NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = E.Fabrici Found 32 matches. 2004BA23 Braz.J.Phys. 34, 897 (2004) G.Battistoni, M.Cavinato, F.Cerutti, A.Clivio, E.Fabrici, E.Gadioli, E.Gadioli Erba, M.V.Garzelli, A.Mairani, A.Empl, L.S.Pinsky, F.Ballarini, A.Ottolenghi, A.Fasso, A.Ferrari, J.Ranft, P.R.Sala Heavy Ion Interactions from Coulomb Barrier to Few GeV/n: Boltzmann Master Equation Theory and FLUKA Code Performances NUCLEAR REACTIONS 165Ho(20Ne, nX), E=11-30 MeV/nucleon; Al(Fe, nX), E=400 MeV/nucleon; calculated neutron spectra, σ(E, θ). 93Nb(16O, BX), E=400 MeV; calculated boron fragment spectra, σ(E, θ). Boltzmann master equation theory, comparison with data.
doi: 10.1590/s0103-97332004000500051
2004BB23 Braz.J.Phys. 34, 897 (2004) G.Battistoni, M.Cavinato, F.Cerutti, A.Clivio, E.Fabrici, E.Gadioli, E.Gadioli Erba, M.V.Garzelli, A.Mairani, A.Empl, L.S.Pinsky, F.Ballarini, A.Ottolenghi, A.Fasso, A.Ferrari, J.Ranft, P.R.Sala Heavy Ion Interactions from Coulomb Barrier to Few GeV/n: Boltzmann Master Equation Theory and FLUKA Code Performances NUCLEAR REACTIONS 165Ho(20Ne, nX), E=11-30 MeV/nucleon; Al(Fe, nX), E=400 MeV/nucleon; calculated neutron spectra, σ(E, θ). 93Nb(16O, BX), E=400 MeV; calculated boron fragment spectra, σ(E, θ). Boltzmann master equation theory, comparison with data.
doi: 10.1590/S0103-97332004000500051
2004BU09 Nucl.Phys. A734, 553 (2004) E.Z.Buthelezi, E.Gadioli, G.F.Steyn, F.Albertini, C.Birattari, M.Cavinato, F.Cerutti, S.H.Connell, A.A.Cowley, E.Fabrici, E.Gadioli Erba Incomplete fusion of projectile fragments in the interaction of 12C with 103Rh up to 33 MeV per nucleon NUCLEAR REACTIONS 103Rh(12C, X)105Ag/104Ag/101Pd/100Pd/102Rh/99Rh/97Ru/95Ru/95Tc/94Tc/93mMo/90Mo/90Nb/86Zr/87Y, E=70-400 MeV; analyzed excitation functions; deduced reaction mechanism features.
doi: 10.1016/j.nuclphysa.2004.01.103
2003BE62 Eur.Phys.J. A 18, 639 (2003) B.Becker, F.Albertini, E.Gadioli, G.F.Steyn, M.Cavinato, S.H.Connell, A.A.Cowley, E.Fabrici, S.V.Fortsch, E.Gadioli Erba, J.J.Lawrie, E.Sideras-Haddad Emission of Li, 7, 9Be and B fragments in the interaction of 12C with 93Nb between 200 and 400 MeV NUCLEAR REACTIONS 93Nb(12C, X), E=200-400 MeV; measured intermediate mass fragments σ(E, θ); deduced binary fragmentation contribution, other reaction mechanism features.
doi: 10.1140/epja/i2003-10091-5
2003GA15 Eur.Phys.J. A 17, 195 (2003) E.Gadioli, G.F.Steyn, F.Albertini, C.Birattari, M.Cavinato, S.H.Connell, A.A.Cowley, E.Fabrici, S.V.Fortsch, E.Gadioli Erba, J.J.Lawrie, M.Pigni, J.P.F.Sellschop, E.Sideras-Haddad Emission of intermediate-mass fragments in the interaction of 16O with 59Co, 93Nb and 197Au NUCLEAR REACTIONS 59Co, 93Nb, 197Au(16O, X), E=6-25 MeV/nucleon; measured intermediate mass fragment yields, spectra, σ(E, θ); deduced reaction mechanism features.
