NSR Query Results

Output year order : Descending
Format : Normal

NSR database version of April 26, 2024.

Search: Author = D.Bianco

Found 14 matches.

Back to query form

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
Citations: PlumX Metrics

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, ^{116,124,130,132}Sn; calculated neutron single-particle spectra, B(E1), strength functions. HFB, comparison with available data.

doi: 10.1088/0954-3899/41/2/025109
Citations: PlumX Metrics

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
Citations: PlumX Metrics
Data from this article have been entered in the XUNDL database. For more information, click here.

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, ^{134,136,138,140}Te, ^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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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). ^132,133,134Xe calculated low-energy states energy, J, π, γ transitions. ¹³⁰Xe calculated energy spectrum. Compared to data.

doi: 10.1088/1742-6596/366/1/012004
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics