NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = J.M.Quesada Found 43 matches. 2024AM02 Phys.Rev.Lett. 132, 122701 (2024) S.Amaducci, N.Colonna, L.Cosentino, S.Cristallo, P.Finocchiaro, M.Krticka, C.Massimi, M.Mastromarco, A.Mazzone, E.A.Maugeri, A.Mengoni, I.U.Roederer, O.Straniero, S.Valenta, D.Vescovi, O.Aberle, V.Alcayne, J.Andrzejewski, L.Audouin, V.Babiano-Suarez, M.Bacak, M.Barbagallo, S.Bennett, E.Berthoumieux, J.Billowes, D.Bosnar, A.Brown, M.Busso, M.Caamano, L.Caballero-Ontanaya, F.Calvino, M.Calviani, D.Cano-Ott, A.Casanovas, F.Cerutti, E.Chiaveri, G.Cortes, M.A.Cortes-Giraldo, L.A.Damone, P.J.Davies, M.Diakaki, M.Dietz, C.Domingo-Pardo, R.Dressler, Q.Ducasse, E.Dupont, I.Duran, Z.Eleme, B.Fernandez-Dominguez, A.Ferrari, V.Furman, K.Gobel, R.Garg, A.Gawlik-Ramiega, S.Gilardoni, I.F.Goncalves, E.Gonzalez-Romero, C.Guerrero, F.Gunsing, H.Harada, S.Heinitz, J.Heyse, D.G.Jenkins, A.Junghans, F.Kappeler, Y.Kadi, A.Kimura, I.Knapova, M.Kokkoris, Y.Kopatch, D.Kurtulgil, I.Ladarescu, C.Lederer-Woods, H.Leeb, J.Lerendegui-Marco, S.J.Lonsdale, D.Macina, A.Manna, T.Martinez, A.Masi, P.Mastinu, E.Mendoza, V.Michalopoulou, P.M.Milazzo, F.Mingrone, J.Moreno-Soto, A.Musumarra, A.Negret, R.Nolte, F.Ogallar, A.Oprea, N.Patronis, A.Pavlik, J.Perkowski, C.Petrone, L.Piersanti, E.Pirovano, I.Porras, J.Praena, J.M.Quesada, D.Ramos-Doval, T.Rauscher, R.Reifarth, D.Rochman, C.Rubbia, M.Sabate-Gilarte, A.Saxena, P.Schillebeeckx, D.Schumann, A.Sekhar, A.G.Smith, N.V.Sosnin, P.Sprung, A.Stamatopoulos, G.Tagliente, J.L.Tain, A.Tarifeno-Saldivia, L.Tassan-Got, Th.Thomas, P.Torres-Sanchez, A.Tsinganis, J.Ulrich, S.Urlass, G.Vannini, V.Variale, P.Vaz, A.Ventura, V.Vlachoudis, R.Vlastou, A.Wallner, P.J.Woods, T.Wright, P.Zugec Measurement of the 140Ce(n, γ) Cross Section at n_TOF and Its Astrophysical Implications for the Chemical Evolution of the Universe NUCLEAR REACTIONS 140Ce(n, γ), E<200 keV; measured reaction products, En, In, Eγ, Iγ; deduced Maxwellian averaged σ, yields, resonance parameters, impact on galactic abundances. Comparison with ENDF/B-VIII.0, JENDL-5 libraries, R-matrix code SAMMY. The neutron beam time-of-flight facility (n_TOF) at CERN.
doi: 10.1103/PhysRevLett.132.122701
2024TA03 Eur.Phys.J. A 60, 21 (2024) G.Tagliente, P.M.Milazzo, C.Paradela, S.Kopecky, D.Vescovi, G.Alaerts, L.A.Damone, J.Heyse, M.Krticka, P.Schillebeeckx, A.Mengoni, R.Wynants, S.Valenta, O.Aberle, V.Alcayne, S.Amaducci, J.Andrzejewski, L.Audouin, V.Babiano-Suarez, M.Bacak, M.Barbagallo, V.Becares, F.Becvar, G.Bellia, E.Berthoumieux, J.Billowes, D.Bosnar, A.S.Brown, M.Busso, M.Caamano, L.Caballero, M.Calviani, F.Calvino, D.Cano-Ott, A.Casanovas, F.Cerutti, Y.H.Chen, E.Chiaveri, N.Colonna, G.P.Cortes, M.A.Cortes-Giraldo, L.Cosentino, S.Cristallo, M.Diakaki, M.Dietz, C.Domingo-Pardo, R.Dressler, E.Dupont, I.Duran, Z.Eleme, B.Fernandez-Domingez, A.Ferrari, I.Ferro-Goncalves, P.Finocchiaro, V.Furman, R.Garg, A.Gawlik, S.Gilardoni, T.Glodariu, K.Gobel, E.Gonzalez-Romero, C.Guerrero, F.Gunsing, S.Heinitz, D.G.Jenkins, E.Jericha, Y.Kadi, F.Kappeler, A.Kimura, N.Kivel, M.Kokkoris, Y.Kopatch, D.Kurtulgil, I.Ladarescu, A.C.Larsen, C.Lederer-Woods, J.Lerendegui-Marco, S.Lo Meo, S.J.Lonsdale, M.Lugaro, D.Macina, A.Manna, T.Martinez, A.Masi, C.Massimi, P.F.Mastinu, M.Mastromarco, F.Matteucci, E.Maugeri, A.Mazzone, E.Mendoza, V.Michalopoulou, F.Mingrone, A.Musumarra, A.Negret, R.Nolte, F.Ogallar, A.Oprea, N.Patronis, A.Pavlik, J.Perkowski, L.Piersanti, I.Porras, J.Praena, J.M.Quesada, D.Radeck, D.Ramos Doval, R.Reifarth, D.Rochman, C.Rubbia, M.Sabate-Gilarte, A.Saxena, D.Schumann, A.G.Smith, M.Spelta, N.Sosnin, A.Stamatopoulos, J.L.Tain, Z.Talip, A.E.Tarifeno-Saldivia, L.Tassan-Got, P.Torres-Sanchez, A.Tsinganis, J.Ulrich, S.Urlass, G.Vannini, V.Variale, P.Vaz, A.Ventura, V.Vlachoudis, R.Vlastou, A.Wallner, P.J.Woods, T.J.Wright, P.Zugec High-resolution cross section measurements for neutron interactions on 89Y with incident neutron energies up to 95 keV NUCLEAR REACTIONS 89Y(n, X), (n, γ), E<95 keV; measured reaction products, En, In, TOF; deduced yields, resonance parameters, Maxwellian-averaged σ, capture kernel. Comparison with ENDF/B-VIII.0, JENDL-5, EXFOR libraries, Atlas of Neutron Resonances, KADONIS. The CERN n_TOF facility, GELINA at JRC-Geel.