doi: 10.1140/epja/i2003-10007-5
2002GA32 Nucl.Phys. A708, 391 (2002) E.Gadioli, G.F.Steyn, C.Birattari, C.Catarisano, M.Cavinato, S.H.Connell, A.A.Cowley, E.Fabrici, S.V.Fortsch, E.Gadioli Erba, J.J.Lawrie, J.P.F.Sellschop, E.Sideras-Haddad Interplay of Mean Field and Nucleon-Nucleon Interactions in the Production of Carbon Fragments in 16O Induced Reactions at Incident Energies up to 25 MeV/amu NUCLEAR REACTIONS 59Co, 93Nb(16O, X), E=100, 250, 400 MeV; measured carbon fragments spectra, σ(θ); deduced projectile breakup and nucleon coalescence contributions.
doi: 10.1016/S0375-9474(02)01021-7
2002GA51 Acta Phys.Hung.N.S. 16, 359 (2002) E.Gadioli, G.F.Steyn, C.Birattari, C.Catarisano, M.Cavinato, S.H.Connell, E.Fabrici, S.V.Fortsch, E.Gadioli Erba, J.J.Lawrie, F.M.Nortier, J.P.F.Sellschop, E.Sideras-Haddad Nucleon Coalescence in the Interaction of 16O with 59Co at an Incident Energy of 250 MeV NUCLEAR REACTIONS 59Co(16O, X), E=250 MeV; measured intermediate mass fragment yields, energy and angular distributions; deduced nucleon coalescence, related reaction mechanism features.
doi: 10.1556/APH.16.2002.1-4.38
2001CA02 Nucl.Phys. A679, 753 (2001) M.Cavinato, E.Fabrici, E.Gadioli, E.Gadioli Erba, G.Riva Monte Carlo Calculations of Heavy Ion Cross-Sections Based on the Boltzmann Master Equation Theory NUCLEAR REACTIONS 165Ho(12C, X), E=25 MeV/nucleon; calculated Ep, En, σ(E, θ), fragment charge and mass distributions. 28Si(28Si, X), E=19.7 MeV/nucleon; calculated proton spectra, σ(E, θ). Ni, 92Mo, 122Sn(40Ar, X), E=26 MeV/nucleon; calculated neutron spectra, σ(E, θ). Monte Carlo calculations, coupled Boltzmann master equations. Comparisons with data.
doi: 10.1016/S0375-9474(00)00357-2
2001GA47 Eur.Phys.J. A 11, 161 (2001) E.Gadioli, G.F.Steyn, C.Birattari, M.Cavinato, S.H.Connell, A.A.Cowley, E.Fabrici, S.V.Fortsch, E.Gadioli Erba, J.J.Lawrie, F.M.Nortier, J.P.F.Sellschop, E.Sideras-Haddad Emission of 8Begs in the Interaction of 12C with Nuclei at Incident Energies up to 33 MeV/amu NUCLEAR REACTIONS 59Co, 93Nb, 197Au(12C, X), E=100-400 MeV; measured σ(θ) vs 8Be energy for 8Be emission, break-up and coalescence contributions. Breakup mechanisms discussed.
doi: 10.1007/s100500170082
2000GA39 Eur.Phys.J. A 8, 373 (2000) E.Gadioli, M.Cavinato, E.Fabrici, E.Gadioli Erba, R.Bassini, C.Birattari, S.Crippa, G.F.Steyn, S.V.Fortsch, J.J.Lawrie, F.M.Nortier, S.H.Connell, E.Sideras-Haddad, J.P.F.Sellschop, A.A.Cowley Evidence for a Dissipative Friction Mechanism Based on 8Be Fragments from the Interaction of 12C with 59Co NUCLEAR REACTIONS 59Co(12C, 8Be), E=8.3-33.3 MeV/nucleon; measured σ(θ), αα-coin. Effect of projectile break up discussed. Comparison with model predictions.
doi: 10.1007/s100500070089
1999GA39 Nucl.Phys. A654, 523 (1999) E.Gadioli, M.Cavinato, E.Fabrici, E.Gadioli Erba, C.Birattari, I.Mica, S.Solia, G.F.Steyn, S.V.Fortsch, J.J.Lawrie, F.M.Nortier, T.G.Stevens, S.H.Connell, J.P.F.Sellschop, A.A.Cowley Alpha Particle Emission in the Interaction of 12C with 59Co and 93Nb at Incident Energies of 300 and 400 MeV NUCLEAR REACTIONS 59Co, 93Nb(12C, αX), E=300, 400 MeV; measured α spectra, σ(Eα, θ); deduced reaction mechanism features.
