Nuclear Science References (NSR)

NUCLEAR STRUCTURE ⁵He, ¹¹B, ¹²C; calculated proton angular distributions, related parameters for nonmesonic weak decay of polarized hypernuclei; deduced final state interaction effects.

doi: 10.1103/PhysRevLett.94.082501
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2005AL11 Nucl.Phys. A750, 359 (2005)

W.M.Alberico, A.Beraudo, A.Molinari

Meson correlation functions in a QCD plasma

doi: 10.1016/j.nuclphysa.2004.12.070
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2004AL19 Acta Phys.Pol. B35, 929 (2004)

W.M.Alberico

Weak Non-Mesonic Decay of Hypernuclei

2004DE36 Nucl.Phys. A741, 249 (2004)

A.De Pace, M.Nardi, W.M.Alberico, T.W.Donnelly, A.Molinari

Role of 2p-2h MEC excitations in superscaling

NUCLEAR REACTIONS ¹²C, ¹⁹⁷Au(e, e'X), E=3595, 4045 MeV; analyzed scaling functions, meson exchange current contributions.

doi: 10.1016/j.nuclphysa.2004.06.014
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2003AL05 Eur.Phys.J. A 16, 221 (2003)

W.M.Alberico, F.Giacosa, M.Nardi, C.Ratti

Baryonic masses based on the NJL model

doi: 10.1140/epja/i2002-10088-6
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2003DE23 Nucl.Phys. A726, 303 (2003)

A.De Pace, M.Nardi, W.M.Alberico, T.W.Donnelly, A.Molinari

The 2p-2h electromagnetic response in the quasielastic peak and beyond

doi: 10.1016/S0375-9474(03)01625-7
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2002AL03 Phys.Rep. 358, 227 (2002)

W.M.Alberico, S.M.Bilenky, C.Maieron

Strangeness in the Nucleon: Neutrino-Nucleon and Polarized Electron-Nucleon Scattering

doi: 10.1016/S0370-1573(01)00058-8
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2002AL16 Nucl.Phys. A706, 143 (2002)

W.M.Alberico, A.Drago, C.Ratti

Stability of Strange Quark Matter: MIT bag versus color dielectric model

doi: 10.1016/S0375-9474(02)00680-2
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2002AL22 Phys.Rep. 369, 1 (2002)

W.M.Alberico, G.Garbarino

Weak decay of Λ-hypernuclei

doi: 10.1016/S0370-1573(02)00199-0
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2001AL08 Nucl.Phys. A680, 94c (2001)

W.M.Alberico, A.Lavagno, P.Quarati

Non-Extensive Statistics Effects in Quark-Gluon Plasma and in Relativistic Heavy-Ion Collisions

NUCLEAR REACTIONS S(S, X), Pb(Pb, X), E=high; calculated fragments transverse momentum distributions.

doi: 10.1016/S0375-9474(00)00396-1
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2001AL13 Astropart.Phys. 15, 211 (2001)

W.M.Alberico, S.M.Bilenky, W.Grimus

On a Possibility to Determine the S-Factor of the hep Process in Experiments with Thermal (Cold) Neutrons

NUCLEAR REACTIONS ³H(n, e), E=thermal; calculated σ. Implications for astrophysical reaction rates discussed.

doi: 10.1016/S0927-6505(00)00145-6
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2001AL35 Nucl.Phys. A691, 163c (2001)

W.M.Alberico

Two-Nucleon Induced Non-Mesonic Decay of Λ-Hypernuclei

NUCLEAR STRUCTURE ¹²C, ²⁸Si, ⁴⁰Ca, ⁵⁶Fe, ⁸⁹Y, ¹³⁹La, ²⁰⁸Pb; calculated hypernucleus decay rates.

doi: 10.1016/S0375-9474(01)01024-7
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2000AL01 Eur.Phys.J. C 12, 499 (2000)

W.M.Alberico, A.Lavagno, P.Quarati

Non-Extensive Statistics, Fluctuations and Correlations in High-Energy Nuclear Collisions

NUCLEAR REACTIONS ¹H(p, X), Pb(Pb, X), E=158 GeV/nucleon; analyzed pion correlations; deduced non-extensive statistical effects.

doi: 10.1007/s100529900220
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2000AL03 Nucl.Phys. A668, 113 (2000)

