NSR Query Results
Output year order : Descending NSR database version of May 10, 2024. Search: Author = D.Bianco Found 14 matches. 2023DI03 Phys.Rev. C 107, 024615 (2023) A.Di Nitto, E.Vardaci, F.Davide, G.La Rana, M.Ashaduzzaman, D.Mercogliano, P.A.Setaro, T.Banerjee, A.Vanzanella, D.Bianco, M.Cinausero, N.Gelli, F.Loffredo, M.Quarto Clustering effects in ^{36}Ar nuclei produced via the ^{24}Mg + ^{12}C reaction NUCLEAR REACTIONS ^{12}C(^{24}Mg, X)^{36}Ar, E=91.72 MeV; measured Eα, Iα, Ep, Ip, evaporation residues (ER), ER Time-of-Flight, (ER)α-coin; deduced spectra and angular distributions of outgoing particles. Comparison to statistical model, rotating liquid drop model and cranked cluster model predictions. Pointed out signature of the formation of a long-lived orbiting-like dinuclear system at high excitation energies (40-60 MeV) from light-particle emission studies of α-like nuclei. Ball of 8πLP consisting of 125 ΔE-E Si-CsI telescope coupled to an PPAC evaporation residue detector tandem accelerator of Laboratori Nazionli di Legnaro (LNL).
doi: 10.1103/PhysRevC.107.024615
2014BI01 J.Phys.(London) G41, 025109 (2014) D.Bianco, F.Knapp, N.Lo Iudice, P.Vesely, F.Andreozzi, G.De Gregorio, A.Porrino A self-consistent study of multipole response in neutron-rich nuclei using a modified realistic potential NUCLEAR STRUCTURE ^{16,18,20,22}O, ^{116,124,130,132}Sn; calculated neutron single-particle spectra, B(E1), strength functions. HFB, comparison with available data.
doi: 10.1088/0954-3899/41/2/025109
2013BA38 Phys.Rev. C 88, 021302 (2013) C.Bauer, G.Rainovski, N.Pietralla, D.Bianco, A.Blazhev, T.Bloch, S.Bonig, A.Damyanova, M.Danchev, K.A.Gladnishki, T.Kroll, J.Leske, N.Lo Iudice, T.Moller, K.Moschner, J.Pakarinen, P.Reiter, M.Scheck, M.Seidlitz, B.Siebeck, C.Stahl, R.Stegmann, T.Stora, Ch.Stoyanov, D.Tarpanov, M.J.Vermeulen, D.Voulot, N.Warr, F.Wenander, V.Werner, H.De Witte Local suppression of collectivity in the N=80 isotones at the Z=58 subshell closure NUCLEAR REACTIONS ^{48}Ti, ^{64}Zn(^{140}Nd, ^{140}Nd'), E=399 MeV; measured Eγ, Iγ, (particle)γ-coin, yields using RILIS source and Miniball array at REX-ISOLDE-CERN facility. ^{140}Nd; deduced E2 and diagonal matrix elements, B(E2) and Q_{2} for first 2+ state from Coulomb excitation. ^{48}Ti, ^{64}Zn, ^{140}Sm; measured Eγ for first 2+ states. Comparison with shell-model and QPM calculations. Systematics of B(E2) values for first 2+ states in even-even N=80, Z=50-60 nuclei.
doi: 10.1103/PhysRevC.88.021302
2013BI08 Phys.Rev. C 88, 024303 (2013) D.Bianco, N.Lo Iudice, F.Andreozzi, A.Porrino, F.Knapp Spectroscopy of neutron-rich Te and Xe isotopes within a new shell model context NUCLEAR STRUCTURE ^{134}Sn, ^{134,136,138,140}Te, ^{136,138,140}Xe; calculated levels, J, π, B(E2), B(M1); deduced collectivity, neutron-proton symmetry. Large-scale shell model calculation based on an iterative matrix diagonalization algorithm. Comparison with experimental data. Systematics of energies and B(E2) values of first 2+ states in even-even A=126-140 Te and A=132-140 Xe nuclei.
doi: 10.1103/PhysRevC.88.024303
2012BI01 Phys.Rev. C 85, 014313 (2012) D.Bianco, F.Knapp, N.Lo Iudice, F.Andreozzi, A.Porrino Upgraded formulation of the nuclear eigenvalue problem in a microscopic multiphonon basis NUCLEAR STRUCTURE ^{16}O; calculated E1 strength function and cross section, isoscalar E2 reduced strength, phonon structure of 0+, 1- and 2+ states. Equation of motion method; eigenvalue problem in multiphonon space in terms of Tamm-Dancoff phonons, and Nilsson or Hartree-Fock basis. Comparison with experimental data.
