NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = E.Santopinto Found 52 matches. 2024CI02 Phys.Rev. C 109, 024615 (2024) I.Ciraldo, F.Cappuzzello, M.Cavallaro, D.Carbone, A.Gargano, G.De Gregorio, H.Garcia-Tecocoatzi, E.Santopinto, R.I.Magana-Vsevolodovna, L.Acosta, C.Agodi, P.Amador-Valenzuela, G.A.Brischetto, S.Burrello, D.Calvo, E.R.Chavez Lomeli, M.Colonna, F.Delaunay, H.Djapo, C.Eke, P.Finocchiaro, S.Firat, M.Fisichella, M.A.Guazzelli, A.Hacisalihoglu, R.Linares, N.H.Medina, M.Moralles, J.R.B.Oliveira, A.Pakou, L.Pandola, H.Petrascu, F.Pinna, O.Sgouros, S.O.Solakci, V.Soukeras, G.Souliotis, A.Spatafora, D.Torresi, S.Tudisco, A.Yildirim, V.A.B.Zagatto Analysis of one-proton transfer reaction in 18O+76Se collisions at 275 MeV
doi: 10.1103/PhysRevC.109.024615
2023CA02 Prog.Part.Nucl.Phys. 128, 103999 (2023) F.Cappuzzello, H.Lenske, M.Cavallaro, C.Agodi, N.Auerbach, J.I.Bellone, R.Bijker, S.Burrello, S.Calabrese, D.Carbone, M.Colonna, G.De Gregorio, J.L.Ferreira, D.Gambacurta, H.Garcia-Tecocoatzi, A.Gargano, J.A.Lay, R.Linares, J.Lubian, E.Santopinto, O.Sgouros, V.Soukeras, A.Spatafora Shedding light on nuclear aspects of neutrinoless double beta decay by heavy-ion double charge exchange reactions
doi: 10.1016/j.ppnp.2022.103999
2022MA51 Phys.Rev. C 106, 044307 (2022) R.I.Magana Vsevolodovna, E.Santopinto, R.Bijker Transfer reactions between odd-odd and even-even nuclei by using the interacting boson fermion fermion model and 0νββ decay in closure approximation RADIOACTIVITY 116Cd(2β-); calculated nuclear matrix elements (NMEs) for 0νββ decay. Interacting boson fermion fermion model (IBFFM). Comparison to IBM-2 calculations. NUCLEAR STRUCTURE 116Cd, 116Sn, 116In; calculated levels, J, π, spectroscopic amplitudes and one-body transition densities (OBTDs) for transitions from the 0+ ground state of 116Sn and 116Cd to the states of 116In. Interacting boson fermion fermion model (IBFFM). Comparison to experimental data.
doi: 10.1103/PhysRevC.106.044307
2021AC08 Eur.Phys.J. A 57, 261 (2021) A.Accardi, A.Afanasev, I.Albayrak, S.F.Ali, M.Amaryan, J.R.M.Annand, J.Arrington, A.Asaturyan, H.Atac, H.Avakian, T.Averett, C.Ayerbe Gayoso, X.Bai, L.Barion, M.Battaglieri, V.Bellini, R.Beminiwattha, F.Benmokhtar, V.V.Berdnikov, J.C.Bernauer, V.Bertone, A.Bianconi, A.Biselli, P.Bisio, P.Blunden, M.Boer, M.Bondi, K.-T.Brinkmann, W.J.Briscoe, V.Burkert, T.Cao, A.Camsonne, R.Capobianco, L.Cardman, M.Carmignotto, M.Caudron, L.Causse, A.Celentano, P.Chatagnon, J.-P.Chen, T.Chetry, G.Ciullo, E.Cline, P.L.Cole, M.Contalbrigo, G.Costantini, A.D'Angelo, L.Darme, D.Day, M.Defurne, M.De Napoli, A.Deur, R.De Vita, N.D'Hose, S.Diehl, M.Diefenthaler, B.Dongwi, R.Dupre, H.Dutrieux, D.Dutta, M.Ehrhart, L.El Fassi, L.Elouadrhiri, R.Ent, J.Erler, I.P.Fernando, A.Filippi, D.Flay, T.Forest, E.Fuchey, S.Fucini, Y.Furletova, H.Gao, D.Gaskell, A.Gasparian, T.Gautam, F.