NSR Query Results
Output year order : Descending NSR database version of April 24, 2024. Search: Author = M.Martini Found 50 matches. 2023AB32 Phys.Rev. D 108, 092009 (2023) K.Abe, N.Akhlaq, R.Akutsu, A.Ali, S.Alonso Monsalve, C.Alt, C.Andreopoulos, M.Antonova, S.Aoki, T.Arihara, Y.Asada, Y.Ashida, E.T.Atkin, M.Barbi, G.J.Barker, G.Barr, D.Barrow, M.Batkiewicz-Kwasniak, V.Berardi, L.Berns, S.Bhadra, A.Blanchet, A.Blondel, S.Bolognesi, T.Bonus, S.Bordoni, S.B.Boyd, A.Bravar, C.Bronner, S.Bron, A.Bubak, M.Buizza Avanzini, J.A.Caballero, N.F.Calabria, S.Cao, D.Carabadjac, A.J.Carter, S.L.Cartwright, M.P.Casado, M.G.Catanesi, A.Cervera, J.Chakrani, D.Cherdack, P.S.Chong, G.Christodoulou, A.Chvirova, M.Cicerchia, J.Coleman, G.Collazuol, L.Cook, A.Cudd, C.Dalmazzone, T.Daret, Yu.I.Davydov, A.De Roeck, G.De Rosa, T.Dealtry, C.C.Delogu, C.Densham, A.Dergacheva, F.Di Lodovico, S.Dolan, D.Douqa, T.A.Doyle, O.Drapier, J.Dumarchez, P.Dunne, K.Dygnarowicz, A.Eguchi, S.Emery-Schrenk, G.Erofeev, A.Ershova, G.Eurin, D.Fedorova, S.Fedotov, M.Feltre, A.J.Finch, G.A.Fiorentini Aguirre, G.Fiorillo, M.D.Fitton, J.M.Franco Patino, M.Friend, Y.Fujii, Y.Fukuda, Y.Furui, L.Giannessi, C.Giganti, V.Glagolev, M.Gonin, J.Gonzalez Rosa, E.A.G.Goodman, A.Gorin, M.Grassi, M.Guigue, D.R.Hadley, J.T.Haigh, P.Hamacher-Baumann, D.A.Harris, M.Hartz, T.Hasegawa, S.Hassani, N.C.Hastings, Y.Hayato, D.Henaff, M.Hogan, J.Holeczek, A.Holin, T.Holvey, N.T.Hong Van, T.Honjo, A.K.Ichikawa, M.Ikeda, T.Ishida, M.Ishitsuka, H.T.Israel, A.Izmaylov, M.Jakkapu, B.Jamieson, S.J.Jenkins, C.Jesus-Valls, J.J.Jiang, J.Y.Ji, P.Jonsson, S.Joshi, C.K.Jung, P.B.Jurj, M.Kabirnezhad, A.C.Kaboth, T.Kajita, H.Kakuno, J.Kameda, S.P.Kasetti, Y.Kataoka, T.Katori, M.Kawaue, E.Kearns, M.Khabibullin, A.Khotjantsev, T.Kikawa, S.King, V.Kiseeva, J.Kisiel, H.Kobayashi, T.Kobayashi, L.Koch, S.Kodama, A.Konaka, L.L.Kormos, Y.Koshio, T.Koto, K.Kowalik, Y.Kudenko, Y.Kudo, S.Kuribayashi, R.Kurjata, T.Kutter, M.Kuze, M.La Commara, L.Labarga, K.Lachner, J.Lagoda, S.M.Lakshmi, M.Lamers James, M.Lamoureux, A.Langella, J.-F.Laporte, D.Last, N.Latham, M.Laveder, L.Lavitola, M.Lawe, Y.Lee, C.Lin, S.