)90324-2
1982MO20 Nucl.Phys. A388, 525 (1982) F.H.Molzahn, M.Kohno, D.W.L.Sprung, X.Campi The Local Fermi Momentum and Effective Nuclear Interactions NUCLEAR STRUCTURE 16O, 40,48Ca, 56Ni, 90Zr, 132Sn, 140Ce, 208Pb; calculated charge radius, nucleon binding energy, incompressibility, nucleon removal energies. 40Ca, 208Pb; calculated charge density. Hartree-Fock method, local Fermi momentum approximation, Skyrme type effective interactions.
doi: 10.1016/0375-9474(82)90475-4
1980CA23 Phys.Rev. C22, 2605 (1980) Calculation of Binding Energies and Isotope Shifts in a Long Series of Rubidium Isotopes NUCLEAR STRUCTURE 76,78,80,82,84,86,88,90,92,94,96,98,100,102,104,106Sr, 75,77,79,81,83,85,87,89,91,93,95,97,99,101,103,105Rb, 74,76,78,80,82,84,86,88,90,92,94,96,98,100,102,104Kr; calculated binding energies, rms charge radii, two-neutron separation energies. Density dependent Hartree-Fock, Skyrme interaction.
doi: 10.1103/PhysRevC.22.2605
1979BR21 Phys.Lett. 86B, 141 (1979) Determination of Matter Densities of Ca Isotopes by 600 MeV and 1 GeV Proton Elastic Scattering NUCLEAR REACTIONS 40,42,44,48Ca(p, p), E=600 MeV, 1 GeV; measured nothing; analyzed scattering data; 48Ca, 40Ca deduced neutron density difference. Matter distribution. Glauber model, fourier series expansion method.
doi: 10.1016/0370-2693(79)90803-7
1979SP03 Nucl.Phys. A325, 125 (1979) D.W.L.Sprung, M.Vallieres, X.Campi, J.Martorell The Charge Density of 58Ni NUCLEAR STRUCTURE 58Ni; calculated charge density; analyzed electron-scattering data. Friar-Negele method.
doi: 10.1016/0375-9474(79)90157-X
1978CA04 Phys.Lett. 73B, 263 (1978) A Simple Approximation for the Nuclear Density Matrix NUCLEAR STRUCTURE 4He, 16O, 40Ca; calculated Coulomb exchange energies.
doi: 10.1016/0370-2693(78)90509-9
1976BO37 Phys.Lett. 64B, 381 (1976) O.Bohigas, X.Campi, H.Krivine, J.Treiner Extensions of the Thomas-Fermi Approximation for Finite Nuclei NUCLEAR STRUCTURE 40Ca, 90Zr, 208Pb; calculated proton, neutron radii.
doi: 10.1016/0370-2693(76)90101-5
1976SP11 Nucl.Phys. A268, 301 (1976) D.W.L.Sprung, J.Martorell, X.Campi 'Model Independent' Determination of the Charge Density Difference between 209Bi and 208Pb NUCLEAR STRUCTURE 209Bi, 208Pb; calculated isotone shift, charge density.
doi: 10.1016/0375-9474(76)90464-4
1975CA27 Nucl.Phys. A251, 193 (1975) X.Campi, H.Flocard, A.K.Kerman, S.Koonin Shape Transition in the Neutron Rich Sodium Isotopes NUCLEAR STRUCTURE 19,20,21,22,23,24,25,26,27,28,29,30,31,32,33,34,35Na; calculated single particle energies, quadrupole moments, β.
doi: 10.1016/0375-9474(75)90065-2
1975SP08 Nucl.Phys. A253, 1 (1975) D.W.L.Sprung, M.Vallieres, X.Campi, C.-M.Ko A Note on the Validity of the Density Matrix Expansion NUCLEAR STRUCTURE 16O, 40Ca, 90Zr, 208Pb; calculated level density, force parameters. 48Ca; calculated force parameters.
doi: 10.1016/0375-9474(75)90117-7
1974CA10 Nucl.Phys. A223, 541 (1974) X.Campi, D.W.L.Sprung, J.Martorell Isotope Effects in Tin with the Local Density Approximation NUCLEAR STRUCTURE 100,102,104,106,108,110,112,114,116,118,120,122Sn, 124,126,128,130,132Sn; calculated binding energies, S(p), S(n).
doi: 10.1016/0375-9474(74)90705-2
1973CA28 Phys.Lett. 46B, 291 (1973) Possible Bubble Nuclei - 36Ar and 200Hg NUCLEAR STRUCTURE 36Ar, 200Hg; calculated charge density.
doi: 10.1016/0370-2693(73)90121-4
1973MA39 Phys.Lett. 46B, 296 (1973) Self Consistent Description of the Nuclear Monopole Polarization in Muonic 208Pb NUCLEAR STRUCTURE 208Pb; calculated monopole part of nuclear polarization energy.
doi: 10.1016/0370-2693(73)90122-6
1972CA23 Nucl.Phys. A194, 401 (1972) Spherical Nuclei in the Local Density Approximation NUCLEAR STRUCTURE 4He, 16O, 40,48Ca, 90Zr, 208Pb; calculated binding energies, radii, single-particle energies. Hartree-Fock theory, density-dependent effective interaction.
doi: 10.1016/0375-9474(72)91046-9
1972CA40 Phys.Lett. 41B, 443 (1972) X.Campi, J.Martorell, D.W.L.Sprung Form Factor of 4He in the Local Density Approximation NUCLEAR REACTIONS 4He(e, e), E not given; calculated form factors. Local density approximation.
doi: 10.1016/0370-2693(72)90670-3
Back to query form |