-X.Girod, K.Gnanvo, J.Grames, G.N.Grauvogel, P.Gueye, M.Guidal, S.Habet, T.J.Hague, D.J.Hamilton, O.Hansen, D.Hasell, M.Hattawy, D.W.Higinbotham, A.Hobart, T.Horn, C.E.Hyde, H.Ibrahim, A.Ilyichev, A.Italiano, K.Joo, S.J.Joosten, V.Khachatryan, N.Kalantarians, G.Kalicy, B.Karky, D.Keller, C.Keppel, M.Kerver, M.Khandaker, A.Kim, J.Kim, P.M.King, E.Kinney, V.Klimenko, H.-S.Ko, M.Kohl, V.Kozhuharov, B.T.Kriesten, G.Krnjaic, V.Kubarovsky, T.Kutz, L.Lanza, M.Leali, P.Lenisa, N.Liyanage, Q.Liu, S.Liuti, J.Mammei, S.Mantry, D.Marchand, P.Markowitz, L.Marsicano, V.Mascagna, M.Mazouz, M.McCaughan, B.McKinnon, D.McNulty, W.Melnitchouk, A.Metz, Z.-E.Meziani, S.Migliorati, M.Mihovilovic, R.Milner, A.Mkrtchyan, H.Mkrtchyan, A.Movsisyan, H.Moutarde, M.Muhoza, C.Munoz Camacho, J.Murphy, P.Nadel-Turonski, E.Nardi, J.Nazeer, S.Niccolai, G.Niculescu, R.Novotny, J.F.Owens, M.Paolone, L.Pappalardo, R.Paremuzyan, B.Pasquini, E.Pasyuk, T.Patel, I.Pegg, C.Peng, D.Perera, M.Poelker, K.Price, A.J.R.Puckett, M.Raggi, N.Randazzo, M.N.H.Rashad, M.Rathnayake, B.Raue, P.E.Reimer, M.Rinaldi, A.Rizzo, Y.Roblin, J.Roche, O.Rondon-Aramayo, F.Sabatie, G.Salme, E.Santopinto, R.Santos Estrada, B.Sawatzky, A.Schmidt, P.Schweitzer, S.Scopetta, V.Sergeyeva, M.Shabestari, A.Shahinyan, Y.Sharabian, S.Sirca, E.S.Smith, D.Sokhan, A.Somov, N.Sparveris, M.Spata, H.Spiesberger, M.Spreafico, S.Stepanyan, P.Stoler, I.Strakovsky, R.Suleiman, M.Suresh, P.Sznajder, H.Szumila-Vance, V.Tadevosyan, A.S.Tadepalli, A.W.Thomas, M.Tiefenback, R.Trotta, M.Ungaro, P.Valente, M.Vanderhaeghen, L.Venturelli, H.Voskanyan, E.Voutier, B.Wojtsekhowski, M.H.Wood, S.Wood, J.Xie, W.Xiong, Z.Ye, M.Yurov, H.-G.Zaunick, S.Zhamkochyan, J.Zhang, S.Zhang, S.Zhao, Z.W.Zhao, X.Zheng, J.Zhou, C.Zorn An experimental program with high duty-cycle polarized and unpolarized positron beams at Jefferson Lab
doi: 10.1140/epja/s10050-021-00564-y
2021BA39 Eur.Phys.J. A 57, 253 (2021) M.Battaglieri, A.Bianconi, P.Bisio, M.Bondi, A.Celentano, G.Costantini, P.L.Cole, L.Darme, R.De Vita, A.D'Angelo, M.De Napoli, L.El Fassi, V.Kozhuharov, A.Italiano, G.Krnjaic, L.Lanza, M.Leali, L.Marsicano, V.Mascagna, S.Migliorati, E.Nardi, M.Raggi, N.Randazzo, E.Santopinto, E.Smith, M.Spreafico, S.Stepanyan, M.Ungaro, P.Valente, L.Venturelli, M.H.Wood Light dark matter searches with positrons
doi: 10.1140/epja/s10050-021-00524-6
2020FE11 Phys.Rev. C 102, 054329 (2020) J.Ferretti, J.Kotila, R.I.Magana Vsevolodovna, E.Santopinto β-decay rates of 115, 117Rh into 115, 117Pd isotopes in the microscopic interacting boson-fermion model NUCLEAR STRUCTURE 115,117Pd; calculated neutron and proton single-particle energies, levels, J, π, β-decay rates from 115,117Rh decays using neutron-proton interacting boson-fermion model (IBFM-2); deduced spin-parity for ground states. Comparison with experimental data. RADIOACTIVITY 115,117Rh(β-); calculated β-decay half-lives and logft values using IBFM-2. Comparison with available experimental data.