doi: 10.1016/S0375-9474(00)88492-4
1998CA44 Nucl.Phys. A643, 15 (1998) M.Cavinato, E.Fabrici, E.Gadioli, E.Gadioli Erba, E.Risi Boltzmann Master Equation Theory of Angular Distributions in Heavy-Ion Reactions NUCLEAR REACTIONS 165Ho(20Ne, X), E=600 MeV; calculated neutron, alpha angular distributions. Ag(36S, X), (16O, X), E=30 MeV/nucleon; calculated light charged particles σ(E, θ). Ni, 92Mo, 122Sn(40Ar, X), E=26 MeV/nucleon; 165Ho(12C, X), E=25 MeV/nucleon; calculated σ(En, θ). Boltzmann master equation theory. Comparison with data.
doi: 10.1016/S0375-9474(98)00545-4
1998GA32 Acta Phys.Hung.N.S. 7, 275 (1998) E.Gadioli, C.Birattari, M.Cavinato, E.Fabrici, E.Gadioli Erba, V.Allori, G.Bello, F.Cerutti, A.Di Filippo, T.G.Stevens, S.H.Connell, J.P.F.Sellschop, F.M.Nortier, G.F.Steyn, C.Marchetta The Interaction of 12C and 16O with 103Rh NUCLEAR REACTIONS 103Rh(12C, X)113Sn/111In/110Sn/108In/105Ag/102Rh, E=50-400 MeV; 103Rh(16O, X)115Sb/113Sn/110Sn/111In/108In/105Ag/103Ag/101Pd/101Rh/100Rh/95Ru/94Tc, E=50-400 MeV; calculated excitation functions; deduced pre-equilibrium emission, other reaction mechanism features. Comparison with data.
1998GA36 Nucl.Phys. A641, 271 (1998) E.Gadioli, C.Birattari, M.Cavinato, E.Fabrici, E.Gadioli Erba, V.Allori, F.Cerutti, A.Di Filippo, S.Vailati, T.G.Stevens, S.H.Connell, J.P.F.Sellschop, F.M.Nortier, G.F.Steyn, C.Marchetta Angular Distributions and Forward Recoil Range Distributions of Residues Created in the Interaction of 12C and 16O Ions with 103Rh NUCLEAR REACTIONS 103Rh(12C, X), E=151, 228 MeV; measured residual nuclei angular distributions, yields; 103Rh(12C, X), E=402 MeV; 103Rh(16O, X), E=303 MeV; measured residual nudlei yields, recoil range distributions; deduced reaction mechanism features, incomplete fusion. Activation technique.
doi: 10.1016/S0375-9474(98)00472-2
1997CA34 Phys.Lett. 405B, 219 (1997) M.Cavinato, E.Fabrici, E.Gadioli, E.Gadioli Erba, E.Risi Ejectile Angular Distributions in Boltzmann Master Equation Theory of Nuclear Reactions NUCLEAR REACTIONS 165Ho(20Ne, X), E=220, 292, 402, 600 MeV; 197Au(36Ar, X), E=35 MeV/nucleon; analyzed α-, n-ejectile σ(θ, E). Boltzmann master equation theory.
doi: 10.1016/S0370-2693(97)00644-8
1997GA09 Phys.Lett. 394B, 29 (1997) E.Gadioli, C.Birattari, M.Cavinato, E.Fabrici, E.Gadioli Erba, V.Allori, C.Bovati, F.Cerutti, A.Di Filippo, E.Galbiati, T.G.Stevens, S.H.Connell, J.P.F.Sellschop, S.J.Mills, F.M.Nortier, G.F.Steyn, C.Marchetta Comprehensive Study of the Reactions Induced by 12C on 103Rh up to 33 MeV/nucleon NUCLEAR REACTIONS 103Rh(12C, X)113Sb/110In/108In/107In/111In/105Ag/104Ag/103Ag/102Ag/101Pd/100Pd/99Rh/98Rh/97Ru/96Tc/95Ru/94Tc/93Mo/93mMo/90Nb, E=45-400 MeV; measured residuals production σ(E). Activation technique.
