NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = J.Retamosa Found 29 matches. 2012MU15 J.Phys.:Conf.Ser. 381, 012031 (2012) L.Munoz, C.Fernandez-Ramirez, A.Relano, J.Retamosa Chaos in hadrons
doi: 10.1088/1742-6596/381/1/012031
2005MO19 Phys.Rev. C 71, 064317 (2005) R.A.Molina, A.P.Zuker, A.Relano, J.Retamosa Spectral statistics of Hamiltonian matrices in tridiagonal form
doi: 10.1103/PhysRevC.71.064317
2004GO30 Phys.Rev. C 69, 057302 (2004) J.M.G.Gomez, K.Kar, V.K.B.Kota, R.A.Molina, J.Retamosa Number of principal components and localization length in E2 and M1 transition strengths in 46V NUCLEAR STRUCTURE 46V; calculated E2 and M1 transition strengths, number of principal components. Embedded Gaussian orthogonal random matrix ensemble.
doi: 10.1103/PhysRevC.69.057302
2003GO16 Phys.Lett. B 567, 251 (2003) J.M.G.Gomez, K.Kar, V.K.B.Kota, R.A.Molina, J.Retamosa Localization in 2p1f nuclear shell-model wavefunctions NUCLEAR STRUCTURE 48,50,52Ca, 46,48,50Sc, 46Ti; calculated localization lengths for shell-model wavefunctions; deduced isospin dependence in onset of nuclear chaos. Embedded Gaussian orthogonal ensemble.
doi: 10.1016/j.physletb.2003.06.041
2001GO37 Phys.Rev. C64, 034305 (2001) J.M.G.Gomez, K.Kar, V.K.B.Kota, J.Retamosa, R.Sahu Transition Strengths and Quantum Chaos in Large Shell-Model Spaces NUCLEAR STRUCTURE 36Ne, 36Na, 36Mg, 46Ti, 48,52Sc; calculated E2, M1, and Gamow-Teller transition strength sums vs excitation energy. Shell model, comparison with embedded Gaussian orthogonal ensemble predictions.
doi: 10.1103/PhysRevC.64.034305
2001MO01 Phys.Rev. C63, 014311 (2001) R.A.Molina, J.M.G.Gomez, J.Retamosa Energy and Isospin Dependence of Nuclear Chaos NUCLEAR STRUCTURE 46,48,50,52Ca, 46,48,50,52Sc, 46Ti; calculated level spacing distributions; deduced isospin dependence for nuclear chaoticity. Shell model.
doi: 10.1103/PhysRevC.63.014311
2000GO14 Phys.Lett. 480B, 245 (2000) J.M.G.Gomez, K.Kar, V.R.Manfredi, R.A.Molina, J.Retamosa Statistical Theory versus Shell Model in a Large pf Configuration Space NUCLEAR STRUCTURE 46V, 50Sc; calculated transition strength distributions. Comparison of shell model, statistical model.
doi: 10.1016/S0370-2693(00)00414-7
1999CA12 Phys.Rev. C59, 2033 (1999) E.Caurier, G.Martinez-Pinedo, F.Nowacki, A.Poves, J.Retamosa, A.P.Zuker Full 0(h-bar)ω Shell Model Calculation of the Binding Energies of the 1f7/2 Nuclei NUCLEAR STRUCTURE 42,43,44,45,46,47,48Ca, 42,43,44,45,46,47,48,49Sc, 42,43,44,45,46,47,48,49,50Ti, 43,44,45,46,47,48,49,50,51V, 44,45,46,47,48,49,50,51,52Cr, 45,46,47,48,49,50,51Mn, 46,47,48,49,50,51,52,54Fe, 48,49,50,51,54Co, 50,51,52,54,56Ni; calculated binding energies, M1, E2, Gamow-Teller sum rules. Shell model, quasispin formalism.
doi: 10.1103/PhysRevC.59.2033
1999CA60 Nucl.Phys. (Supplement) A654, 747c (1999) E.Caurier, F.Nowacki, A.P.Zuker, G.Martinez-Pinedo, A.Poves, J.Retamosa Large Scale Diagonalizations in the pf Shell: Achievements and perspectives NUCLEAR STRUCTURE 48,50Cr; calculated levels, J, π. Shell model, comparison with data and with Hartree-Fock-Bogolyubov results. 58,60Ni; calculated level densities vs excitation energy. Shell model, comparison with data.
doi: 10.1016/S0375-9474(00)88541-3
1999CA62 Nucl.Phys. (Supplement) A654, 973c (1999) E.Caurier, F.Nowacki, A.Poves, J.Retamosa Shell Model Study of the Neutrinoless Double Beta Decays RADIOACTIVITY 48Ca, 76Ge, 82Se, 124Sn, 128,130Te, 136Xe(2β-); calculated 2ν-accompanied 2β-decay T1/2, 0ν-accomanied 2β-decay matrix elements. Large-scale shell model calculations.