doi: 10.1140/epja/s10050-024-01243-4
2024WR01 Eur.Phys.J. A 60, (2024) T.Wright, A.G.Smith, N.V.Sosnin, S.A.Bennett, P.J.Davies, A.V.Popescu, J.A.Ryan, A.Sekhar, S.Warren, O.Aberle, S.Amaducci, J.Andrzejewski, L.Audouin, M.Bacak, J.Balibrea, M.Barbagallo, F.Becvar, E.Berthoumieux, J.Billowes, D.Bosnar, A.Brown, M.Caamano, F.Calvino, M.Calviani, D.Cano-Ott, R.Cardella, A.Casanovas, F.Cerutti, Y.H.Chen, E.Chiaveri, N.Colonna, G.Cortes, M.A.Cortes-Giraldo, L.Cosentino, L.A.Damone, M.Diakaki, C.Domingo-Pardo, R.Dressler, E.Dupont, I.Duran, B.Fernandez-Dominguez, A.Ferrari, P.Ferreira, P.Finocchiaro, V.Furman, K.Gobel, A.R.Garcia, A.Gawlik-Ramiega, S.Gilardoni, T.Glodariu, I.F.Goncalves, E.Gonzalez-Romero, E.Griesmayer, C.Guerrero, F.Gunsing, H.Harada, S.Heinitz, J.Heyse, D.G.Jenkins, E.Jericha, F.Kappeler, Y.Kadi, A.Kalamara, P.Kavrigin, A.Kimura, N.Kivel, M.Kokkoris, M.Krticka, D.Kurtulgil, E.Leal-Cidoncha, C.Lederer-Woods, H.Leeb, J.Lerendegui-Marco, S.L.Meo, S.J.Lonsdale, D.Macina, A.Manna, J.Marganiec, T.Martinez, A.Masi, C.Massimi, P.Mastinu, M.Mastromarco, E.A.Maugeri, A.Mazzone, E.Mendoza, A.Mengoni, P.M.Milazzo, F.Mingrone, A.Musumarra, A.Negret, R.Nolte, A.Oprea, N.Patronis, A.Pavlik, J.Perkowski, I.Porras, J.Praena, J.M.Quesada, D.Radeck, T.Rauscher, R.Reifarth, C.Rubbia, M.Sabate-Gilarte, A.Saxena, P.Schillebeeckx, D.Schumann, P.Sedyshev, A.Stamatopoulos, G.Tagliente, J.L.Tain, A.Tarifeno-Saldivia, L.Tassan-Got, S.Valenta, G.Vannini, V.Variale, P.Vaz, A.Ventura, V.Vlachoudis, R.Vlastou, A.Wallner, C.Weiss, P.J.Woods, P.Zugec Measurement of the prompt fission γ-rays from slow neutron-induced fission of 235U with STEFF NUCLEAR REACTIONS 235U(n, F), E; measured reaction products, Eγ, Iγ; deduced prompt-fission γ-ray energies and multiplicities. Comparison with EXFOR and ENDF/B-VIII.0 libraries. STEFF 2E2ν device installed in the second experimental area (EAR2) of the neutron time-of-flight facility n_TOF at CERN.
doi: 10.1140/epja/s10050-024-01277-8
2023RO01 Nucl.Data Sheets 187, 579 (2023) T.Rodriguez-Gonzalez, C.Guerrero, C.M.Backer, J.Bauer, C.Baumer, S.Brons, W.Jentzen, M.C.Jimenez-Ramos, M.A.Millan-Callado, C.Schomers, B.Timmermann, J.M.Quesada, R.Capote Production of 11C, 13N and 15O in proton-induced nuclear reactions up to 200 MeV NUCLEAR REACTIONS C, N, O(p, X)11C/13N/15O, E<200 MeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with available data. The clinical proton treatment centers WPE (Essen) and HIT (Heidelberg), Germany.
doi: 10.1016/j.nds.2023.01.004
2021BA30 Eur.Phys.J. A 57, 197 (2021) V.Babiano-Suarez, J.Lerendegui-Marco, J.Balibrea-Correa, L.Caballero, D.Calvo, I.Ladarescu, D.Real, C.Domingo-Pardo, F.Calvino, A.Casanovas, A.Tarifeno-Saldivia, V.Alcayne, C.Guerrero, M.A.Millan-Callado, T.Rodriguez-Gonzalez, M.Barbagallo, O.Aberle, S.Amaducci, J.Andrzejewski, L.Audouin, M.Bacak, S.Bennett, E.Berthoumieux, J.Billowes, D.Bosnar, A.Brown, M.Busso, M.Caamano, M.Calviani, D.Cano-Ott, F.Cerutti, E.Chiaveri, N.Colonna, G.Cortes, M.A.Cortes-Giraldo, L.Cosentino, S.Cristallo, L.A.Damone, P.J.Davies, M.Diakaki, M.Dietz, R.Dressler, Q.Ducasse, E.Dupont, I.Duran, Z.Eleme, B.Fernandez-Dominguez, A.Ferrari, P.Finocchiaro, V.Furman, K.Gobel, R.Garg, A.Gawlik, S.Gilardoni, I.F.Goncalves, E.Gonzalez-Romero, F.Gunsing, H.Harada, S.Heinitz, J.Heyse, D.G.Jenkins, A.Junghans, F.Kappeler, Y.Kadi, A.Kimura, I.Knapova, M.Kokkoris, Y.Kopatch, M.Krticka, D.Kurtulgil, C.Lederer-Woods, H.Leeb, S.J.Lonsdale, D.Macina, A.Manna, T.Martinez, A.Masi, C.Massimi, P.Mastinu, M.Mastromarco, E.A.Maugeri, A.Mazzone, E.Mendoza, A.Mengoni, V.Michalopoulou, P.M.Milazzo, F.Mingrone, J.Moreno-Soto, A.Musumarra, A.Negret, F.Ogallar, A.Oprea, N.Patronis, A.Pavlik, J.Perkowski, L.Persanti, C.Petrone, E.Pirovano, I.Porras, J.Praena, J.M.Quesada, D.Ramos Doval, T.Rauscher, R.Reifarth, D.Rochman, C.Rubbia, M.Sabate-Gilarte, A.Saxena, P.Schillebeeckx, D.Schumann, A.Sekhar, A.G.Smith, N.V.Sosnin, P.Sprung, A.Stamatopoulos, G.Tagliente, J.L.Tain, L.Tassan-Got, Th.Thomas, P.Torres-Sanchez, A.Tsinganis, J.Ulrich, S.Urlass, S.Valenta, G.Vannini, V.Variale, P.Vaz, A.Ventura, D.Vescovi, V.Vlachoudis, R.Vlastou, A.Wallner, P.J.Woods, T.Wright, P.Zugec Imaging neutron capture cross sections: i-TED proof-of-concept and future prospects based on Machine-Learning techniques NUCLEAR REACTIONS 197Au, 56Fe(n, γ), E<200 KeV; measured reaction products, Eγ, Iγ, En, In, TOF; deduced neutron spectra, signal-to-background ratio in (n, γ) σ measurements using Machine-Learning techniques.
doi: 10.1140/epja/s10050-021-00507-7
2021CA17 Eur.Phys.J. A 57, 210 (2021) An impact of Jacques Raynal on nuclear data evaluation NUCLEAR REACTIONS 27Al(n, X), E=10-250 MeV; 238U(p, n), E=26 MeV; 239,240,242Pu, 233,235,238U, 232Th(n, X), E<20 MeV; 57Fe(p, p), E not given; 238U(n, n'), E<20 MeV; analyzed available data; calculated σ, σ(θ), J, π using ECIS.
doi: 10.1140/epja/s10050-021-00486-9
2021ZH36 J.Phys.(London) G48, 075101 (2021) X.Zhao, W.Sun, E.Sh.Soukhovitskii, D.S.Martyanov, J.M.Quesada, R.Capote Nucleon scattering analysis with a lane-consistent dispersive optical potential for Hf, W and Ta isotopes NUCLEAR REACTIONS 182,184,186W, 178,180Hf, 181Ta(n, X), (n, n), (n, n'), E<200 MeV; calculated σ, σ(θ); deduced optical model parameters. Comparison with experimental data.
doi: 10.1088/1361-6471/abe280
2020MA14 Phys.Lett. B 804, 135405 (2020) A.Mazzone, S.Cristallo, O.Aberle, G.Alaerts, V.Alcayne, S.Amaducci, J.Andrzejewski, L.Audouin, V.Babiano-Suarez, M.Bacak, M.Barbagallo, V.Becares, F.Becvar, G.Bellia, E.Berthoumieux, J.Billowes, D.Bosnar, A.S.Brown, M.Busso, M.Caamano, L.Caballero, M.Calviani, F.Calvino, D.Cano-Ott, A.Casanovas, D.M.Castelluccio, F.Cerutti, Y.H.Chen, E.Chiaveri, G.Clai, N.Colonna, G.P.Cortes, M.A.Cortes-Giraldo, L.Cosentino, L.A.Damone, M.Diakaki, M.Dietz, C.Domingo-Pardo, R.Dressler, E.Dupont, I.Duran, Z.Eleme, B.Fernandez-Domingez, A.Ferrari, I.Ferro-Goncalves, P.Finocchiaro, V.Furman, R.Garg, A.Gawlik, S.Gilardoni, T.Glodariu, K.Gobel, E.Gonzalez-Romero, C.Guerrero, F.Gunsing, S.Heinitz, J.Heyse, D.G.Jenkins, E.Jericha, Y.Kadi, F.Kappeler, A.Kimura, N.Kivel, M.Kokkoris, Y.Kopatch, S.Kopecky, M.Krticka, D.Kurtulgil, I.Ladarescu, C.Lederer-Woods, J.Lerendegui-Marco, S.Lo Meo, S.-J.Lonsdale, D.Macina, A.Manna, T.Martinez, A.Masi, C.Massimi, P.F.Mastinu, M.Mastromarco, F.Matteucci, E.Maugeri, E.Mendoza, A.Mengoni, V.Michalopoulou, P.M.Milazzo, F.Mingrone, R.Mucciola, A.Musumarra, A.Negret, R.Nolte, F.Ogallar, A.Oprea, N.Patronis, A.Pavlik, J.Perkowski, L.Piersanti, I.Porras, J.Praena, J.M.Quesada, D.Radeck, D.Ramos Doval, R.Reifarth, D.Rochman, C.Rubbia, M.Sabate-Gilarte, A.Saxena, P.Schillebeeckx, D.Schumann, A.G.Smith, N.Sosnin, A.Stamatopoulos, G.Tagliente, J.L.Tain, Z.Talip, A.E.Tarifeno-Saldivia, L.Tassan-Got, P.Torres-Sanchez, A.Tsinganis, J.Ulrich, S.Urlass, S.Valenta, G.Vannini, V.Variale, P.Vaz, A.Ventura, D.Vescovi, V.Vlachoudis, R.Vlastou, A.Wallner, P.J.Woods, R.Wynants, T.J.Wright, P.Zugec Measurement of the 154Gd(n, γ) cross section and its astrophysical implications NUCLEAR REACTIONS 154Gd(n, γ), E=0.001-300 keV; measured reaction products, En, In, Eγ, Iγ; deduced capture yields, transmissions, capture σ. Comparison with ENDF/B-VIII library and KADoNiS.
doi: 10.1016/j.physletb.2020.135405
2020ZH21 Phys.Rev. C 101, 064618 (2020) X.Zhao, W.Sun, R.Capote, E.Sh.Soukhovitskih, D.S.Martyanov, J.M.Quesada Dispersive optical model description of nucleon scattering on Pb and Bi isotopes NUCLEAR REACTIONS 208Pb(n, X), E=6-16 MeV; 206,207,208Pb, 209Bi(n, X), E=0.3-200 MeV; calculated total reactions σ(E). 206Pb(n, n), E=2.53, 4.6, 8, 11.01, 13.7, 21.6 MeV; 207Pb(n, n), E=1.47, 2.02, 2.53, 3.04, 3.56, 13.7 MeV; 209Bi(n, n), E=3.99, 5.5, 7.5, 11, 20, 24 MeV; 209Bi(p, p), E=16, 38.7, 55, 57, 65, 153 MeV; calculated elastic scattering differential σ(E, θ). 208Pb(polarized n, n), E=5.969, 6.967, 7.962, 8.958, 9.95, 13.9 MeV; 208Pb(p, p), E=16, 65, 79.8, 98, 160, 182 MeV; 209Bi(n, n), E=3, 3.5, 4, 4.5, 6, 9 MeV; 209Bi(p, p), E=10.76, 12.96, 16, 65, 78, 153 MeV; calculated analyzing power Ay(E, θ). 208Pb(p, n), E=25.8, 35, 45 MeV; 206Pb(p, n), E=25.8 MeV; 209Bi(p, n), E=27 MeV; calculated quasielastic differential σ(E, θ). Modified dispersive optical model potential (DOMP). Comparison with experimental data, and with other theoretical calculations. 208Pb; calculated neutron single-particle energies, spectroscopic factors of valence-neutron-particle states and valence-neutron-hole states. Comparison with experimental data for energies, and with other theoretical calculations.
doi: 10.1103/PhysRevC.101.064618
2019GU06 Nucl.Instrum.Methods Phys.Res. A925, 87 (2019) C.Guerrero, J.Lerendegui-Marco, K.Eberhardt, Ch.E.Dullmann, A.Junghans, B.Lommel, C.Mokry, J.M.Quesada, J.Runke, P.Thorle-Pospiech, for the n_TOF Collaboration On the use of stacks of fission-like targets for neutron capture experiments
doi: 10.1016/j.nima.2019.01.063
2019GU28 Phys.Lett. B 797, 134809 (2019); Erratum Phys.Lett. B 802, 135268 (2020) C.Guerrero, M.Tessler, M.Paul, J.Lerendegui-Marco, S.Heinitz, E.A.Maugeri, C.Domingo-Pardo, R.Dressler, S.Halfon, N.Kivel, U.Koster, T.Palchan-Hazan, J.M.Quesada, D.Schumann, L.Weissman The s-process in the Nd-Pm-Sm region: Neutron activation of 147Pm NUCLEAR REACTIONS 147Pm, 197Au(n, γ), E ∼ 40 keV; measured reaction products, Eγ, Iγ; deduced Maxwellian averaged σ. Comparison with available data.
doi: 10.1016/j.physletb.2019.134809
2019LE04 Phys.Lett. B 790, 458 (2019); Erratum Phys.Lett. B 840, 137835 (2023) C.Lederer-Woods, U.Battino, P.Ferreira, A.Gawlik, C.Guerrero, F.Gunsing, S.Heinitz, J.Lerendegui-Marco, A.Mengoni, R.Reifarth, A.Tattersall, S.Valenta, C.Weiss, O.Aberle, J.Andrzejewski, L.Audouin, V.Becares, M.Bacak, J.Balibrea, M.Barbagallo, S.Barros, F.Becvar, C.Beinrucker, F.Belloni, E.Berthoumieux, J.Billowes, D.Bosnar, M.Brugger, M.Caamano, F.Calvino, M.Calviani, D.Cano-Ott, F.Cerutti, E.Chiaveri, N.Colonna, G.Cortes, M.A.Cortes-Giraldo, L.Cosentino, L.A.Damone, K.Deo, M.Diakaki, M.Dietz, C.Domingo-Pardo, R.Dressler, E.Dupont, I.Duran, B.Fernandez-Dominguez, A.Ferrari, P.Finocchiaro, R.J.W.Frost, V.Furman, K.Gobel, A.R.Garcia, I.Gheorghe, T.Glodariu, I.F.Goncalves, E.Gonzalez-Romero, A.Goverdovski, E.Griesmayer, H.Harada, T.Heftrich, A.Hernandez-Prieto, J.Heyse, D.G.Jenkins, E.Jericha, F.Kappeler, Y.Kadi, T.Katabuchi, P.Kavrigin, V.Ketlerov, V.Khryachkov, A.Kimura, N.Kivel, I.Knapova, M.Kokkoris, M.Krticka, E.Leal-Cidoncha, H.Leeb, M.Licata, S.Lo Meo, R.Losito, D.Macina, J.Marganiec, T.Martinez, C.Massimi, P.Mastinu, M.Mastromarco, F.Matteucci, E.Mendoza, P.M.Milazzo, F.Mingrone, M.Mirea, S.Montesano, A.Musumarra, R.Nolte, F.R.Palomo-Pinto, C.Paradela, N.Patronis, A.Pavlik, J.Perkowski, J.I.Porras, J.Praena, J.M.Quesada, T.Rauscher, A.Riego-Perez, M.Robles, C.Rubbia, J.A.Ryan, M.Sabate-Gilarte, A.Saxena, P.Schillebeeckx, S.Schmidt, D.Schumann, P.Sedyshev, A.G.Smith, A.Stamatopoulos, S.V.Suryanarayana, G.Tagliente, J.L.Tain, A.Tarifeno-Saldivia, L.Tassan-Got, A.Tsinganis, G.Vannini, V.Variale, P.Vaz, A.Ventura, V.Vlachoudis, R.Vlastou, A.Wallner, S.Warren, M.Weigand, T.Wright, P.Zugec Measurement of 73Ge(n, γ) cross sections and implications for stellar nucleosynthesis NUCLEAR REACTIONS 73Ge(n, γ), E<300 keV; measured reaction products, En, In; deduced σ, resonance energies and capture kernels, astrophysical impact, Maxwellian-averaged σ for ground and excited states capture. The neutron time-of-flight facility n_TOF at CERN.
doi: 10.1016/j.physletb.2019.01.045
2019LE09 Eur.Phys.J. A 55, 63 (2019) J.Lerendegui-Marco, C.Guerrero, T.Belgya, B.Maroti, K.Eberhardt, Ch.E.Dullmann, A.R.Junghans, C.Mokry, J.M.Quesada, J.Runke, P.Thorle-Pospiech Improved 242Pu(n, γ) thermal cross section combining activation and prompt gamma analysis NUCLEAR REACTIONS 242Pu(n, γ), E=thermal, keV; measured prompt Eγ, Iγ using BGO guarded coaxial n-type HPGe, digitized by PC-driven Multi Channel Analyser (MCA), activation Eγ, Iγ using DOME, low background chamber with HPGe inside. 197Au(n, γ), E not given; measured activation Eγ, Iγ using DOME, start and stop time after irradiation; deduced absolute intensities of 243Pu and 198Au decay lines, T1/2; compared with its evaluated value.
doi: 10.1140/epja/i2019-12730-6
2019ZH56 J.Phys.(London) G46, 055103 (2019) X.Zhao, W.Sun, E.S.Soukhovitskii, D.S.Martyanov, J.M.Quesada, R.Capote Analysis of neutron bound states of 208Pb by a dispersive optical model potential NUCLEAR REACTIONS 208Pb(n, X), (n, n), E<100 MeV; analyzed available data. 208Pb; calculated energy levels, J, π using Bear-Hodgon(BH) and Woods-Saxon potentials, rms radii of valence neutron particle and hole states, σ, σ(θ) using the real dispersive optical model potential for nucleon scattering; deduced optical model parameters.
doi: 10.1088/1361-6471/ab0010
2017GU12 Eur.Phys.J. A 53, 87 (2017) C.Guerrero, C.Domingo-Pardo, F.Kappeler, J.Lerendegui-Marco, F.R.Palomo, J.M.Quesada, R.Reifarth Prospects for direct neutron capture measurements on s-process branching point isotopes
doi: 10.1140/epja/i2017-12261-2
2017MA15 Phys.Lett. B 768, 1 (2017) C.Massimi, S.Altstadt, J.Andrzejewski, L.Audouin, M.Barbagallo, V.Becares, F.Becvar, F.Belloni, E.Berthoumieux, J.Billowes, S.Bisterzo, D.Bosnar, M.Brugger, M.Calviani, F.Calvino, D.Cano-Ott, C.Carrapico, D.M.Castelluccio, F.Cerutti, E.Chiaveri, L.Cosentino, M.Chin, G.Clai, N.Colonna, G.Cortes, M.A.Cortes-Giraldo, S.Cristallo, M.Diakaki, C.Domingo-Pardo, I.Duran, R.Dressler, C.Eleftheriadis, A.Ferrari, P.Finocchiaro, K.Fraval, S.Ganesan, A.R.Garcia, G.Giubrone, I.F.Goncalves, E.Gonzalez-Romero, E.Griesmayer, C.Guerrero, F.Gunsing, A.Hernandez-Prieto, D.G.Jenkins, E.Jericha, Y.Kadi, F.Kappeler, D.Karadimos, N.Kivel, P.Koehler, M.Kokkoris, S.Kopecky, M.Krticka, J.Kroll, C.Lampoudis, C.Langer, E.Leal-Cidoncha, C.Lederer, H.Leeb, L.S.Leong, S.Lo Meo, R.Losito, A.Mallick, A.Manousos, J.Marganiec, T.Martinez, P.F.Mastinu, M.Mastromarco, E.Mendoza, A.Mengoni, P.M.Milazzo, F.Mingrone, M.Mirea, W.Mondelaers, A.Musumarra, C.Paradela, A.Pavlik, J.Perkowski, M.Pignatari, L.Piersanti, A.Plompen, J.Praena, J.M.Quesada, T.Rauscher, R.Reifarth, A.Riego, M.S.Robles, C.Rubbia, M.Sabate-Gilarte, R.Sarmento, A.Saxena, P.Schillebeeckx, S.Schmidt, D.Schumann, G.Tagliente, J.L.Tain, D.Tarrio, L.Tassan-Got, A.Tsinganis, S.Valenta, G.Vannini, I.Van Rijs, V.Variale, P.Vaz, A.Ventura, M.J.Vermeulen, V.Vlachoudis, R.Vlastou, A.Wallner, T.Ware, M.Weigand, C.Weiss, R.Wynants, T.Wright, P.Zugec Neutron spectroscopy of 26Mg states: Constraining the stellar neutron source 22Ne(α, n)25Mg NUCLEAR REACTIONS 25Mg(n, γ), (n, X), E<300 KeV; measured reaction products, En, In, Eγ, Iγ; deduced yields, σ, resonance parameters and corresponding excitation energies of the 26Mg compound nucleus, Maxwellian-averaged cross sections, reaction rates for inverse reactions. R-matrix analysis of the experimental data.
doi: 10.1016/j.physletb.2017.02.025
2017MA52 Chin.Phys.C 41, 094105 (2017) D.S.Martyanov, E.Sh.Soukhovitskii, R.Capote, J.M.Quesada, S.Chiba Predicting the optical observables for nucleon scattering on even-even actinides NUCLEAR REACTIONS 228,230,232Th, 232,234,236,238U, 238,240,242,244Pu, 246,248Cm, 250Cf(n, X), E<200 MeV; analyzed available data; deduced extended Lane consistent dispersive coupled-channel optical model for nucleon scattering.