doi: 10.1016/S0370-2693(97)00003-8
1996BI19 Phys.Rev. C54, 3051 (1996) C.Birattari, M.Bonardi, M.Cavinato, E.Fabrici, E.Gadioli, E.Gadioli Erba, F.Groppi, M.Bello, C.Bovati, A.Di Filippo, T.G.Stevens, S.H.Connell, J.P.F.Sellschop, S.J.Mills, F.M.Nortier, G.F.Steyn, C.Marchetta Preequilibrium Processes in the Fusion of 12C with 103Rh up to 20 MeV/nucleon NUCLEAR REACTIONS, ICPND 103Rh(12C, xnyp)113Sb/111Sn/110Sn/109Sn/108Sn/113Sn/111In/110In/110mIn, E=40-210 MeV; measured residuals production σ(E); deduced fusion σ, multiplicity of pre-equilibrium particles, mean-field interaction. Boltzmann master equation calculation.
doi: 10.1103/PhysRevC.54.3051
1996CA15 Phys.Lett. 382B, 1 (1996) M.Cavinato, E.Fabrici, E.Gadioli, E.Gadioli Erba, E.Galbiati Monte Carlo Calculations using the Boltzmann Master Equation Theory of Nuclear Reactions NUCLEAR REACTIONS 107Ag(16O, X), E=480 MeV; calculated mass, charge, excitation energy distributions after thermalization in fusion, angle integrated particle spectra. 165Ho(20Ne, X), E=220-600 MeV; calculated angle integrated neutron spectra. Boltzmann master equation, Monte Carlo calculations.
doi: 10.1016/0370-2693(96)00652-1
1995BR33 Z.Phys. A353, 57 (1995) C.Brusati, M.Cavinato, E.Fabrici, E.Gadioli, E.Gadioli Erba Nuclear Surface, Mean Field and Isospin Effects in Boltzmann Master Equation Theory of Pre-Equilibrium Reactions NUCLEAR STRUCTURE 16O, 40Ca; calculated neutron momentum distribution. Shell, Saxon-Woods wave functions. NUCLEAR REACTIONS 165Ho(20Ne, X), E=292-600 MeV; 165Ho(12C, X), E=300, 379.2 MeV; Ag(16O, X), E=480 MeV; Ag(32S, X), E=960 MeV; 40Ca(40Ar, X), E=800 MeV; calculated average primary collision time, projectile translational momentum, total kinetic energy gain. Boltzmann master equation, nuclear surface, mean field, isospin effects, preequilibrium reactions.
doi: 10.1007/BF01297728
1995CA32 Phys.Rev. C52, 2577 (1995) M.Cavinato, E.Fabrici, E.Gadioli, E.Gadioli Erba, P.Vergani, M.Crippa, G.Colombo, I.Redaelli, M.Ripamonti Study of the Reactions Occurring in the Fusion of 12C and 16O with Heavy Nuclei at Incident Energies Below 10 MeV/Nucleon NUCLEAR REACTIONS, ICPND 181Ta, 197Au(12C, X), E=54-98 MeV; 165Ho, 181Ta(16O, X), E=75-125 MeV; measured evaporation residues production σ(E); deduced fusion (without fission) σ.
doi: 10.1103/PhysRevC.52.2577
1994CA29 Acta Phys.Pol. B25, 475 (1994) M.Cavinato, E.Fabrici, E.Gadioli, E.Gadioli Erba, M.Galmarini, P.Vergani Non Equilibrium Particle Emission in Nuclear Reactions NUCLEAR REACTIONS 165Ho(12C, X), E=25 MeV/nucleon; 40Ca(40Ar, X), E=20 MeV/nucleon; 107Ag(16O, X), E=30 MeV/nucleon; 197Au(36Ar, X), E=35 MeV/nucleon; compiled, reviewed data, analyses; deduced new mechanism evidence. Boltzmann master equation approach.