doi: 10.1016/S0375-9474(00)88583-8
1999KO48 Phys.Rev. C60, 051306 (1999) V.K.B.Kota, R.Sahu, K.Kar, J.M.G.Gomez, J.Retamosa Transition Strength Sums and Quantum Chaos
doi: 10.1103/PhysRevC.60.051306
1998CA40 Phys.Rev. C58, 2033 (1998) E.Caurier, F.Nowacki, A.Poves, J.Retamosa Shell Model Study of the Neutron Rich Isotopes from Oxygen to Silicon NUCLEAR STRUCTURE Z=8-13; calculated neutron-rich nuclei 2+ levels, B(E2), one-, two-neutron separation energies, intruder states features. Shell model calculations.
doi: 10.1103/PhysRevC.58.2033
1998VO12 Phys.Lett. 443B, 1 (1998) P.von Neumann-Cosel, A.Poves, J.Retamosa, A.Richter Magnetic Dipole Response in Nuclei at the N = 28 Shell Closure: A new look NUCLEAR STRUCTURE 48Ca, 50Ti, 52Cr, 54Fe; calculated magnetic dipole response, B(M1) distributions; deduced spin quenching factors. Shell-model calculations.
doi: 10.1016/S0370-2693(98)01298-2
1997RE04 Phys.Rev. C55, 1266 (1997) J.Retamosa, E.Caurier, F.Nowacki, A.Poves Shell Model Study of the Neutron-Rich Nuclei Around N = 28 NUCLEAR STRUCTURE 40,41,42K, 42,39,40,41Ar, 38Cl; calculated levels. 44,46Ar, 38,40,42,44S; calculated total Gamow-Teller strength, B(λ) in some cases, β-decay T1/2. Z=14-20; N=16-30; calculated two-neutron separation energies. 40,42S deduced deformation β. 36,38,40,42,44Si, 38,40,42,44,46S, 40,42,44,46,48Ar, 42,44,46,48,50Ca, 44,46,48,50,52Ti, 46,48,50,52,54Cr; calculated 2+ levels. Shell model.
doi: 10.1103/PhysRevC.55.1266
1996CA35 Phys.Rev.Lett. 77, 1954 (1996) E.Caurier, F.Nowacki, A.Poves, J.Retamosa Shell Model Studies of the Double Beta Decays of 76Ge, 82Se, and 136Xe RADIOACTIVITY 76Ge, 82Se, 136Xe(2β); calculated 0ν-accompanied 2β-decay T1/2 lower limits. Large shell model space.
doi: 10.1103/PhysRevLett.77.1954
1996MA56 Phys.Rev. C54, R2150 (1996) G.Martinez-Pinedo, A.Poves, L.M.Robledo, E.Caurier, F.Nowacki, J.Retamosa, A.Zuker Backbending in 50Cr NUCLEAR STRUCTURE 50Cr; analyzed collective yrast, high-spin states; deduced backbending features. Spherical shell model, cranked HFB method.
doi: 10.1103/PhysRevC.54.R2150
1996RA21 Phys.Rev.Lett. 76, 2642 (1996) P.B.Radha, D.J.Dean, S.E.Koonin, T.T.S.Kuo, K.Langanke, A.Poves, J.Retamosa, P.Vogel Shell Model Monte Carlo Method for Two-Neutrino Double Beta Decay NUCLEAR STRUCTURE 48Ca, 76Ge(2β); calculated 2ν-accompanied 2β-decay matrix element vs temperature. Shell model Monte Carlo techniques.
doi: 10.1103/PhysRevLett.76.2642
1995CA33 Phys.Rev.Lett. 75, 2466 (1995) E.Caurier, J.L.Egido, G.Martinez-Pinedo, A.Poves, J.Retamosa, L.M.Robledo, A.P.Zuker Intrinsic vs Laboratory Frame Description of the Deformed Nucleus 48Cr NUCLEAR STRUCTURE 48Cr; calculated levels, g vs spin, B(E2), intrinsic quadrupole moment. Spherical shell model, HFB method.
doi: 10.1103/PhysRevLett.75.2466
1995RE01 Phys.Rev. C51, 371 (1995) J.Retamosa, E.Caurier, F.Nowacki Neutrinoless Double Beta Decay of 48Ca RADIOACTIVITY 48Ca(2β); calculated 0ν-accompanied 2β-decay T1/2. Shell model, recoil terms in hadronic currents.
doi: 10.1103/PhysRevC.51.371
1995ZU02 Phys.Rev. C52, R1741 (1995) A.P.Zuker, J.Retamosa, A.Poves, E.Caurier Spherical Shell Model Description of Rotational Motion NUCLEAR STRUCTURE 152,154,156,158Nd, 154,156,158,160Sm, 156,158,160,162Gd, 158,160,162,164Dy; calculated B(E2). Spherical shell model.