doi: 10.1103/PhysRevC.102.054329
2018CA16 Eur.Phys.J. A 54, 72 (2018) F.Cappuzzello, C.Agodi, M.Cavallaro, D.Carbone, S.Tudisco, D.Lo Presti, J.R.B.Oliveira, P.Finocchiaro, M.Colonna, D.Rifuggiato, L.Calabretta, D.Calvo, L.Pandola, L.Acosta, N.Auerbach, J.Bellone, R.Bijker, D.Bonanno, D.Bongiovanni, T.Borello-Lewin, I.Boztosun, O.Brunasso, S.Burrello, S.Calabrese, A.Calanna, E.R.Chavez-Lomeli, G.D'Agostino, P.N.De Faria, G.De Geronimo, F.Delaunay, N.Deshmukh, J.L.Ferreira, M.Fisichella, A.Foti, G.Gallo, H.Garcia-Tecocoatzi, V.Greco, A.Hacisalihoglu, F.Iazzi, R.Introzzi, G.Lanzalone, J.A.Lay, F.La Via, H.Lenske, R.Linares, G.Litrico, F.Longhitano, J.Lubian, N.H.Medina, D.R.Mendes, M.Moralles, A.Muoio, A.Pakou, H.Petrascu, F.Pinna, S.Reito, A.D.Russo, G.Russo, G.Santagati, E.Santopinto, R.B.B.Santos, O.Sgouros, M.A.G.da Silveira, S.O.Solakci, G.Souliotis, V.Soukeras, A.Spatafora, D.Torresi, R.Magana Vsevolodovna, A.Yildirim, V.A.B.Zagatto The NUMEN project: NUclear Matrix Elements for Neutrinoless double beta decay
doi: 10.1140/epja/i2018-12509-3
2018SA36 Acta Phys.Pol. B49, 381 (2018) G.Santagati, B.Paes, R.Magana Vsevolodovna, F.Cappuzzello, D.Carbone, E.N.Cardozo, M.Cavallaro, H.Garcia-Tecocoatzi, A.Gargano, J.L.Ferreira, S.M.Lenzi, R.Linares, E.Santopinto, A.Vitturi, J.Lubian Study of the 18O + 64Ni Two-neutron Transfer Reaction at 84 MeV by MAGNEX NUCLEAR REACTIONS 64Ni(18O, 16O), 66Ni, E=84 MeV; measured reaction products in angular range 30-310 (lab) at INFN-LNS in Catania, ejectiles momenta analyzed using MAGNEX spectrometer; deduced 66Ni excitation energy spectrum, σ(θ) to gs to to 1.424 state of 66Ni; calculated σ(θ) to gs to to 1.424 state; deduced that short-range pairing correlation may play important role in 2n transfer to 66Ni gs, verified predominance of 2n transfer to the first excited state of 66Ni, confirmed long-range effect of the wave function of this state. Calculations independent on the nuclear structure model.
