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NSR database version of May 10, 2024.

Search: Author = D.Bianco

Found 14 matches.

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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 36Ar nuclei produced via the 24Mg + 12C reaction

NUCLEAR REACTIONS 12C(24Mg, X)36Ar, 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
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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 16,18,20,22O, 116,124,130,132Sn; calculated neutron single-particle spectra, B(E1), strength functions. HFB, comparison with available data.

doi: 10.1088/0954-3899/41/2/025109
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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 48Ti, 64Zn(140Nd, 140Nd'), E=399 MeV; measured Eγ, Iγ, (particle)γ-coin, yields using RILIS source and Miniball array at REX-ISOLDE-CERN facility. 140Nd; deduced E2 and diagonal matrix elements, B(E2) and Q2 for first 2+ state from Coulomb excitation. 48Ti, 64Zn, 140Sm; 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
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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 134Sn, 134,136,138,140Te, 136,138,140Xe; 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
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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 16O; 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
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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 132Te, 134Xe, 136Ba, 138Ce, 140Nd, 142Sm; 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
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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 126,128,130,132Te; 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
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2012BI12      Phys.Rev. C 86, 044327 (2012)

D.Bianco, F.Knapp, N.Lo Iudice, F.Andreozzi, A.Porrino, P.Vesely

Electric dipole response in 208Pb within a new microscopic multiphonon approach

NUCLEAR STRUCTURE 208Pb; 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
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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 130,131,132,133,134Xe; calculated level energy, B(E2), B(M1). 132,133,134Xe calculated low-energy states energy, J, π, γ transitions. 130Xe calculated energy spectrum. Compared to data.

doi: 10.1088/1742-6596/366/1/012004
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2012KN03      J.Phys.:Conf.Ser. 337, 012028 (2012)

F.Knapp, D.Bianco, N.Lo Iudice, F.Andreozzi, A.Porrino

Multiphonon nuclear response in 16O: A microscopic treatment equivalent to shell model

NUCLEAR STRUCTURE 16O; calculated energy levels, γ E1 strength distribution using multiphonon states built on Tamm-Dancoff phonons.

doi: 10.1088/1742-6596/337/1/012028
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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
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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 130,132,134Xe; calculated levels, J, B(E2), B(M1). New matrix diagonalization algorithm, shell model calculations. Comparison with experimental data.

doi: 10.1103/PhysRevC.84.024310
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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 128Te; calculated low-lying states E, J, π, B(E2) using large-scale shell model.

doi: 10.1088/1742-6596/312/9/092018
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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 48Cr, 110Sn; 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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