doi: 10.1088/1674-1137/41/9/094105
2016LE07 Eur.Phys.J. A 52, 100 (2016) J.Lerendegui-Marco, S.Lo Meo, C.Guerrero, M.A.Cortes-Giraldo, C.Massimi, J.M.Quesada, M.Barbagallo, N.Colonna, D.Mancusi, F.Mingrone, M.Sabate-Gilarte, G.Vannini, V.Vlachoudis, for the n_TOF Collaboration Geant4 simulation of the n_TOF-EAR2 neutron beam: Characteristics and prospects
doi: 10.1140/epja/i2016-16100-8
2016SO16 Phys.Rev. C 94, 064605 (2016); Erratum Phys.Rev. C 102, 059901 (2020) E.Sh.Soukhovitskii, R.Capote, J.M.Quesada, S.Chiba, D.S.Martyanov Nucleon scattering on actinides using a dispersive optical model with extended couplings NUCLEAR REACTIONS 233,235,238U, 232Th(n, X), E=0.001-200 MeV; calculated total σ(E) using dispersive potential with multiple-band couplings, compound-nucleus formation cross section using the rigid-rotor RIPL 2408 potential and the potential derived in the present work. Dispersive isospin-dependent coupled-channels optical model analysis, and extended Tamura's coupling formalism for low-lying bands of vibrational nature in even-even and single-particle nature in odd-A actinides. Comparison with experimental data and with RIPL 2408 potential. 232Th, 233,235,238U, 239Pu; calculated average resonance parameters using derived optical model potential, and compared with experimental data and with RIPL 2408 potential and evaluated data, ground-state deformation parameters β2, β4 and β6, and interband effective coupling parameters.
doi: 10.1103/PhysRevC.94.064605
2015LO12 Eur.Phys.J. A 51, 160 (2015) S.Lo Meo, M.A.Cortes-Giraldo, C.Massimi, J.Lerendegui-Marco, M.Barbagallo, N.Colonna, C.Guerrero, D.Mancusi, F.Mingrone, J.M.Quesada, M.Sabate-Gilarte, G.Vannini, V.Vlachoudis, for the n_TOF Collaboration GEANT4 simulations of the n_TOF spallation source and their benchmarking
doi: 10.1140/epja/i2015-15160-6
2014PO06 Nucl.Data Sheets 120, 246 (2014) I.Porras, M.Sabate-Gilarte, J.Praena, J.M.Quesada, P.L.Esquinas 33S for Neutron Capture Therapy: Nuclear Data for Monte Carlo Calculations NUCLEAR REACTIONS 33S(n, α), E not given; analyzed available data.; deduced data discrepancies.
doi: 10.1016/j.nds.2014.07.058
2014PR07 Nucl.Data Sheets 120, 205 (2014) J.Praena, P.F.Mastinu, M.Pignatari, J.M.Quesada, R.Capote, Y.Morilla Measurement of the MACS of 159Tb(n, γ) at kT=30 keV by Activation NUCLEAR REACTIONS 159Tb(n, γ), E=30 keV; measured reaction products, Eγ, Iγ.; deduced Maxwellian-averaged σ. Comparison with available data, ENDF/B-VII.1 and KADoNiS libraries.
doi: 10.1016/j.nds.2014.07.047
2014QU02 Nucl.Data Sheets 118, 270 (2014) J.M.Quesada, R.Capote, E.Sh.Soukhovitskii, S.Chiba Rotational-vibrational Description of Nucleon Scattering on Actinide Nuclei Using a Dispersive Coupled-channel Optical Model NUCLEAR REACTIONS 232Th, 238U(p, x), E=threshold-100 MeV; calculated total σ using DCCOMP (dispersive optical model with different types of rotational bands). Compared with data and calculations with RIPL potentials.
doi: 10.1016/j.nds.2014.04.055
2014SU13 Nucl.Data Sheets 118, 191 (2014) W.Sun, R.Li, E.S.Soukhovitskii, J.M.Quesada, R.Capote A Fully Lane-consistent Dispersive Optical Model Potential for Even Fe Isotopes Based on a Soft-rotator Model NUCLEAR REACTIONS 54,56Fe(n, n), E=0-20 MeV; calculated σ using DCCOM (Lane-consistent dispersive CC optical model); deduced optical model parameters. Cross sections compared to data. 54Fe(n, n'), E=9.9-16.9 MeV;54Fe(p, p'), E=10.0=40.0 MeV;56Fe(n, n'), E=9.993 MeV;56Fe(p, p'), E=17.2-65.0 MeV; calculated analyzing power to discrete states. Compared to data. NUCLEAR STRUCTURE 54,58Fe; calculated collective levels, J, π using soft rotator model. Compared with data.