doi: 10.5506/aphyspolb.49.381
2018SA52 Phys.Rev. C 98, 061601 (2018) E.Santopinto, H.Garcia-Tecocoatzi, R.I.M.Vsevolodovna, J.Ferretti Heavy-ion double-charge-exchange and its relation to neutrinoless double-β decay NUCLEAR REACTIONS 40Ca(18O, 18Ne), E=15 MeV/nucleon; calculated heavy-ion double charge exchange (DCE) cross sections, DCE-double-Gamow-Teller (DGT) and DCE-double-Fermi (DF) matrix elements for 40Ca to 40Ar and 18O to 18Ne using the eikonal approximation and generalized seniority scheme. RADIOACTIVITY 76Ge, 82Se, 116Cd, 128Te(2β-); calculated double Fermi (DF), double Gamow-Teller (DGT), and total nuclear matrix elements (NMEs) for the 0νββ decay mode using microscopic interacting boson model 2 (IBM-2).
doi: 10.1103/PhysRevC.98.061601
2017GA16 Eur.Phys.J. A 53, 115 (2017) H.Garcia-Tecocoatzi, R.Bijker, J.Ferretti, E.Santopinto Self-energies of octet and decuplet baryons due to the coupling to the baryon-meson continuum
doi: 10.1140/epja/i2017-12306-6
2017PA38 Phys.Rev. C 96, 044612 (2017) B.Paes, G.Santagati, R.Magana Vsevolodovna, F.Cappuzzello, D.Carbone, E.N.Cardozo, M.Cavallaro, H.Garcia-Tecocoatzi, A.Gargano, J.L.Ferreira, S.M.Lenzi, R.Linares, E.Santopinto, A.Vitturi, J.Lubian Long-range versus short-range correlations in the two-neutron transfer reaction 64Ni (18O, 16O) 66Ni NUCLEAR REACTIONS 64Ni(18O, 16O)66Ni, E=84 MeV; measured reaction products, 16O spectra, σ(θ) for g.s. and first 2+ state in 66Ni using MAGNEX spectrometer at INFN-LNS-Catania. 66Ni; deduced levels, J, π, configurations, two-neutron spectroscopic amplitudes, σ(θ) data analyzed using three methods: the extreme cluster model, independent coordinate, and two-step DWBA model; calculated cross sections by exact finite range coupled-channel Born approximation (CCBA) and coupled reaction channel (CRC) methods using Sao Paulo double folding potential (SPP) and FRESCO code. NUCLEAR STRUCTURE 66Ni; calculated spectroscopic amplitudes for one- and two-neutron transfer to the first and second 0+ and 2+ states using NUSHELLX code and the model space bjuff with an effective phenomenological interaction and 48Ca as an inert core, and also using the microscopic IBM-2 method. 65Ni; calculated spectroscopic amplitudes for one-neutron transfer to the first and second 5/2-, 1/2-, 3/2- states and first 9/2+ using NUSHELLX code, and also using the microscopic IBM-2 method. 64,66Ni; calculated low-lying positive-parity 0+, 2+ and 4+ levels, and compared with experimental values. 65Ni; calculated low-lying negative-parity levels, and compared with experimental values.
doi: 10.1103/PhysRevC.96.044612
2016DE16 Eur.Phys.J. A 52, 121 (2016) M.De Sanctis, J.Ferretti, E.Santopinto, A.Vassallo Relativistic quark-diquark model of baryons with a spin-isospin transition interaction: Non-strange baryon spectrum and nucleon magnetic moments NUCLEAR STRUCTURE 1n, 1H; calculated mass excess using relativistic quark-diquark model of baryons with a spin-isospin transition interaction.