1994CA49 Z.Phys. A347, 237 (1994) M.Cavinato, E.Fabrici, E.Gadioli, E.Gadioli Erba, M.Galmarini, A.Gritti Intermediate Mass Fragment Emission in Boltzmann Master Equation Theory of Pre-Equilibrium Reactions NUCLEAR REACTIONS 197Au(36Ar, X), E=35 MeV/nucleon; calculated intermediate mass fragments angle integrated multiplicity spectra. 54Fe(p, X), E=62 MeV; calculated light charged particle spectra. Ag(32S, X), E=30 MeV/nucleon; calculated light particles multiplicity spectra. Coalescence model.
doi: 10.1007/BF01289790
1993VE09 Phys.Rev. C48, 1815 (1993) P.Vergani, E.Gadioli, E.Vaciago, E.Fabrici, E.Gadioli Erba, M.Galmarini, G.Ciavola, C.Marchetta Complete and Incomplete Fusion and Emission of Preequilibrium Nucleons in the Interaction of 12C with 197Au Below 10 MeV/nucleon NUCLEAR REACTIONS, ICPND 197Au(12C, X), E ≤ 10 MeV/nucleon; measured production σ(E) for 206,205,204,203At, 203,202,205,204Po, 203,202,201,200,199Bi, 201,200,199Pb, 199,198m,198Tl. Complete, incomplete fusion, preequilibrium emission. Activation technique.
doi: 10.1103/PhysRevC.48.1815
1992CE03 Phys.Rev. C45, 2369 (1992) I.Cervesato, E.Fabrici, E.Gadioli, E.Gadioli-Erba, M.Galmarini Light Particle Emission in Boltzmann Master Equation Theory of Pre-Equilibrium Reactions NUCLEAR REACTIONS 107Ag(32S, X), E=960 MeV; calculated deuteron spectra; 107Ag(16O, X), E=480 MeV; calculated proton, deuteron, triton, α-particles. 165Ho(12C, xn), E=300 MeV; 165Ho(20Ne, xn), E=402-600 MeV; 40Ca(40Ar, xn), E=20 MeV/nucleon; 209Bi(p, xn), E=90 MeV; calculated neutron spectra. 60Ni(n, xp), E=60 MeV; calculated proton spectra. 120Sn, 54Fe(p, X), E=62 MeV; calculated spectra of X=p, d, t, α, 3He; 54Fe, 89Y, 120Sn, 197Au(p, xα), E=62 MeV; calculated α spectra. Preequilibrium reactions, Boltzmann master equation.
doi: 10.1103/PhysRevC.45.2369
1991FA02 Z.Phys. A338, 17 (1991) E.Fabrici, E.Gadioli, E.Gadioli Erba, M.Galmarini Fast Neutron Emission from Partial Fusion Heavy Ion Reactions NUCLEAR REACTIONS Ni, 165Ho(14N, X), E=35 MeV/nucleon; analyzed (nucleon)(fragment)-coin data; deduced reaction mechanism. Boltzmann master equation.
doi: 10.1007/BF01279112
1991PA09 Phys.Rev. C44, 1528 (1991) D.J.Parker, P.Vergani, E.Gadioli, J.J.Hogan, F.Vettore, E.Gadioli-Erba, E.Fabrici, M.Galmarini Recoil Range Study of Complete and Incomplete Fusion of C and Au at 10 MeV/Nucleon NUCLEAR REACTIONS 197Au(12C, X), E=120 MeV; measured residue production σ, X=196Au-204Po; deduced reaction mechanism. Monte Carlo calculations.
doi: 10.1103/PhysRevC.44.1528
1990FA11 Phys.Rev. C42, 2163 (1990) E.Fabrici, E.Gadioli, E.Gadioli Erba, M.Galmarini Hard Photon Emission in Heavy-Ion Reactions NUCLEAR REACTIONS 40Ca(40Ar, xn), E=20 MeV/nucleon; 165Ho(C, xn), E=24 MeV/nucleon; 209Bi(p, xn), E=90 MeV; calculated neutron spectrum. C, Cu, Ag, 197Au(p, X), E=72 MeV; 197Au(p, X), E=168 MeV; Pb, C(n, X), E=20, 30, 40 MeV/nucleon; 12C(12C, X), E=48, 60, 74 MeV/nucleon; C(86Kr, X), E=44 MeV/nucleon; 158Gd(40Ar, X), E=44 MeV/nucleon; 238U, 12C(12C, X), E=84 MeV/nucleon; Sn(136Xe, X), E=89 MeV/nucleon; calculated γ-spectra, multiplicities. Single p-n bremsstrahlung process.