doi: 10.1103/PhysRevC.85.014313
2012BI04 Phys.Rev. C 85, 034332 (2012) D.Bianco, F.Andreozzi, N.Lo Iudice, A.Porrino, F.Knapp Importance-sampling diagonalization algorithm for large-scale shell model calculations on N=80 isotones NUCLEAR STRUCTURE ^{132}Te, ^{134}Xe, ^{136}Ba, ^{138}Ce, ^{140}Nd, ^{142}Sm; calculated levels, J, π, B(E2), B(M1), mixed symmetry states. Iterative matrix diagonalization algorithm with an importance sampling, convergence properties. Comparison with experimental data, other shell-model calculations, and systematics of lowest 2+ states in N=80 isotones.
doi: 10.1103/PhysRevC.85.034332
2012BI11 Phys.Rev. C 86, 044325 (2012) D.Bianco, N.Lo Iudice, F.Andreozzi, A.Porrino, F.Knapp Mixed-symmetry states in Te isotopes within a large-scale shell model approach NUCLEAR STRUCTURE ^{126,128,130,132}Te; calculated levels, B(E2), B(M1), using large-scale shell model calculations with a new diagonalization algorithm. Mixed symmetry states. Comparison with experimental data.
doi: 10.1103/PhysRevC.86.044325
2012BI12 Phys.Rev. C 86, 044327 (2012) D.Bianco, F.Knapp, N.Lo Iudice, F.Andreozzi, A.Porrino, P.Vesely Electric dipole response in ^{208}Pb within a new microscopic multiphonon approach NUCLEAR STRUCTURE ^{208}Pb; calculated dipole resonances, E1 σ(ω), B(E1) for giant and pygmy dipole resonances (GDR and PDR) using the microscopic multiphonon approach with a new equation of motion phonon method. Comparison with experimental data.
doi: 10.1103/PhysRevC.86.044327
2012BI17 J.Phys.:Conf.Ser. 366, 012004 (2012) D.Bianco, F.Andreozzi, N.Lo Iudice, A.Porrino, F.Knapp Complex nuclear spectra in a large scale shell model approach NUCLEAR STRUCTURE ^{130,131,132,133,134}Xe; calculated level energy, B(E2), B(M1). ^{132,133,134}Xe calculated low-energy states energy, J, π, γ transitions. ^{130}Xe calculated energy spectrum. Compared to data.
doi: 10.1088/1742-6596/366/1/012004
2012KN03 J.Phys.:Conf.Ser. 337, 012028 (2012) F.Knapp, D.Bianco, N.Lo Iudice, F.Andreozzi, A.Porrino Multiphonon nuclear response in ^{16}O: A microscopic treatment equivalent to shell model NUCLEAR STRUCTURE ^{16}O; calculated energy levels, γ E1 strength distribution using multiphonon states built on Tamm-Dancoff phonons.
doi: 10.1088/1742-6596/337/1/012028
2012LO17 J.Phys.:Conf.Ser. 366, 012031 (2012) N.Lo Iudice, D.Bianco, F.Knapp, F.Andreozzi, A.Porrino, P.Vesely Multiphonon Approaches to Complex Spectroscopy
doi: 10.1088/1742-6596/366/1/012031
2011BI07 Phys.Rev. C 84, 024310 (2011) D.Bianco, F.Andreozzi, N.Lo Iudice, A.Porrino, F.Knapp Matrix diagonalization algorithm and its applicability to the nuclear shell model NUCLEAR STRUCTURE ^{130,132,134}Xe; calculated levels, J, B(E2), B(M1). New matrix diagonalization algorithm, shell model calculations. Comparison with experimental data.
doi: 10.1103/PhysRevC.84.024310
2011BI11 J.Phys.:Conf.Ser. 312, 092018 (2011) D.Bianco, F.Andreozzi, N.Lo Iudice, A.Porrino, F.Knapp A new algorithm for large scale shell model calculations and its applicability to medium-heavy and neutron rich nuclei NUCLEAR STRUCTURE ^{128}Te; calculated low-lying states E, J, π, B(E2) using large-scale shell model.
doi: 10.1088/1742-6596/312/9/092018
2010BI16 J.Phys.:Conf.Ser. 205, 012002 (2010) D.Bianco, F.Andreozzi, N.Lo Iudice, A.Porrino, S.Dimitrova An upgraded version of an importance sampling algorithm for large scale shell model calculations NUCLEAR STRUCTURE ^{48}Cr, ^{110}Sn; calculated specified levels, J, π using large scale shell model with sampling iterative algorithm.
doi: 10.1088/1742-6596/205/1/012002
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