doi: 10.1140/epja/i2016-16121-3
2015SA30 Phys.Rev. C 92, 025202 (2015) Strange and nonstrange baryon spectra in the relativistic interacting quark-diquark model with a Gursey and Radicati-inspired exchange interaction
doi: 10.1103/PhysRevC.92.025202
2014DO12 Few-Body Systems 55, 873 (2014) Y.Dong, M.Giannini, E.Santopinto, A.Vassallo Electromagnetic N - Δ(1232) Transitions within the Point-Form of Relativistic Quantum Mechanics
doi: 10.1007/s00601-014-0805-7
2013FE06 Phys.Rev. C 88, 015207 (2013) J.Ferretti, G.Galata, E.Santopinto Interpretation of the X(3872) as a charmonium state plus an extra component due to the coupling to the meson-meson continuum
doi: 10.1103/PhysRevC.88.015207
2012BI05 Phys.Rev. C 85, 035204 (2012) R.Bijker, J.Ferretti, E.Santopinto ss(bar) sea pair contribution to electromagnetic observables of the proton in the unquenched quark model
doi: 10.1103/PhysRevC.85.035204
2012BI16 J.Phys.:Conf.Ser. 387, 012011 (2012) R.Bijker, J.Ferretti, E.Santopinto Strangeness of the proton NUCLEAR STRUCTURE 1H; calculated strangeness radius, strange magnetic moment using unquenched quark model with the effect of strange quarks. Compared to data.
doi: 10.1088/1742-6596/387/1/012011
2012FE08 Phys.Rev. C 86, 015204 (2012) J.Ferretti, G.Galata, E.Santopinto, A.Vassallo Bottomonium self-energies due to the coupling to the meson-meson continuum
doi: 10.1103/PhysRevC.86.015204
2012GA43 Phys.Rev. C 86, 045202 (2012) Hybrid quark-diquark baryon model
doi: 10.1103/PhysRevC.86.045202
2012SA56 Phys.Rev. C 86, 065202 (2012) Systematic study of longitudinal and transverse helicity amplitudes in the hypercentral constituent quark model
doi: 10.1103/PhysRevC.86.065202
2011DE33 Phys.Rev. C 84, 055201 (2011) M.De Sanctis, J.Ferretti, E.Santopinto, A.Vassallo Electromagnetic form factors in the relativistic interacting quark-diquark model of baryons
doi: 10.1103/PhysRevC.84.055201
2011FE04 Phys.Rev. C 83, 065204 (2011) J.Ferretti, A.Vassallo, E.Santopinto Relativistic quark-diquark model of baryons
doi: 10.1103/PhysRevC.83.065204
2010SA35 Phys.Rev. C 82, 062202 (2010) Flavor asymmetry of sea quarks in the unquenched quark model
doi: 10.1103/PhysRevC.82.062202
2010SA37 Phys.Rev. C 82, 065204 (2010) E.Santopinto, A.Vassallo, M.M.Giannini, M.De Sanctis High Q2 behavior of the electromagnetic form factors in the relativistic hypercentral constituent quark model
doi: 10.1103/PhysRevC.82.065204
2009BI11 Phys.Rev. C 80, 065210 (2009) Unquenched quark model for baryons: Magnetic moments, spins, and orbital angular momenta
doi: 10.1103/PhysRevC.80.065210
2008AD11 Phys.Rev. C 78, 035201 (2008) C.Adamuscin, E.Tomasi-Gustafsson, E.Santopinto, R.Bijker Two-component model for the axial form factor of the nucleon
doi: 10.1103/PhysRevC.78.035201
2008CA12 Eur.Phys.J. A 35, 253 (2008) S.Capstick, A.Svarc, L.Tiator, J.Gegelia, M.M.Giannini, E.Santopinto, C.Hanhart, S.Scherer, T.-S.H.Lee, T.Sato, N.Suzuki The physical meaning of scattering matrix singularities in coupled-channel formalisms BRAG 2007 Workshop summary
doi: 10.1140/epja/i2007-10576-1
2007CH21 Nucl.Phys. A782, 62c (2007) D.Y.Chen, Y.B.Dong, M.M.Giannini, E.Santopinto Hypercentral Constituent Quark Model with a Meson Cloud NUCLEAR STRUCTURE 1H; calculated elastic electromagnetic form factors. Hypercentral constituent quark model with meson cloud correction.