W.M.Alberico, A.De Pace, G.Garbarino, R.Cenni

Functional Appraoch to the Non-Mesonic Decay of Λ-Hypernuclei

doi: 10.1016/S0375-9474(99)00683-1
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2000AL08 Phys.Rev. C61, 044314 (2000)

W.M.Alberico, A.De Pace, G.Garbarino, A.Ramos

Weak Decays of Medium and Heavy Λ Hypernuclei

NUCLEAR STRUCTURE ¹²C, ²⁸Si, ⁴⁰Ca, ⁵⁶Fe, ⁸⁹Y, ¹³⁹La, ²⁰⁸Pb; calculated hypernucleus decay widths. Propagator method, local density approximation.

doi: 10.1103/PhysRevC.61.044314
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2000AL10 Phys.Lett. 478B, 208 (2000)

W.M.Alberico, J.Bernabeu, S.M.Bilenky, W.Grimus

Is It Possible to Determine the S-Factor of the hep Process from a Laboratory Experiment ?

NUCLEAR REACTIONS ⁴He(e, nν), E not given; ³He(p, e⁺ν), E not given; calculated relationship between σ of first reaction and S-factor for of second reaction.

doi: 10.1016/S0370-2693(00)00287-2
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2000AL16 Nucl.Phys. A663-664, 833c (2000)

W.M.Alberico, C.Giunti, S.M.Bilenky, C.Maieron

Neutrino (Antineutrino)-Nucleon Scattering and Strange Form Factors of the Nucleon

NUCLEAR REACTIONS ¹H(ν, ν), E not given; calculated σ ratios; deduced nucleon form factor contributions. Comparison with data.

doi: 10.1016/S0375-9474(99)00780-0
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2000AL27 Phys.Lett. 486B, 362 (2000)

W.M.Alberico, G.Garbarino

The ΔI = 1/2 Rule in Non-Mesonic Weak Decay of Λ-Hypernuclei

NUCLEAR STRUCTURE ⁴H, ^4,5He, ¹²C; analyzed hypernuclei non-mesonic decay data, ΔI=1/2 rule validity. Phenomenological model.

doi: 10.1016/S0370-2693(00)00766-8
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1999AL08 Eur.Phys.J. A 4, 195 (1999)

W.M.Alberico, P.Czerski, M.Nardi

Deconfinement Transition: A three dimensional model

doi: 10.1007/s100500050218
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1999AL16 Nucl.Phys. A651, 277 (1999)

W.M.Alberico, M.B.Barbaro, S.M.Bilenky, J.A.Caballero, C.Giunti, C.Maieron, E.Moya de Guerra, J.M.Udias

Strange Form Factors of the Proton: A new analysis of the ν(ν-bar) data of the BNL-734 experiment

doi: 10.1016/S0375-9474(99)00142-6
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1998AL13 Nucl.Phys. A634, 233 (1998)

W.M.Alberico, G.Chanfray, J.Delorme, M.Ericson, A.Molinari

The Semi-Classical Approach to the Exclusive Electron Scattering

doi: 10.1016/S0375-9474(98)00160-2
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1998AL28 Phys.Lett. 438B, 9 (1998)

W.M.Alberico, M.B.Barbaro, S.M.Bilenky, J.A.Caballero, C.Giunti, C.Maieron, E.Moya de Guerra, J.M.Udias

The Ratio of p and n Yields in NC ν(ν-bar) Nucleus Scattering and Strange Form Factors of the Nucleon

doi: 10.1016/S0370-2693(98)01043-0
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1997AL21 Nucl.Phys. A623, 471 (1997)

W.M.Alberico, M.B.Barbaro, S.M.Bilenky, J.A.Caballero, C.Giunti, C.Maieron, E.Moya de Guerra, J.M.Udias

Inelastic ν and (ν-bar) Scattering on Nuclei and ' Strangeness ' of the Nucleon

NUCLEAR REACTIONS ¹²C(ν, ν'X), (ν-bar, ν-bar'X), E=200-1000 GeV; calculated differential σ vs ejected nucleon energy, proton to neutron production ratio, asymmetry related quantity; deduced nucleon strangeness role. Shell, Fermi gas models.

doi: 10.1016/S0375-9474(97)00416-8
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1995AL13 Nucl.Phys. A589, 620 (1995)

W.M.Alberico, M.Nardi, S.Quattrocolo

Deconfinement Transition in a One-Dimensional Model at Finite Temperature

doi: 10.1016/0375-9474(95)00172-W
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1994AL03 Phys.Lett. 321B, 177 (1994)

