NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = A.Molinari Found 77 matches. 2014NA36 Nucl.Phys. A932, 134c (2014) M.Nardi, W.Alberico, A.Beraudo, A.De Pace, A.Molinari, M.Monteno, F.Prino, M.Sitta A transport set-up for heavy-flavour observables in nucleus-nucleus collisions at RHIC and LHC
doi: 10.1016/j.nuclphysa.2014.07.022
2013AL16 Nucl.Phys. 910-911, 395c (2013) W.M.Alberico, A.Beraudo, A.De Pace, A.Molinari, M.Monteno, M.Nardi, F.Prino Heavy flavor production in pp and AA collisions at the LHC
doi: 10.1016/j.nuclphysa.2012.12.066
2011BE15 Nucl.Phys. A855, 404c (2011) A.Beraudo, W.M.Alberico, A.De Pace, A.Molinari, M.Monteno, M.Nardi, F.Prino Heavy quark dynamics in the QGP: RAA and ν2 from RHIC to LHC
doi: 10.1016/j.nuclphysa.2011.02.091
2011BE45 Phys.Rev. C 84, 054315 (2011) D.Berardo, M.B.Barbaro, R.Cenni, T.W.Donnelly, A.Molinari Connecting scaling with short-range correlations
doi: 10.1103/PhysRevC.84.054315
2011DE08 Nucl.Phys. A849, 15 (2011) A.De Pace, A.Molinari, H.A.Weidenmuller Spreading widths of doorway states
doi: 10.1016/j.nuclphysa.2010.10.004
2009BA55 Phys.Rev. C 80, 064320 (2009) M.B.Barbaro, D.Berardo, R.Cenni, T.W.Donnelly, A.Molinari Fermion propagators in space-time
doi: 10.1103/PhysRevC.80.064320
2009BE48 Nucl.Phys. A831, 59 (2009) A.Beraudo, A.De Pace, W.M.Alberico, A.Molinari Transport properties and Langevin dynamics of heavy quarks and quarkonia in the Quark Gluon Plasma
doi: 10.1016/j.nuclphysa.2009.09.002
2008AL38 Eur.Phys.J. A 38, 97 (2008) W.M.Alberico, S.Chiacchiera, H.Hansen, A.Molinari, M.Nardi Shear viscosity and entropy of quark matter
doi: 10.1140/epja/i2008-10648-8
2008BA33 Phys.Rev. C 78, 024602 (2008) M.B.Barbaro, R.Cenni, T.W.Donnelly, A.Molinari Model for BCS-type correlations in superscaling
doi: 10.1103/PhysRevC.78.024602
2007AL46 Nucl.Phys. A792, 152 (2007) W.M.Alberico, A.Beraudo, A.Czerska, P.Czerski, A.Molinari Meson screening masses in the interacting QCD plasma
doi: 10.1016/j.nuclphysa.2007.04.019
2006AL17 Nucl.Phys. A775, 188 (2006) W.M.Alberico, A.Beraudo, P.Czerski, A.Molinari Finite momentum meson correlation functions in a QCD plasma
doi: 10.1016/j.nuclphysa.2006.06.006
2006BA17 Nucl.Phys. B(Proc.Supp.) S155, 257 (2006) M.B.Barbaro, J.E.Amaro, J.A.Caballero, T.W.Donnelly, A.Molinari, I.Sick Superscaling and Charge-changing Neutrino Cross Sections NUCLEAR REACTIONS 12C(ν, μ-), E at 1000 MeV/c; calculated σ(E, θ).
doi: 10.1016/j.nuclphysbps.2006.02.065
2006MO13 Phys.Lett. B 637, 48 (2006) Nuclear masses, chaos, and the residual interaction
doi: 10.1016/j.physletb.2006.04.025
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
2005AM03 Phys.Rev. C 71, 015501 (2005) J.E.Amaro, M.B.Barbaro, J.A.Caballero, T.W.Donnelly, A.Molinari, I.Sick Using electron scattering superscaling to predict charge-changing neutrino cross sections in nuclei NUCLEAR REACTIONS 12C(e, e'), E=1.3, 1.5 GeV; 16O(e, e'), E=0.88 GeV; analyzed σ(E, θ); deduced electromagnetic response. 12C(ν, μ), E=1 GeV; calculated σ(E, θ). Superscaling analysis.