doi: 10.1016/j.nds.2014.04.034
2013LI22 Phys.Rev. C 87, 054611 (2013) R.Li, W.Sun, E.Sh.Soukhovitskih, J.M.Quesada, R.Capote Dispersive coupled-channels optical-model potential with soft-rotator couplings for Cr, Fe, and Ni isotopes NUCLEAR REACTIONS 52Cr, 54,56,58Fe, 59,60,62Ni(n, X), E=0.1-200 MeV; calculated total cross sections and compared with measurements. 54Fe(n, n), E=7.0, 7.96, 8.5, 9.94, 11.0, 11.93, 13.92, 14.7, 16.93, 20.0, 22.0, 24.0, 26.0 MeV; 54Fe(n, n'), E=13.92, 16.93, 20.0, 22.0, 24.0, 26.0 MeV; 56Fe(n, n), E=7.96, 9.94, 11.0, 11.93, 14.0, 14.7, 20.0, 26.0, 55.0, 65.0, 96.0 MeV; 56Fe(n, n'), E=7.96, 9.94, 11.0, 11.93, 13.92, 15.20, 21.1, 26.0 MeV; 54Fe(p, p), E=19.6, 20.4, 24.6, 28.8, 30.4, 35.2, 38.8, 39.7, 40.0, 61.5, 65.0 MeV; 54Fe(p, p'), E=17.9, 18.6, 30.4, 39.7, 40.0, 61.5, 65.0 MeV; 56Fe(p, p), E=7.74, 10.93, 17.2, 19.1, 20.4, 24.6, 30.3, 35.2, 39.8, 61.5, 65.0, 156.0 MeV; 56Fe(p, p'), E=17.2, 19.1, 61.5, 65.0 MeV; 58Fe(p, p), E=6.0, 10.93, 11.66, 22.2, 35.2 MeV; 58Fe(p, p'), E=10.93, 11.66, 17.5, 49.35 MeV; calculated differential σ(θ) and compared with experimental data. 52Cr, 54,56,58Fe, 59,60,62Ni(p, p'), E=1-200 MeV; calculated inelastic cross sections and compared with measurements. 52Cr(p, n), E=17.3, 18.0, 120.0 MeV; 54Fe(p, n), E=23.0, 35.0, 135.0 MeV; 56Fe(p, n), E=17.0, 23.0, 35.2 MeV; 58Fe(p, n), E=23.0, 120.0 MeV; 58Ni(p, n), E=23.0, 32.0, 35.0 MeV; 62Ni(p, n), E=16.0, 22.8, 35.0 MeV; calculated σ(θ) for transition exciting IAS and EAS. 54Fe(polarized p, p), E=10.0, 14.0, 18.6, 30.4, 40.0, 65.0 MeV; 56Fe(polarized p, p), E=5.77, 14.0, 18.6, 24.6, 30.3, 65.0, 179.0 MeV; 58Fe(polarized p, p), E=5.85, 6.51, 14.0, 14.5 MeV; 58Ni(polarized p, p), E=20.9, 30.3, 40.0, 65.0, 172.0 MeV; 54Fe(polarized n, n), (polarized n, n'), E=9.941, 13.9, 13.94, 16.93 MeV; 56Fe(polarized n, n), (polarized n, n'), E=9.993 MeV; 57Fe(polarized p, p), E=5.88, 6.15, 6.51, 14.0 MeV; 58Fe(polarized n, n), E=9.92, 13.91, 16.93 MeV; 54Fe(polarized p, p'), E=10.0, 18.6, 30.4, 40.0 MeV; 56Fe(polarized p, p'), E=17.2, 18.6, 20.4, 24.6, 65.0, 179.0 MeV; 58Ni(polarized p, p'), E=20.4, 24.6, 40.0, 57.5, 60.2, 178.0 MeV; calculated analyzing powers and compared with experimental data, and with TALYS calculations, including DWBA. Derived approximate Lane-consistent dispersive coupled-channels optical potential. NUCLEAR STRUCTURE 54,56,58Fe; analyzed levels, J, π; assigned soft-rotor model (SRM) quantum numbers and Hamiltonian parameters. Coupled-channels optical model analysis using matrix elements derived by the soft-rotator model.
doi: 10.1103/PhysRevC.87.054611
2013PR06 Nucl.Instrum.Methods Phys.Res. A727, 1 (2013) J.Praena, P.F.Mastinu, M.Pignatari, J.M.Quesada, J.Garcia-Lopez, M.Lozano, N.Dzysiuk, R.Capote, G.Martin-Hernandez Measurement of the MACS of 181Ta(n, γ) at kT=30 KeV as a test of a method for Maxwellian neutron spectra generation NUCLEAR REACTIONS 181Ta, 197Au(n, γ), E<120 keV; measured reaction products, Eγ, Iγ; deduced Maxwellian-averaged σ. Comparison with experimental results, ENDF libraries.
doi: 10.1016/j.nima.2013.05.151
2011LE31 J.Korean Phys.Soc. 59, 1019s (2011) J.-Y.Lee, E.Sh.Soukhovitskii, Y.Kim, R.Capote, S.Chiba, J.M.Quesada Self-Consistent Analyses of Nuclear Level Structures, and Nucleon Interaction Data of Even-even Sn Isotopes NUCLEAR REACTIONS 120Sn(n, n), E=0.1-200 MeV;120Sn(n, p), E=10-200 Mev; calculated σ; 120Sn(n, n), (n, n'), E=0.94, 11.0, 13.9, 16.1 MeV;120Sn(p, p), E=9.7, 16.0, 20.4, 24.6, 30.3, 40.0, 61.5, 100.4, 134.7, 156.0 MeV;120Sn(p, p'), E=20.4, 24.6, 61.5 MeV; calculated σ(θ); 116Sn(p, n), E=22.8 MeV;118Sn(p, n), E=22.8, 25 MeV;120Sn(p, n), E=22.8, 25, 35, 45 MeV; calculated σ(θ). Deduced optical potential parameters. Soft-rotator model, coupled-channels optical model with dispersive Lane-consistent potential. Comparison with data. NUCLEAR STRUCTURE 120Sn; calculated levels, J, π, rotational band using soft-rotator model. Comparison with data.
doi: 10.3938/jkps.59.1019
2008CA32 J.Nucl.Sci.Technol.(Tokyo) 45, 333 (2008) R.Capote, S.Chiba, E.Sh.Soukhovitskii, J.M.Quesada, E.Bauge A Global Dispersive Coupled-Channel Optical Model Potential for Actinides
doi: 10.1080/18811248.2008.9711442
2007OK01 Phys.Rev. C 75, 034616 (2007) N.T.Okumusoglu, F.Korkmaz Gorur, J.Birchall, E.Sh.Soukhovitskii, R.Capote, J.M.Quesada, S.Chiba Angular distributions of protons scattered by 40Ar nuclei with excitation of the 2+(1.46 MeV) and 3-(3.68 MeV) collective levels for incident energies of 25.1, 32.5, and 40.7 MeV NUCLEAR REACTIONS 40Ar(p, p), (p, p'), E=25.1, 32.5, 40.7 MeV; measured σ(E, θ), Ay(θ). 40Ar deduced deformation parameters. Isospin dependent soft-rotator coupled-channels optical model analysis.
doi: 10.1103/PhysRevC.75.034616
2007QU04 Phys.Rev. C 76, 057602 (2007) J.M.Quesada, R.Capote, E.Sh.Soukhovitskii, S.Chiba Approximate Lane consistency of the dispersive coupled-channels potential for actinides NUCLEAR REACTIONS 238U, 232Th(p, n), E=26 MeV; calculated angular distributions, compared with experimental data.
doi: 10.1103/PhysRevC.76.057602
2005CA27 Phys.Rev. C 71, 064320 (2005) R.Capote, A.Ventura, F.Cannata, J.M.Quesada Level densities of transitional Sm nuclei NUCLEAR STRUCTURE 148,149,150,152Sm; calculated level densities, resonance spacing. Interacting boson model, comparison with data.