doi: 10.1016/j.nuclphysa.2006.10.004
2007DE11 Nucl.Phys. A782, 57c (2007) M.De Sanctis, M.M.Giannini, E.Santopinto, A.Vassallo Elastic nucleon form factors NUCLEAR STRUCTURE 1H; calculated elastic electromagnetic form factors. Relativized hypercentral constituent quark model.
doi: 10.1016/j.nuclphysa.2006.10.049
2007DE58 Phys.Rev. C 76, 062201 (2007) M.De Sanctis, M.M.Giannini, E.Santopinto, A.Vassallo Electromagnetic form factors and the hypercentral constituent quark model
doi: 10.1103/PhysRevC.76.062201
2007SA24 Phys.Rev. C 75, 045206 (2007) Spectroscopy of tetraquark states
doi: 10.1103/PhysRevC.75.045206
2005DE25 Nucl.Phys. A755, 294c (2005) M.De Sanctis, M.M.Giannini, E.Santopinto, A.Vassallo Electromagnetic form factors in the Hypercentral Constituent Quark Model NUCLEAR STRUCTURE 1H; analyzed electromagnetic form factors. Hypercentral constituent quark model.
doi: 10.1016/j.nuclphysa.2005.03.143
2005GI12 Eur.Phys.J. A 25, 241 (2005) M.M.Giannini, E.Santopinto, A.Vassallo A new application of the Gursey and Radicati mass formula
doi: 10.1140/epja/i2005-10113-4
2005SA43 Phys.Rev. C 72, 022201 (2005) Interacting quark-diquark model of baryons
doi: 10.1103/PhysRevC.72.022201
2004BI13 Eur.Phys.J. A 22, 319 (2004) R.Bijker, M.M.Giannini, E.Santopinto Spectroscopy of pentaquark states
doi: 10.1140/epja/i2003-10232-x
2004DE05 Eur.Phys.J. A 19, Supplement 1, 81 (2004) M.De Sanctis, M.M.Giannini, E.Santopinto, A.Vassallo Electromagnetic form factors in the hypercentral CQM
doi: 10.1140/epjad/s2004-03-014-0
2004GO13 Eur.Phys.J. A 19, Supplement 1, 77 (2004) M.Gorchtein, D.Drechsel, M.Giannini, E.Santopinto Generalized sum rules of the nucleon in the constituent quark model NUCLEAR STRUCTURE 1n, 1H; analyzed sum rules, related features. Constituent quark model.
doi: 10.1140/epjad/s2004-03-013-1
2004GO50 Phys.Rev. C 70, 055202 (2004) M.Gorchtein, D.Drechsel, M.M.Giannini, E.Santopinto, L.Tiator Generalized sum rules of the nucleon in the constituent quark model NUCLEAR STRUCTURE 1n, 1H; calculated sum rules, polarizabilities. Hypercentral constituent quark model.
doi: 10.1103/PhysRevC.70.055202
2004TI01 Eur.Phys.J. A 19, Supplement 1, 55 (2004) L.Tiator, D.Drechsel, S.Kamalov, M.M.Giannini, E.Santopinto, A.Vassallo Electroproduction of nucleon resonances NUCLEAR REACTIONS 1H(e, π0X), E=high; analyzed data; deduced resonance production associated helicity amplitudes, Q2 dependence. Unitary isobar model.
doi: 10.1140/epjad/s2004-03-009-9
2003GI01 Phys.Lett. 552B, 149 (2003) M.M.Giannini, E.Santopinto, A.Vassallo, M.Vanderhaeghen Quark model predictions for the SU(6)-breaking ratio of the proton momentum distributions NUCLEAR STRUCTURE 1n, 1H; calculated parton distribution features, relative anomalous magnetic moments. Constituent quark model.