-K.Lin, R.P.Litchfield, S.L.Liu, W.Li, A.Longhin, K.R.Long, A.Lopez Moreno, L.Ludovici, X.Lu, T.Lux, L.N.Machado, L.Magaletti, K.Mahn, M.Malek, M.Mandal, S.Manly, A.D.Marino, L.Marti-Magro, D.G.R.Martin, M.Martini, J.F.Martin, T.Maruyama, T.Matsubara, V.Matveev, C.Mauger, K.Mavrokoridis, E.Mazzucato, N.McCauley, J.McElwee, K.S.McFarland, C.McGrew, J.McKean, A.Mefodiev, G.D.Megias, P.Mehta, L.Mellet, C.Metelko, M.Mezzetto, E.Miller, A.Minamino, O.Mineev, S.Mine, M.Miura, L.Molina Bueno, S.Moriyama, S.Moriyama, P.Morrison, Th.A.Mueller, D.Munford, L.Munteanu, K.Nagai, Y.Nagai, T.Nakadaira, K.Nakagiri, M.Nakahata, Y.Nakajima, A.Nakamura, H.Nakamura, K.Nakamura, K.D.Nakamura, Y.Nakano, S.Nakayama, T.Nakaya, K.Nakayoshi, C.E.R.Naseby, T.V.Ngoc, V.Q.Nguyen, K.Niewczas, S.Nishimori, Y.Nishimura, K.Nishizaki, T.Nosek, F.Nova, P.Novella, J.C.Nugent, H.M.O'Keeffe, L.O'Sullivan, T.Odagawa, W.Okinaga, K.Okumura, T.Okusawa, N.Ospina, Y.Oyama, V.Palladino, V.Paolone, M.Pari, J.Parlone, J.Pasternak, M.Pavin, D.Payne, G.C.Penn, D.Pershey, L.Pickering, C.Pidcott, G.Pintaudi, C.Pistillo, B.Popov, K.Porwit, M.Posiadala-Zezula, Y.S.Prabhu, F.Pupilli, B.Quilain, T.Radermacher, E.Radicioni, B.Radics, M.A.Ramirez, P.N.Ratoff, M.Reh, C.Riccio, E.Rondio, S.Roth, N.Roy, A.Rubbia, A.C.Ruggeri, C.A.Ruggles, A.Rychter, K.Sakashita, F.Sanchez, C.M.Schloesser, K.Scholberg, M.Scott, Y.Seiya, T.Sekiguchi, H.Sekiya, D.Sgalaberna, A.Shaikhiev, F.Shaker, M.Shiozawa, W.Shorrock, A.Shvartsman, N.Skrobova, K.Skwarczynski, D.Smyczek, M.Smy, J.T.Sobczyk, H.Sobel, F.J.P.Soler, Y.Sonoda, A.J.Speers, R.Spina, I.A.Suslov, S.Suvorov, A.Suzuki, S.Y.Suzuki, Y.Suzuki, M.Tada, S.Tairafune, S.Takayasu, A.Takeda, Y.Takeuchi, K.Takifuji, H.K.Tanaka, M.Tani, A.Teklu, V.V.Tereshchenko, N.Thamm, L.F.Thompson, W.Toki, C.Touramanis, T.Towstego, K.M.Tsui, T.Tsukamoto, M.Tzanov, Y.Uchida, M.Vagins, D.Vargas, M.Varghese, G.Vasseur, C.Vilela, E.Villa, W.G.S.Vinning, U.Virginet, T.Vladisavljevic, T.Wachala, J.G.Walsh, Y.Wang, L.Wan, D.Wark, M.O.Wascko, A.Weber, R.Wendell, M.J.Wilking, C.Wilkinson, J.R.Wilson, K.Wood, C.Wret, J.Xia, Y.-h.Xu, K.Yamamoto, T.Yamamoto, C.Yanagisawa, G.Yang, T.Yano, K.Yasutome, N.Yershov, U.Yevarouskaya, M.Yokoyama, Y.Yoshimoto, N.Yoshimura, M.Yu, R.Zaki, A.Zalewska, J.Zalipska, K.Zaremba, G.Zarnecki, X.Zhao, T.Zhu, M.Ziembicki, E.D.Zimmerman, M.Zito, S.Zsoldos Measurements of the νμ and ν-barμ-induced coherent charged pion production cross sections on 12C by the T2K experiment NUCLEAR REACTIONS 12C(ν, μ-), (ν-bar, μ+), E ∼ 0.8 GeV; measured reaction products; deduced coherent charged pion production σ in the Tokai-to-Kamioka experiment.
doi: 10.1103/PhysRevD.108.092009
2023AL12 Phys.Rev. C 107, 065501 (2023) O.Al Hammal, M.Martini, J.Frontera-Pons, T.H.Nguyen, R.Perez-Ramos Neural network predictions of inclusive electron-nucleus cross sections NUCLEAR REACTIONS 12C, 16O, 40Ar, 40Ca, 48Ti(e, e'), E=0.16-2.2 GeV; calculated σ(θ, E). Prediction of neural networks trained on data from University of Virginia's Quasielastic Electron Nucleus Scattering Archive. Comparison to experimental data and to theoretical results obtained with SuSAv2 and GiBUU theoretical models, as well as to the results from GENIE MonteCarlo event generator.
doi: 10.1103/PhysRevC.107.065501
2023PI06 Phys.Rev. C 108, 055201 (2023) K.Piscicchia, M.Skurzok, M.Cargnelli, R.Del Grande, L.Fabbietti, J.Marton, P.Moskal, A.Ramos, A.Scordo, D.L.Sirghi, O.Vazquez Doce, J.Zmeskal, S.Wycech, P.Branchini, F.Ceradini, E.Czerwinski, E.De Lucia, S.Fiore, A.Kupsc, G.Mandaglio, M.Martini, A.Passeri, V.Patera, E.Perez Del Rio, A.Selce, M.Silarski, C.Curceanu First simultaneous K- p → Σ0π0, Λπ0 cross section measurements at 98 MeV/c
doi: 10.1103/PhysRevC.108.055201
2022MA36 Phys.Rev. C 106, 015503 (2022) M.Martini, M.Ericson, G.Chanfray Investigation of the MicroBooNE neutrino cross sections on argon NUCLEAR REACTIONS 40Ar(ν, X), E<1.2 GeV; analyzed data on σ(E) from MicroBooNE experiment; calculated charged current inclusive flux-integrated single differential σ(E). Random phase approximation (RPA) on top of a local Fermi gas calculation.
doi: 10.1103/PhysRevC.106.015503
2021PE12 Phys.Rev. C 104, 024328 (2021) S.Peru, S.Hilaire, S.Goriely, M.Martini Description of magnetic moments within the Gogny Hartree-Fock-Bogolyubov framework: Application to Hg isotopes NUCLEAR STRUCTURE 177Hg; calculated potential energy curves for different Kπ blockings as a function of quadrupole deformation parameter β, magnetic moments as a function of spectroscopic quadrupole moments. 178,180,182,184,186,188,190,192,194,196,198,200,202,204Hg; calculated quadrupole deformation parameters β and binding energies of the oblate and prolate minima. 177,178,179,180,181,182,183,184,185,186,187,188,189,190,191,192,193,194,195,196,197,198,199,200,201,202,203,204,205,206Hg; calculated isotope shifts and spectroscopic quadrupole moments. Gogny Hartree-Fock-Bogolyubov (HFB) calculations with self-consistent blocking of the unpaired nucleon, and D1M interaction. Comparison with experimental data.
doi: 10.1103/PhysRevC.104.024328
2019MA67 Eur.Phys.J. A 55, 150 (2019) M.Martini, A.De Pace, K.Bennaceur Spurious finite-size instabilities with Gogny-type interactions NUCLEAR STRUCTURE 4He, 48Ca, 120Sn, 208Pb; calculated proton and neutron critical densities vs radius using D1M, D1N and DIM* interactions using fully antisymmetrized RPA; deduced no convergence for 48Ca beyond number of shells Nsh=24 using HFBTHO code.
doi: 10.1140/epja/i2019-12838-7
2019PE23 Eur.Phys.J. A 55, 232 (2019) S.Peru, I.Deloncle, S.Hilaire, S.Goriely, M.Martini Study of dipole excitations in even-even 156-166Dy with QRPA using the Gogny force
doi: 10.1140/epja/i2019-12896-9
2018AL24 Prog.Part.Nucl.Phys. 100, 1 (2018) L.Alvarez-Ruso, M.Sajjad Athar, M.B.Barbaro, D.Cherdack, M.E.Christy, P.Coloma, T.W.Donnelly, S.Dytman, A.de Gouvea, R.J.Hill, P.Huber, N.Jachowicz, T.Katori, A.S.Kronfeld, K.Mahn, M.Martini, J.G.Morfin, J.Nieves, G.N.Perdue, R.Petti, D.G.Richards, F.Sanchez, T.Sato, J.T.Sobczyk, G.P.Zeller NuSTEC1 White Paper: Status and challenges of neutrino-nucleus scattering
doi: 10.1016/j.ppnp.2018.01.006
2018KA06 J.Phys.(London) G45, 013001 (2018) Neutrino-nucleus cross sections for oscillation experiments NUCLEAR REACTIONS 12C(ν, X), E not given; calculated σ. Comparison with experimental data.