doi: 10.1103/PhysRevC.71.064320
2005CA56 Phys.Rev. C 72, 064610 (2005) R.Capote, E.Sh.Soukhovitskii, J.M.Quesada, S.Chiba Is a global coupled-channel dispersive optical model potential for actinides feasible? NUCLEAR REACTIONS 232Th, 238U(n, X), (p, X), E=0.001-200 MeV; analyzed data; deduced parameters. Dispersive coupled-channels optical model.
doi: 10.1103/PhysRevC.72.064610
2005SU16 Phys.Rev. C 72, 024604 (2005) E.Sh.Sukhovitskii, R.Capote, J.M.Quesada, S.Chiba Dispersive coupled-channel analysis of nucleon scattering from 232Th up to 200 MeV NUCLEAR REACTIONS 232Th(n, X), (p, X), E=0.001-200 MeV; analyzed σ, σ(θ); deduced optical model parameters. Dispersive isospin-dependent relativistic coupled-channels optical model analysis.
doi: 10.1103/PhysRevC.72.024604
2003QU01 Comput.Phys.Commun. 153, 97 (2003) J.M.Quesada, R.Capote, A.Molina, M.Lozano Dispersion relations in the nuclear optical model
doi: 10.1016/S0010-4655(03)00157-7
2003QU02 Phys.Rev. C 67, 067601 (2003) J.M.Quesada, R.Capote, A.Molina, M.Lozano, J.Raynal Analytical expressions for the dispersive contributions to the nucleon-nucleus optical potential
doi: 10.1103/PhysRevC.67.067601
2002LH01 Phys.Rev. C65, 024318 (2002) G.Lhersonneau, B.Pfeiffer, R.Capote, J.M.Quesada, H.Gabelmann, K.-L.Kratz, and the ISOLDE Collaboration A K = 3 Two-Quasiparticle Isomer in 98Sr RADIOACTIVITY 98Rb, 100Y(β-) [from 238U(p, X)]; measured Eγ, Iγ, γγ-coin; deduced log ft. 100Zr(IT) [from 238U(p, X)]; measured Eγ, Iγ, γγ-coin. 98Sr deduced levels, J, π, configurations, isomeric state. 100Zr deduced levels, J, π. Mass separated source. Quantum Monte Carlo pairing calculation.
doi: 10.1103/PhysRevC.65.024318
2002MO09 Phys.Rev. C65, 034616 (2002) A.Molina, R.Capote, J.M.Quesada, M.Lozano Dispersive Spherical Optical Model of Neutron Scattering from 27Al up to 250 MeV NUCLEAR REACTIONS 27Al(n, n), E=0.1-250 MeV; calculated σ, σ(θ), Ay(θ); deduced nonlocality effects. Dispersive spherical optical model, relativistic kinematics, comparison with data.
doi: 10.1103/PhysRevC.65.034616
2001CA41 J.Phys.(London) G27, B15 (2001) R.Capote, A.Molina, J.M.Quesada A General Numerical Solution of Dispersion Relations for the Nuclear Optical Model
doi: 10.1088/0954-3899/27/8/402
1985AN16 Nucl.Phys. A443, 380 (1985) M.V.Andres, J.M.Quesada, M.Lozano, G.Madurga A Level-Density-Dependent Imaginary Potential for Heavy Ions NUCLEAR REACTIONS 28Si, 40Ca(9Be, 9Be), E=14-26 MeV; 24Mg(12C, 12C), E=21, 24 MeV; 24Mg(16O, 16O), E=28-33 MeV; 40Ca(20Ne, 20Ne), E=44.1-70.4 MeV; 40Ca(32S, 32S), E=100-151.5 MeV; calculated real folding potential renormalization constants, σ(θ). Level density dependent heavy ion potential component. NUCLEAR STRUCTURE 9Be, 12C, 16O, 20Ne, 24Mg, 28Si, 32S, 40Ca; calculated neutron, proton, charge density distributions. Woods-Saxon potential.
doi: 10.1016/0375-9474(85)90269-6
1985BR26 Yad.Fiz. 42, 1114 (1985) Anomalous Scattering of 16O Ions on 28,29,30Si Nuclei and the Shell Structure of Silicon Isotopes NUCLEAR REACTIONS 28,29,30Si(16O, 16O), E=54.7, 60 MeV; analyzed σ(θ); deduced optical model parameters. 28,29,30Si deduced shell structure. Microscopic approach.
1985QU02 Nucl.Phys. A442, 381 (1985) J.M.Quesada, G.Pollarolo, R.A.Broglia, A.Winther A Simple Parametrization of One-Particle Transfer Form Factors for Heavy-Ion Reactions NUCLEAR REACTIONS 208Pb, 40Ca(16O, 15O), 114Sn(36Ar, 35Cl), 208Pb(160Dy, 159Tb), E not given; calculated single particle form factors. 28,29,30Si(16O, 16O), E=33, 54.7 MeV; calculated absorptive potential radial separation. Simple parameterization, one particle transfer. NUCLEAR STRUCTURE A=16-250; calculated single particle state normalizations, effective wave number vs mass.
doi: 10.1016/0375-9474(85)90151-4
1984QU03 Nucl.Phys. A428, 305c (1984) J.M.Quesada, R.A.Broglia, V.Bragin, G.Pollarolo Single-Particle and Collective Aspects of the Absorptive Potential for Heavy Ion Reactions NUCLEAR REACTIONS 28,29,30Si(16O, X), 28Si(17O, X), E=33 MeV; calculated absorptive potential parameters; deduced transfer process induced mass dependence.
doi: 10.1016/0375-9474(84)90259-8
1983QU01 Phys.Lett. 125B, 14 (1983) J.M.Quesada, M.Lozano, G.Madurga A Phenomenological Imaginary Part of the Optical Potential for Heavy Ions NUCLEAR REACTIONS 28Si(16O, 16O), E=33-81 MeV; calculated σ(θ). Optical potential, phenomenological imaginary part.
doi: 10.1016/0370-2693(83)91224-8
Back to query form |