doi: 10.1103/PhysRevC.71.015501
2004BA82 Phys.Rev. C 70, 034309 (2004) M.B.Barbaro, A.Molinari, F.Palumbo, M.R.Quaglia Goldstone bosons in the pairing Hamiltonian: The path integral approach
doi: 10.1103/PhysRevC.70.034309
2004BB01 Eur.Phys.J. A 22, 377 (2004) M.B.Barbaro, R.Cenni, A.Molinari, M.R.Quaglia The many levels pairing Hamiltonian for two pairs
doi: 10.1140/epja/i2004-10043-7
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
2004MO46 Phys.Lett. B 601, 119 (2004) Statistical fluctuations of ground-state energies and binding energies in nuclei NUCLEAR STRUCTURE A=20-250; analyzed ground-state energy and binding energy fluctuations. Perturbation theory, supersymmetry.
doi: 10.1016/j.physletb.2004.09.042
2003AL20 Nucl.Phys. A724, 157 (2003) L.Alvarez-Ruso, M.B.Barbaro, T.W.Donnelly, A.Molinari Nuclear response functions for the N-N*(1440) transition NUCLEAR REACTIONS 12C(e, e'X), E=high; calculated parity-conserving and parity-violating response functions for resonance production.
doi: 10.1016/S0375-9474(03)01480-5
2003AM05 Nucl.Phys. A723, 181 (2003) J.E.Amaro, M.B.Barbaro, J.A.Caballero, T.W.Donnelly, A.Molinari Delta-isobar relativistic meson exchange currents in quasielastic electron scattering
doi: 10.1016/S0375-9474(03)01269-7
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
2002AM01 Nucl.Phys. A697, 388 (2002) J.E.Amaro, M.B.Barbaro, J.A.Caballero, T.W.Donnelly, A.Molinari Relativistic Pionic Effects in Quasielastic Electron Scattering NUCLEAR REACTIONS 40Ca(e, e'), E not given; calculated transverse and longitudinal response functions; deduced reaction mechanism features.
doi: 10.1016/S0375-9474(01)01253-2
2002AM09 Eur.Phys.J. A 15, 421 (2002) J.E.Amaro, M.B.Barbaro, J.A.Caballero, T.W.Donnelly, A.Molinari Momentum distribution of relativistic nuclei with Hartree-Fock mesonic correlations
doi: 10.1140/epja/i2002-10080-2
2002AM12 Phys.Rep. 368, 317 (2002) J.E.Amaro, M.B.Barbaro, J.A.Caballero, T.W.Donnelly, A.Molinari Gauge and Lorentz invariant one-pion exchange currents in electron scattering from a relativistic Fermi gas
doi: 10.1016/S0370-1573(02)00195-3
2002BA88 Phys.Rev. C66, 034310 (2002) M.Barbaro, R.Cenni, A.Molinari, M.R.Quaglia Analytic Solution of the Pairing Problem: One pair in many levels NUCLEAR STRUCTURE 210Pb; calculated level energies, collective energy vs pair strength. Analytical pairing solution.
doi: 10.1103/PhysRevC.66.034310
2002CZ01 Phys.Rev. C65, 044317 (2002) P.Czerski, A.De Pace, A.Molinari Revisiting the Hugenholtz-Van Hove Theorem in Nuclear Matter
doi: 10.1103/PhysRevC.65.044317
2002DE47 Ann.Phys.(New York) 296, 263 (2002) Statistical Theory of the Many-Body Nuclear System
doi: 10.1006/aphy.2001.6205
2001AL05 Phys.Lett. 497B, 214 (2001) L.Alvarez-Ruso, M.B.Barbaro, T.W.Donnelly, A.Molinari Influence of Nucleonic Motion in Relativistic Fermi Gas Inclusive Responses NUCLEAR STRUCTURE 12C; calculated response functions for electron scattering. Relativistic Fermi gas.