doi: 10.1088/1361-6471/aa8bf7
2018NI15 Phys.Rev. C 98, 054603 (2018) A.Nikolakopoulos, M.Martini, M.Ericson, N.Van Dessel, R.Gonzalez-Jimenez, N.Jachowicz Mean-field approach to reconstructed neutrino energy distributions in accelerator-based experiments
doi: 10.1103/PhysRevC.98.054603
2018PI05 Phys.Lett. B 782, 339 (2018) K.Piscicchia, S.Wycech, L.Fabbietti, M.Cargnelli, C.Curceanu, R.Del Grande, J.Marton, P.Moskal, A.Scordo, M.Silarski, D.Sirghi, M.Skurzok, I.Tucakovic, O.Vazquez Doce, J.Zmeskal, P.Branchini, E.Czerwinski, V.De Leo, E.De Lucia, A.Di Cicco, P.Fermani, S.Fiore, W.Krzemien, G.Mandaglio, M.Martini, E.Perez del Rio, A.Selce First measurement of the K-n → Λπ- non-resonant transition amplitude below threshold NUCLEAR REACTIONS 4He(K-, Λ), E ∼ 120 MeV; measured reaction products; deduced yields, resonant to non-resonant ratios and amplitudes of the various channels, momentum distributions. Comparison with phenomenological model.
doi: 10.1016/j.physletb.2018.05.025
2017DE27 Eur.Phys.J. A 53, 170 (2017) Electromagnetic dipole and Gamow-Teller responses of even and odd 90-9440Zr isotopes in QRPA calculations with the D1M Gogny force NUCLEAR STRUCTURE 90,91,92,93,94Zr; calculated B(E1), B(M1) strength distribution for pygmy and giant dipole resonances using HFB + QRPA with D1M Gogny force, magnetic nuclear spin-flip excitations, GT transitions using pnQRPA charge exchange code. Compared to available data.
doi: 10.1140/epja/i2017-12354-x
2017GO14 Phys.Lett. B 772, 359 (2017) A.Gottardo, D.Verney, I.Deloncle, S.Peru, C.Delafosse, S.Roccia, I.Matea, C.Sotty, C.Andreoiu, C.Costache, M.-C.Delattre, A.Etile, S.Franchoo, C.Gaulard, J.Guillot, F.Ibrahim, M.Lebois, M.MacCormick, N.Marginean, R.Marginean, M.Martini, C.Mihai, I.Mitu, L.Olivier, C.Portail, L.Qi, B.Roussiere, L.Stan, D.Testov, J.Wilson, D.T.Yordanov Unexpected high-energy γ emission from decaying exotic nuclei RADIOACTIVITY 80,83Ga(β-); measured decay products, Eγ, Iγ; deduced γ-ray emissions, B(E1), GT β-decay and E1 strength distributions. Comparison with microscopic Gogny-QRPA calculations.
doi: 10.1016/j.physletb.2017.06.050
2017KO20 Phys.Rev. C 95, 054317 (2017) J.Kopecky, S.Goriely, S.Peru, S.Hilaire, M.Martini E1 and M1 strength functions from average resonance capture data NUCLEAR REACTIONS 75As, 91Zr, 95,97Mo, 101Ru, 105Pd, 113Cd, 123Te, 127I, 134,135Ba, 145Nd, 154Sm, 153Eu, 154,155,156,157,158Gd, 161,162,163,164Dy, 165Ho, 167Er, 169Tm, 171,173Yb, 175Lu, 177Hf, 181Ta, 183,184,186W, 187,188,190,192Os, 192,194Ir, 194,195,196,198Pt, 197Au, 232Th, 238U, 239Pu(n, γ), E=2, 24 keV; analyzed average resonance capture (ARC) data measured at different filter beam facilities ANL, INEL, and BNL between 1970 and 1990; deduced E1 and M1 photon strength function, comparison to the photon strength function extracted from other experimental methods, such as photoneutron data and Oslo-method data, and with quasiparticle random phase approximation (QRPA) calculations based on the D1M Gogny force.