W.M.Alberico, G.Gervino, A.Lavagno

Phenomenological Approach to Baryon Resonance Damping in Nuclei

NUCLEAR REACTIONS ⁹Be, C, ²³⁸U(γ, X), E=0.2-1.2 GeV; analyzed photoabsorption σ(E); deduced nuclear medium role on baryon resonance width. Resonance-hole model.

doi: 10.1016/0370-2693(94)90460-X
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1994AL12 Z.Phys. A348, 17 (1994)

W.M.Alberico, P.Czerski, A.De Pace, V.R.Manfredi

Collective Modes in a Slab of Interacting Nuclear Matter The Effects of Finite Range Interactions

doi: 10.1007/BF01291647
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1993AL07 Phys.Lett. 303B, 5 (1993)

W.M.Alberico, M.B.Barbaro, A.De Pace, A.Molinari

Parity-Violating Experiments Using the Quasi-Elastic Electron and Positron Scattering

NUCLEAR REACTIONS ¹²C(polarized e^-, e^-), (polarized e⁺, e⁺), E not given; calculated asymmetry vs energy transfer; deduced parity violation measurement feasibility conditions. Relativistic Fermi gas model.

doi: 10.1016/0370-2693(93)90034-F
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1993AL20 Nucl.Phys. A563, 605 (1993)

W.M.Alberico, M.B.Barbaro, A.De Pace, T.W.Donnelly, A.Molinari

The Pion in Electromagnetic and Weak Neutral-Current Nuclear Response Functions

NUCLEAR REACTIONS ¹²C(e, e'), E not given; calculated longitudinal, transverse response functions; deduced pionic correlations, meson exchange current role. Weak neutral current, Hartree-Fock, RPA, infinite order summation schemes.

doi: 10.1016/0375-9474(93)90057-5
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1993LA07 Nucl.Phys. A555, 237 (1993)

I.Laktineh, W.M.Alberico, J.Delorme, M.Ericson

Coherent Photoproduction of Neutral Pions in Nuclei as a Detector of Nuclear Pionic Modes

NUCLEAR REACTIONS ¹⁶O(π⁺, π⁺), (π^-, π^-), E=303 MeV; calculated averaged σ(θ). ¹⁶O(π⁺, π⁺), (π^-, π^-), E ≈ 160-500 MeV; ¹²C(π⁺, π⁺), (π^-, π^-), E ≈ 200-500 MeV; calculated averaged σ(E). ⁴He, ¹²C, ¹⁶O(γ, π⁰); calculated σ(E). ¹²C(γ, π⁰), E=235 MeV; calculated σ(θ). Coherent production.

doi: 10.1016/0375-9474(93)90321-N
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1992DO05 Nucl.Phys. A541, 525 (1992)

T.W.Donnelly, M.J.Musolf, W.M.Alberico, M.B.Barbaro, A.De Pace, A.Molinari

Parity-Violating Quasielastic Electron Scattering

NUCLEAR REACTIONS ¹²C(e, e'X), E not given; calculated response functions, asymmetry. Parity-violating quasielastic electron scattering, relativistic Fermi gas model.

doi: 10.1016/0375-9474(92)90220-E
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1991AL02 Nucl.Phys. A523, 488 (1991)

W.M.Alberico, A.De Pace, M.Pignone

Neutron-Antineutron Oscillations in Nuclei

NUCLEAR STRUCTURE ¹⁶O, ⁴⁰Ca, ⁴⁰Ar; calculated n-(n-bar) oscillation time, medium effects dependent quantity T(R). Shell model.

doi: 10.1016/0375-9474(91)90032-2
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1991AL24 J.Phys.(London) G17, S81 (1991)

W.M.Alberico, A.De Pace

Second Order Effects in the Nuclear Response Functions

NUCLEAR REACTIONS ⁴⁰Ca(e, e'X), E not given; compiled, reviewed transverse, longitudinal response functions calculations; deduced 2p-2h states role. Perturbation theory, polarization propogator up to second order.

doi: 10.1088/0954-3899/17/S/008
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1990AL35 Phys.Rev.Lett. 65, 1845 (1990)

W.M.Alberico, R.Cenni, A.Molinari, P.Saracco

Dynamical Pion Propagation in the Functional Approach to the Charge Response

NUCLEAR STRUCTURE ⁴⁰Ca; calculated electromagnetic response function. Functional approach.