doi: 10.1016/S0370-2693(00)01332-0
2001AM04 Nucl.Phys. A690, 509 (2001) P.Amore, R.Cenni, T.W.Donnelly, A.Molinari Constrasting N → Δ and N → N Parity-Violating Asymmetries in Nuclei
doi: 10.1016/S0375-9474(00)00706-5
2001BA56 Phys.Rev. C64, 011302 (2001) M.B.Barbaro, L.Fortunato, A.Molinari, M.R.Quaglia Pairing Hamiltonian for One Pair of Identical Nucleons Bound in a Potential Well
doi: 10.1103/PhysRevC.64.011302
1999AM10 Nucl.Phys. A657, 161 (1999) J.E.Amaro, M.B.Barbaro, J.A.Caballero, T.W.Donnelly, A.Molinari Relativistic Effects in Electromagnetic Nuclear Responses in the Quasi-Elastic Delta Region NUCLEAR REACTIONS 1H(e, e'), E(cm)=1100-1400 MeV; calculated transverse σ. 12C(e, e'X), E=620, 1108 MeV; calculated σ(θ), electromagnetic response functions; deduced resonance role. Relativistic Fermi Gas model.
doi: 10.1016/S0375-9474(99)00334-6
1999DE48 Ann.Phys.(New York) 278, 109 (1999) A.De Pace, H.Feshbach, A.Molinari Ground State Energy Fluctuations in Nuclear Matter, II
doi: 10.1006/aphy.1999.5958
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
1998AM11 Nucl.Phys. A643, 349 (1998) J.E.Amaro, M.B.Barbaro, J.A.Caballero, T.W.Donnelly, A.Molinari Relativistic Effects in Electromagnetic Meson-Exchange Currents for One-Particle Emission Reactions
doi: 10.1016/S0375-9474(98)00569-7
1998BA94 Nucl.Phys. A643, 137 (1998) M.B.Barbaro, R.Cenni, A.De Pace, T.W.Donnelly, A.Molinari Relativistic y-Scaling and the Coulomb Sum Rule in Nuclei
doi: 10.1016/S0375-9474(98)00443-6
1997AM01 Nucl.Phys. A615, 353 (1997) P.Amore, R.Cenni, T.W.Donnelly, A.Molinari On the Coulomb and Higher-Order Sum Rules in the Relativistic Fermi Gas
doi: 10.1016/S0375-9474(97)00028-6
1997CE05 Phys.Rev. C56, 276 (1997) R.Cenni, T.W.Donnelly, A.Molinari Relativistic Electromagnetic Charge Response: Finite versus infinite systems, exclusive versus inclusive processes NUCLEAR STRUCTURE 16O, 40Ca, 90Zr, 140Yb; calculated longitudinal reduced responses, normalized Coulomb, energy-weighted sum rules. Relativistic PWIA.
doi: 10.1103/PhysRevC.56.276
1996BA07 Nucl.Phys. A596, 553 (1996) M.B.Barbaro, A.De Pace, T.W.Donnelly, A.Molinari The Charge Response of a Meson-Correlated Relativistic Fermi Gas
doi: 10.1016/0375-9474(95)00424-6
1996BA09 Nucl.Phys. A598, 503 (1996) M.B.Barbaro, A.De Pace, T.W.Donnelly, A.Molinari Parity-Violating Longitudinal Response NUCLEAR REACTIONS 12C(e, e'X), E not given; calculated longitudinal quasielastic parity-violating response. Anti-symmetrized RPA-HF correlations, relativistic Fermi gas basis.
doi: 10.1016/S0375-9474(96)00010-3
1996BA59 Phys.Rev. C54, 1954 (1996) M.B.Barbaro, A.De Pace, T.W.Donnelly, A.Molinari, M.J.Musolf Probing Nucleon Strangeness with Neutrinos: Nuclear model dependences
doi: 10.1103/PhysRevC.54.1954
1994BA14 Nucl.Phys. A569, 701 (1994) M.B.Barbaro, A.De Pace, T.W.Donnelly, A.Molinari Parity-Violating Electron Scattering from the Pion-Correlated Relativistic Fermi Gas
doi: 10.1016/0375-9474(94)90381-6
1994CE05 Nuovo Cim. 107A, 407 (1994) R.Cenni, A.Molinari, G.Vagradov On the Relativistic Description of the Nucleus
doi: 10.1007/BF02831445
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
1983MO19 Nuovo Cim. 76A, 406 (1983) Mesonic Effects in the Nuclear Response NUCLEAR STRUCTURE 56Fe, 12C; analyzed nuclear response characteristics; deduced spin-longitudinal, spin-transverse component differences. Meson effects, inelastic electron scattering data input.