doi: 10.1103/PhysRevC.95.054317
2016DE20 Phys.Rev. C 94, 024342 (2016) Nuclear response functions with finite-range Gogny force: Tensor terms and instabilities
doi: 10.1103/PhysRevC.94.024342
2016GO28 Phys.Rev. C 94, 044306 (2016) S.Goriely, S.Hilaire, S.Peru, M.Martini, I.Deloncle, F.Lechaftois Gogny-Hartree-Fock-Bogolyubov plus quasiparticle random-phase approximation predictions of the M1 strength function and its impact on radiative neutron capture cross section NUCLEAR STRUCTURE 58,62,66,70,74,78,80,82,84Ni, 120,124,128,132,136,140,144,148,152,156,160Sn, 92Zr, 106Pd, 198Au, 208Pb, 232Th, 238U, 240Pu; N=6-150, 412 even-even nuclei; calculated B(M1) strengths, centroid M1 energies, integrated B(M1) strengths, M1 photoabsorption σ for 128,134Xe, B(E1) strengths for 232Th and 238U. A=20-250; calculated Γγ for E1 and M1 contributions. Large-scale calculations in the framework of axially-symmetric-deformed quasiparticle random phase approximation (QRPA) based on finite-range D1M Gogny force. Comparison with available experimental data. Analyzed impact on radiative neutron capture cross sections.
doi: 10.1103/PhysRevC.94.044306
2016MA43 Phys.Rev. C 94, 014304 (2016) M.Martini, S.Peru, S.Hilaire, S.Goriely, F.Lechaftois Large-scale deformed quasiparticle random-phase approximation calculations of the γ-ray strength function using the Gogny force NUCLEAR STRUCTURE 34S, 70,76Ge, 92Zr, 120Sn, 152Sm, 158Gd, 196Pt, 208Pb, 238U, 240Pu; A=10-250; calculated E1 γ-strength functions, B(E1) distributions in the GDR region. 115,120,125,130,135,140,145,150,155Sn; calculated and comparison E1 strength functions for Sn isotopes obtained with the three prescriptions used to correct the HFB+QRPA model based on D1M force. Self-consistent Hartree-Fock-Bogoliubov (HFB) plus axially symmetric deformed quasiparticle random-phase approximation (QRPA) calculations based on finite-range Gogny interactions D1S and D1M. Comparison with experimental photoabsorption data. Discussed predictions of γ-ray strength functions and Maxwellian-averaged neutron capture rates for Sn isotopes. NUCLEAR REACTIONS 28Si, 60Ni, 70,74Ge, 76,80Se, 90,94Zr, 90,98Mo, 116,119,120Sn, 124,128Te, 138Ba, 142Ce, 144,148Nd, 144,150,154Sm, 158Gd, 174Yb, 181Ta, 190Os, 206Pb, 232Th, 236,238U, 239Pu(γ, X), E*=5-30 MeV; calculated σ and compared with experimental data near the GDR. Self-consistent Hartree-Fock-Bogoliubov (HFB) plus axially symmetric deformed quasiparticle random-phase approximation (QRPA) calculations based on finite-range Gogny interactions D1S and D1M.
doi: 10.1103/PhysRevC.94.014304
2016MA45 Phys.Rev. C 94, 015501 (2016) M.Martini, N.Jachowicz, M.Ericson, V.Pandey, T.Van Cuyck, N.Van Dessel Electron-neutrino scattering off nuclei from two different theoretical perspectives NUCLEAR REACTIONS 12C(ν, X), E=150-750 MeV electron and muon neutrinos; calculated charged-current (CC) double differential cross section, momentum transfer versus the transferred energy, Coulomb-longitudinal and transverse contributions to cross sections, ratio of νe over νμ differential cross sections. Continuum random phase approximation (CRPA), and RPA-based calculations. Comparison with experimental data from T2K collaboration.