doi: 10.1103/PhysRevLett.65.1845
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1989AL28 Phys.Lett. 233B, 37 (1989)

W.M.Alberico, M.Ericson, A.Molinari, Z.-X.Wang

The Δ in the Nuclear Quasi-Elastic Peak

NUCLEAR STRUCTURE ⁴⁰Ca, ¹²C; calculated transverse response function. Quasielastic peak region, Δ degree of freedom.

doi: 10.1016/0370-2693(89)90611-4
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1988AL20 Phys.Rev. C38, 109 (1988)

W.M.Alberico, A.De Pace, M.Ericson, M.B.Johnson, A.Molinari

Spin-Isospin Nuclear Responses with Hadronic Probes

NUCLEAR REACTIONS ⁴⁰Ca(³He, t), E not given; calculated σ(θt, Et). RPA spin-isospin nuclear responses.

doi: 10.1103/PhysRevC.38.109
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1988AL34 Ann.Phys.(New York) 187, 79 (1988)

W.M.Alberico, M.B.Barbaro, A.Bottino, A.Molinari

The 2ν Double Beta Decay in Nuclear Matter

RADIOACTIVITY ⁷⁶Ge, ⁸²Se, ¹³⁰Te, ¹³⁶Xe(2β); calculated 2ν-accompanied decay Gamow-Teller matrix element.

doi: 10.1016/0003-4916(88)90281-3
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1987AL04 Phys.Lett. 183B, 135 (1987)

W.M.Alberico, A.De Pace, M.Ericson, M.B.Johnson, A.Molinari

Spin-Isospin Surface Responses

NUCLEAR REACTIONS Ca, Pb(p, p'), E=20-100 MeV; calculated spin-isospin longitudinal, transverse responses, free isovector response ratio. RPA calculations.

doi: 10.1016/0370-2693(87)90426-6
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1987AL05 Nucl.Phys. A462, 269 (1987)

W.M.Alberico, P.Czerski, M.Ericson, A.Molinari

Inclusive Charge Longitudinal Response in Finite Nuclei

NUCLEAR STRUCTURE ¹²C, ⁴⁰Ca, ⁵⁶Fe; calculated charge dynamic, static longitudinal structure factors. Semi-classical RPA theory.

doi: 10.1016/0375-9474(87)90548-3
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1987AL19 Europhys.Lett. 4, 415 (1987)

W.M.Alberico, M.B.Barbaro

On the Semi-Classical Charge Longitudinal Response in ¹²C and ⁴⁰Ca

NUCLEAR REACTIONS ¹²C, ⁴⁰Ca(e, e'), E not given; calculated charge longitudinal response functions. Semi-classical RPA.

doi: 10.1209/0295-5075/4/4/006
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1987AL24 Nucl.Phys. A475, 233 (1987)

W.M.Alberico, G.Chanfray, M.Ericson, A.Molinari

Proton and Neutron Contributions to the Charge Longitudinal Response

NUCLEAR STRUCTURE ¹²C, ^40,48Ca; calculated charge longitudinal response function; deduced p, n contributions, differences. RPA.

doi: 10.1016/0375-9474(87)90164-3
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1986AL13 Phys.Rev. C34, 977 (1986)

W.M.Alberico, A.Molinari, A.De Pace, M.Ericson, M.B.Johnson

Random Phase Approximation Spin-Isospin Nuclear Response in the Deep Inelastic Region

NUCLEAR REACTIONS ⁴⁰Ca(e, e'), E not given; calculated longitudinal response, transverse dynamic structure factors. RPA.

doi: 10.1103/PhysRevC.34.977
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1985AL10 Phys.Rev. C31, 2007 (1985)

W.M.Alberico, A.De Pace, A.Molinari

Spin Isovector Responses in Finite Nuclei

NUCLEAR REACTIONS ^40,48Ca, ⁵⁶Fe(e, e'), E at 330, 410 MeV/c; calculated transverse magnetic response function. RPA.

doi: 10.1103/PhysRevC.31.2007
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1985AL20 Phys.Rev. C32, 1722 (1985)

W.M.Alberico, A.Bottino, P.Czerski, A.Molinari

Double Proton Decay and H-H(bar) Oscillations

NUCLEAR STRUCTURE ¹⁶O, ⁵⁶Fe; calculated double proton-decay related nuclear effects; deduced hydrogen-antihydrogen oscillation time lower bound, effective Lagrangian coupling constant upper bound.

doi: 10.1103/PhysRevC.32.1722
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1985ST09 Phys.Lett. 156B, 291 (1985)

U.Stroth, R.W.Hasse, P.Schuck, W.M.Alberico, A.Molinari, M.Ericson

On the Nuclear Isovector Spin Response in the Quasielastic Peak Region

NUCLEAR REACTIONS ²⁰⁸Pb(p, p'), E not given; calculated longitudinal, transverse nuclear response. Nonlocal mean field plus particle-hole interactions.