doi: 10.1007/BF02833736
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
1982AL32 Z.Phys. A309, 143 (1982) 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
1975BR17 Phys.Lett. 57B, 113 (1975) R.A.Broglia, A.Molinari, G.Pollarolo, T.Regge Band Hybridization in Rotational Motion NUCLEAR STRUCTURE 156Dy; calculated backbending, band hybridization.
doi: 10.1016/0370-2693(75)90002-7
1975CA14 Nuovo Cim. 27A, 60 (1975) M.Carbone, R.Cenni, R.Malvano, A.Molinari Asymmetry in the Photonucleon Angular Distributions NUCLEAR REACTIONS 209Pb(γ, n), 209Bi(γ, p), E=21-31 MeV; calculated σ(E, θ).
doi: 10.1007/BF02785266
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
1974BR21 Phys.Lett. 50B, 295 (1974) R.A.Broglia, A.Molinari, G.Pollarolo, T.Regge On the Back-Bending in the Rotational Motion NUCLEAR STRUCTURE 154Gd; calculated B(E2), levels.
doi: 10.1016/0370-2693(74)90672-8
1972MO30 Phys.Lett. 41B, 93 (1972) Rotational Motion at Large Angular Momentum in Even-Even Deformed Nuclei NUCLEAR STRUCTURE 162Er; calculated levels, rotational bands at high angular momentum. Band hybridization.
doi: 10.1016/0370-2693(72)90434-0
1971BE47 Ann.Phys.(N.Y.) 63, 393 (1971) Nonstatic Second Order Contribution to the Elastic Electron-Nucleus Scattering NUCLEAR REACTIONS 40Ca(e, e), E=757 MeV; calculated σ(θ). Nonstatic 2nd-order corrections.
doi: 10.1016/0003-4916(71)90019-4
1971BR53 Phys.Lett. 36B, 297 (1971) Isovector Potential in 208Pb from Partial Muon Capture NUCLEAR STRUCTURE 208Pb; calculated isovector potential.
doi: 10.1016/0370-2693(71)90707-6
1970BE21 Nucl.Phys. A148, 87 (1970) Correlation Effect on Unique Forbidden Decays RADIOACTIVITY 17N, 39Ar, 41Ca; calculated hindrance in nuclear matrix elements for unique first-forbidden transitions.
doi: 10.1016/0375-9474(70)90614-7
1969BR06 Nucl.Phys. A127, 429 (1969); Erratum Nucl.Phys. A139, 710 (1969) R.Broglia, J.Damgard, A.Molinari Particle-Vibration Coupling in 209Bi NUCLEAR STRUCTURE 209Bi; calculated levels.
doi: 10.1016/0375-9474(69)90583-1
1968BL01 Nucl.Phys. A106, 545 (1968) Collective 0- Vibrations in Even Spherical Nuclei with Tensor Forces
doi: 10.1016/0375-9474(68)90515-0
1968BR06 Nucl.Phys. A109, 353 (1968) R.A.Broglia, A.Molinari, B.Sorensen Spin Vibrational 1+ States in 208Pb NUCLEAR STRUCTURE 208Pb; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0375-9474(68)90599-X
1968DA18 Nucl.Phys. A121, 625 (1968) J.Damgaard, V.V.Gortchakov, G.M.Vagradov, A.Molinari Monopole States in 40Ca NUCLEAR STRUCTURE 40Ca; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0375-9474(68)90112-7
1964CI02 Nuovo Cimento, Suppl. 2, 57 (1964) Diffusione Elastica ed Anelastica di Eletroni da Nuclei Complessi
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