doi: 10.1016/S0370-2693(02)03158-1
2002GI03 Nucl.Phys. A699, 308c (2002) M.M.Giannini, E.Santopinto, A.Vassallo The Hypercentral Constituent Quark Model
doi: 10.1016/S0375-9474(01)01508-1
2001GI18 Eur.Phys.J. A 12, 447 (2001) M.M.Giannini, E.Santopinto, A.Vassallo Hypercentral Constituent Quark Model and Isospin Dependence
doi: 10.1007/s10050-001-8668-y
2000DE40 Phys.Rev. C62, 025208 (2000) M.De Sanctis, M.M.Giannini, L.Repetto, E.Santopinto Proton Form Factors in the Hypercentral Constituent Quark Model NUCLEAR STRUCTURE 1H; calculated charge, magnetic form factors.
doi: 10.1103/PhysRevC.62.025208
2000DR09 Phys.Lett. 484B, 236 (2000) D.Drechsel, M.Vanderhaeghen, M.M.Giannini, E.Santopinto Inelastic Photon Scattering and the Magnetic Moment of the Δ (1232) Resonance NUCLEAR REACTIONS 1H(γ, γπ0), E=286 MeV; calculated σ, σ(E, θ). Constituent quark model, effective Lagrangian procedure.
doi: 10.1016/S0370-2693(00)00654-7
1998AI01 J.Phys.(London) G24, 753 (1998) M.Aiello, M.M.Giannini, E.Santopinto Electromagnetic Transition Form Factors of Negative Parity Nucleon Resonances
doi: 10.1088/0954-3899/24/4/007
1998DE08 Eur.Phys.J. A 1, 187 (1998) M.De Sanctis, E.Santopinto, M.M.Giannini A Relativistic Study of the Nucleon Form Factors NUCLEAR STRUCTURE 1n, 1H; calculated charge, magnetic form factors; deduced relativistic effects. Constituent quark models. Comparison with data.
doi: 10.1007/s100500050047
1998DE45 Eur.Phys.J. A 2, 403 (1998) M.De Sanctis, E.Santopinto, M.M.Giannini A Relativistic Study of the Nucleon Helicity Amplitudes NUCLEAR STRUCTURE 1n, 1H; calculated nucleon resonances form factors. Constituent quark model.
doi: 10.1007/s100500050137
1998SA11 Eur.Phys.J. A 1, 307 (1998) E.Santopinto, F.Iachello, M.M.Giannini Nucleon Form Factors in a Simple Three-Body Quark Model
doi: 10.1007/s100500050065
1997SA49 Nucl.Phys. A623, 100c (1997) E.Santopinto, F.Iachello, M.M.Giannini Exactly Solvable Models of Baryon Spectroscopy
doi: 10.1016/S0375-9474(97)00427-2
1996AI06 Phys.Lett. 387B, 215 (1996) M.Aiello, M.Ferraris, M.M.Giannini, M.Pizzo, E.Santopinto A Three-Body Force Model for the Electromagnetic Excitation of the Nucleon
doi: 10.1016/0370-2693(96)00986-0
1995MO35 Int.J.Mod.Phys. E4, 607 (1995) V.I.Mokeev, E.Santopinto, M.M.Giannini, G.Ricco The Influence of the Nuclear Medium on the Baryon Resonance Excitation NUCLEAR REACTIONS 1H(γ, X), E ≈ 0.5-4 GeV; 2H(γ, X), E ≈ 1.05-2 GeV; calculated photoabsorption σ(E). 9Be, 12C(γ, X), E=0.2-1.6 GeV; calculated per nucleon photoabsorption σ(E); deduced nuclear medium role.
doi: 10.1142/S0218301395000237
1994GI02 Phys.Rev. C49, R1258 (1994) Nucleon Resonances in Nuclei and Quark Exchange
doi: 10.1103/PhysRevC.49.R1258
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