NUCLEAR STRUCTURE ⁴⁰Ca; calculated structure function. ⁴⁸Ca, ¹²C; calculated transverse nuclear response function.

doi: 10.1016/0370-2693(85)91611-9
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1984AL04 Phys.Lett. 136B, 307 (1984)

W.M.Alberico, M.Ericson, A.Molinari

Unifying Photon and Pion Absorption

NUCLEAR REACTIONS ⁵⁶Fe(e, e'X), E not given; calculated transverse magnetic response function vs excitation. Deep inelastic inclusive reaction, meson exchange, nucleon-nucleon correlation, 2p-2h contribution.

doi: 10.1016/0370-2693(84)92009-4
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1984AL26 Nucl.Phys. A429, 445 (1984)

W.M.Alberico, J.Bernabeu, A.Bottino, A.Molinari

nn(bar) Mixing Inside Nuclei

NUCLEAR STRUCTURE ¹⁶O, ⁵⁶Fe; A=0-200; calculated binding energy per particle; deduced neutron-antineutron mixing, oscillation time.

doi: 10.1016/0375-9474(84)90691-2
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1984AL27 Phys.Rev. C30, 1776 (1984)

W.M.Alberico, M.Ericson, A.Molinari

Interpretation of the Polarization Transfer Measurement in the (p, p') Reaction on ²⁰⁸Pb

NUCLEAR STRUCTURE ⁴⁰Ca; calculated transverse magnetic response vs excitation energy. ^40,48Ca, ⁵⁶Fe; calculated transverse sum rule function; deduced inconclusivity of volume spin-isospin response nature derived from ²⁰⁸Pb(p, p') analysis.

doi: 10.1103/PhysRevC.30.1776
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1984AL28 Ann.Phys.(New York) 154, 356 (1984)

W.M.Alberico, M.Ericson, A.Molinari

The Role of Two Particle-Two Hole Excitations in the Spin-Isospin Nuclear Response

NUCLEAR REACTIONS ⁵⁶Fe(e, e'), E at 210-410 MeV/c; calculated transverse magnetic response function vs E(e'). ²⁰⁸Pb(γ, X), E ≈ 25-175 MeV; calculated quasideuteron component photoabsorption σ(E). Microscopic approach, meson exchange currents, nucleon-nucleon interactions.

doi: 10.1016/0003-4916(84)90155-6
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1982AL12 Nucl.Phys. A379, 429 (1982)

W.M.Alberico, M.Ericson, A.Molinari

Quenching and Hardening in the Transverse Quasi-Elastic Peak

NUCLEAR REACTIONS ⁵⁶Fe(e, e'), E=0.1-14 GeV; ¹²C(e, e'), E=120-560 MeV; calculated transverse magnetic response function; deduced quenching, hardening effects. RPA, particle-hole, isobar-hole interactions.

doi: 10.1016/0375-9474(82)90007-0
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1982AL32 Z.Phys. A309, 143 (1982)

W.M.Alberico, A.Molinari

Compton Scattering on ²⁰⁸Pb

NUCLEAR REACTIONS ²⁰⁸Pb(γ, γ), E=10-110 MeV; calculated σ(absorption), σ(θ) vs E, elastic, exchange form factors. Low energy theorem, Compton scattering.

doi: 10.1007/BF01414975
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1975MO01 Nucl.Phys. A239, 45 (1975)

A.Molinari, M.B.Johnson, H.A.Bethe, W.M.Alberico

Effective Two-Body Interaction in Simple Nuclear Spectra

NUCLEAR STRUCTURE ³⁴Cl, ³⁴S, ^90,92Nb, ^48,50Sc, ^208,210Bi, ²¹⁰Pb; calculated interaction matrix elements.

doi: 10.1016/0375-9474(75)91132-X
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