doi: 10.1103/PhysRevC.42.2163
1989FA06 Phys.Rev. C40, 459 (1989) E.Fabrici, E.Gadioli, E.Gadioli Erba Exciton Model Analysis of Neutron Spectra from Fusion and Quasifusion of Two Heavy Ions NUCLEAR REACTIONS 165Ho(12C, xn), (20Ne, xn), E=20, 25, 30 MeV/nucleon; calculated preequilibrium neutron spectra. Exciton model.
doi: 10.1103/PhysRevC.40.459
1989FA11 Phys.Rev. C40, 2548 (1989) E.Fabrici, E.Gadioli, E.Gadioli Erba, M.Galmarini, F.Fabbri, G.Reffo Importance of Nucleon-Nucleon Interactions in Hardening Nucleon Spectra in Heavy Ion Fusion NUCLEAR REACTIONS 165Ho(12C, xn), E=300 MeV; 165Ho(20Ne, xn), E=600, 402 MeV; calculated preequilibrium neutron multiplicity distributions. 40Ca(40Ar, xn), E=800 MeV; 27Al, 58Ni, 120Sn, 197Au(32S, xp), E not given; calculated nucleon spectra; deduced nucleon-nucleon interaction role. Master equation approach.
doi: 10.1103/PhysRevC.40.2548
1980FA06 Phys.Rev. C21, 830 (1980) E.Fabrici, S.Micheletti, M.Pignanelli, F.G.Resmini, R.De Leo, G.D'Erasmo, A.Pantaleo, J.L.Escudie, A.Tarrats Proton Elastic Scattering on Light Nuclei. I. Energy Dependence NUCLEAR REACTIONS 15N(p, p), E=18.1-44.2 MeV; 18O(p, p), E=14.7-44.1 MeV; 24Mg(p, p), E=35.2-44.1 MeV; 40Ar(p, p), E=20.9-44.1 MeV; measured σ(θ); deduced optical model potentials. Phase shift, optical model analyses.
doi: 10.1103/PhysRevC.21.830
1980FA07 Phys.Rev. C21, 844 (1980) E.Fabrici, S.Micheletti, M.Pignanelli, F.G.Resmini, R.De Leo, G.D'Erasmo, A.Pantaleo Proton Elastic Scattering on Light Nuclei. II. Nuclear Structure Effects NUCLEAR REACTIONS 9Be, 10,11B, 12,13C, 14,15N, 16,17,18O, 19F, 20,22Ne, 23Na, 24,25,26Mg, 27Al, 28,29,30Si, 31P, 32,34S, 35,37Cl, 40Ar, 39,41K, 40,42,43,44,48Ca, 45Sc, 46,47,48,50Ti, 51V, 50,52,53,54Cr, 55Mn, 54,56,58Fe, 59Co, 58,60,61,62,64Ni, 63,65Cu, 64,66,67,68,70Zn(p, p), (p, p'), E=35.2 MeV; 23Na, 31P, 39K, 45Sc, 51V, 50,53,54Cr, 62,64Ni(p, p), (p, p'), E=29.7 MeV; measured σ(θ); deduced optical-model parameters. 9Be, 10,11B, 12C, 14,15N, 16,17,18O, 19F, 20,22Ne, 23Na, 24,25,26Mg, 27Al, 28,29,30Si, 31P, 32,34S, 35,37Cl, 40Ar, 39,41K, 40,42,43,44,48Ca, 45Sc, 46,47,48,50Ti, 51V, 50,52,53,54Cr, 55Mn, 54,56,58Fe, 59Co, 58,60,61,62,64Ni, 63,65Cu, 64,66,67,68,70Zn level deduced β2. Optical-model, coupled-channel analyses.
doi: 10.1103/PhysRevC.21.844
1975PI01 Nucl.Phys. A237, 64 (1975) M.Pignanelli, F.Resmini, E.Fabrici, J.L.Escudie, Y.Terrien A Study of the Effective Interaction by the 15N(3He, t)15O Reaction at Incident Energies between 16.5 and 37.7 MeV NUCLEAR REACTIONS 15N(3He, t), E=16.5, 20.0, 24.4, 30.2, 34.4, 37.7 MeV; 15N(3He, 3He'), E=30.2.34.4, 37.7 MeV; measured σ(Et, θ), σ(E(3He), θ); deduced optical model parameters. Enriched 15N gaseous target.
doi: 10.1016/0375-9474(75)90463-7
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