doi: 10.1103/PhysRevC.52.R1741
1994PO05 Nucl.Phys. A571, 221 (1994) Theoretical Study of the Very Neutron-Rich Nuclei Around N = 20 NUCLEAR STRUCTURE 28O, 34Si, 30Ne, 32Mg; calculated intruder levels, B(λ), quadrupole moments. 27,28,29,30O, 28,29,30,31F, 29,30,31,32Ne, 30,31,32,33Na, 31,32,33,34Mg, 32,33,34,35Al, 33,34,35,36Si; calculated levels, binding energies. Shell model.
doi: 10.1016/0375-9474(94)90058-2
1994PO34 Z.Phys. A347, 227 (1994) A.Poves, J.Retamosa, M.J.G.Borge, O.Tengblad Halo Signals in the Beta Decay of 28O RADIOACTIVITY 28O(β-); calculated Gamow-Teller β-decay strength function. Shell model.
doi: 10.1007/BF01289788
1993KL02 Phys.Rev. C47, 2502 (1993) G.Klotz, P.Baumann, M.Bounajma, A.Huck, A.Knipper, G.Walter, G.Marguier, C.Richard-Serre, A.Poves, J.Retamosa Beta Decay of 31,32Na and 31Mg: Study of the N = 20 shell closure RADIOACTIVITY 31,32Na, 31Mg(β-n) [from U(p, X), E=600 MeV]; measured Eγ, Iγ, γγ-, nγ-coin, Iβ; deduced log ft. 31,32Mg, 31Al deduced levels, J, π. 32Al deduced γ-cascade evidence.
doi: 10.1103/PhysRevC.47.2502
1992TE03 Z.Phys. A342, 303 (1992) O.Tengblad, M.J.G.Borge, L.Johannsen, B.Jonson, M.Lindroos, T.Nilsson, G.Nyman, A.Poves, H.L.Ravn, J.Retamosa, K.Riisager, P.Sona, K.Wilhelmsen, and the ISOLDE Collaboration Study of Neutron Rich Neon Isotopes RADIOACTIVITY 26,27,28,29Ne(β-n) [from Th(3He, X), E=910 MeV]; measured Iβ, T1/2, neutron emission probabilities. Shell model analysis.
doi: 10.1007/BF01291514
1991DU05 Phys.Rev. C44, 2872 (1991) J.Dukelsky, A.Poves, J.Retamosa Phase Transitions in Light Nuclei NUCLEAR STRUCTURE 20Ne; calculated intrinsic quadrupole moment expectation value, specific heat vs temperature; deduced phase transition features. SU(3) Elliott model.
doi: 10.1103/PhysRevC.44.2872
1990RE06 Nucl.Phys. A511, 221 (1990) J.Retamosa, J.M.Udias, A.Poves, E.Moya de Guerra 1+ Excitations in Light Nuclei: SU(3) versus realistic shell model results NUCLEAR STRUCTURE 20,22Ne, 24Mg, 44Ti; calculated levels, B(λ), form factor. Shell model.
doi: 10.1016/0375-9474(90)90157-H
1989BA50 Phys.Lett. 228B, 458 (1989) P.Baumann, A.Huck, G.Klotz, A.Knipper, G.Walter, G.Marguier, H.L.Ravn, C.Richard-Serre, A.Poves, J.Retamosa 34Si: A new doubly magic nucleus ( Question ) RADIOACTIVITY 34Al(β-) [from U(p, X), E=600 MeV]; measured βγγ-coin, Eγ, Iγ; deduced log ft, neutron emission probability. 34Al level deduced J, π. 34Si deduced levels, J, π, γ-branching ratios.
doi: 10.1016/0370-2693(89)90974-X
1989PO04 Phys.Rev. C39, 1639 (1989) A.Poves, J.Retamosa, E.Moya de Guerra Shell-Model Realization of the Scissors Mode NUCLEAR STRUCTURE 20Ne; calculated levels, B(M1), quadrupole moment ratio. Realistic shell model, SU(3) limit.
doi: 10.1103/PhysRevC.39.1639
1987PO01 Phys.Lett. 184B, 311 (1987) The Onset of Deformation at the N = 20 Neutron Shell Closure far from Stability NUCLEAR STRUCTURE 20,21O, 20,21F, 18,19,20,21,22Ne, 18,19,20,21,22Na, 18,19,20,21,22Mg, 20,21Al, 20,21Si; calculated ground state spins, percentages, centroid, correlation energies; 30Ne, 32Mg; calculated yrast states energies, J, π, B(E2); Na, Mg; calculated binding energies; 31Na, 32Mg; calculated levels, J, π; deduced deformation onset mass dependence. Shell model.
doi: 10.1016/0370-2693(87)90171-7
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