doi: 10.1103/PhysRevC.94.015501
2016PA43 Phys.Rev. C 94, 054609 (2016) V.Pandey, N.Jachowicz, M.Martini, R.Gonzalez-Jimenez, J.Ryckebusch, T.Van Cuyck, N.Van Dessel Impact of low-energy nuclear excitations on neutrino-nucleus scattering at MiniBooNE and T2K kinematics NUCLEAR REACTIONS 12C(ν, μ-), (ν-bar, μ+), E<2.5 GeV; calculated double-differential cross sections and total cross sections. Mean-field approach and solving Hartree-Fock (HF) equations using a Skyrme (SkE2) nucleon-nucleon interaction, and continuum random-phase approximation (CRPA). Comparison with MiniBooNE and T2K measurements. Relevance to accelerator-based neutrino-oscillation experiments.
doi: 10.1103/PhysRevC.94.054609
2016VA08 Phys.Rev. C 94, 024611 (2016) T.Van Cuyck, N.Jachowicz, R.Gonzalez-Jimenez, M.Martini, V.Pandey, J.Ryckebusch, N.Van Dessel Influence of short-range correlations in neutrino-nucleus scattering NUCLEAR REACTIONS 12C(ν, μ-), (ν, μ-), E=750 MeV; calculated cross section for incident muon neutrino, 1N and 2N knockout cross sections, 2p2h short-range correlation (SRC) response functions with contributions of the initial pn and nn pairs. Comparison with theoretical calculations for 12C(e, e'), and (e, e') experimental data.
doi: 10.1103/PhysRevC.94.024611
2016VE06 Phys.Rev. C 94, 044325 (2016) M.Versteegen, D.Denis-Petit, V.Meot, T.Bonnet, M.Comet, F.Gobet, F.Hannachi, M.Tarisien, P.Morel, M.Martini, S.Peru Low-energy modification of the γ strength function of the odd-even nucleus 115In NUCLEAR REACTIONS In, Cu, Au(γ, γ'), (γ, n), E=4.5-18 MeV bremsstrahlung beam from ELSA facility; measured Eγ, Iγ from the decay of 115mIn, 112In, 112mIn, 112Cd, 113mIn, 114In, 114mIn, 62Cu, 196Au radioisotopes formed by (γ, γ'), and (n, n') and (n, γ) reactions from photoneutrons produced in the main reaction; deduced yields of (γ, n) reactions, energy distributions of photoneutrons produced in (γ, n) reactions in natural In sample. 115mIn; deduced yield, σ(E) in (γ, γ') and compared to theoretical calculations using TALYS code with generalized Lorentzian (GLO) for E1 and standard Lorentzian form (SLO) of the Brink-Axel hypothesis for M1 photon strength functions (PSFs). QRPA calculations using the Gogny D1S force. Comparison with previous experimental results.
doi: 10.1103/PhysRevC.94.044325
2015CO03 Phys.Lett. B 743, 451 (2015) A.Corsi, S.Boissinot, A.Obertelli, P.Doornenbal, M.Dupuis, F.Lechaftois, M.Matsushita, S.Peru, S.Takeuchi, H.Wang, N.Aoi, H.Baba, P.Bednarczyk, M.Ciemala, A.Gillibert, T.Isobe, A.Jungclaus, V.Lapoux, J.Lee, M.Martini, K.Matsui, T.Motobayashi, D.Nishimura, S.Ota, E.Pollacco, H.Sakurai, C.Santamaria, Y.Shiga, D.Sohler, D.Steppenbeck, R.Taniuchi Neutron-driven collectivity in light tin isotopes: Proton inelastic scattering from 104Sn NUCLEAR REACTIONS 1H(104Sn, 104Sn'), E=150 MeV/nucleon; measured reaction products, Eγ, Iγ. 104Sn; deduced σ(θ), energy levels, J, π. QRPA with the D1M Gogny interaction calculations.
doi: 10.1016/j.physletb.2015.03.018
2015ER01 Phys.Rev. C 91, 035501 (2015) Neutrino versus antineutrino cross sections and CP violation
doi: 10.1103/PhysRevC.91.035501
2015NY01 Phys.Rev. C 91, 015808 (2015) H.-T.Nyhus, T.Renstrom, H.Utsunomiya, S.Goriely, D.M.Filipescu, I.Gheorghe, O.Tesileanu, T.Glodariu, T.Shima, K.Takahisa, S.Miyamoto, Y.-W.Lui, S.Hilaire, S.Peru, M.Martini, L.Siess, A.J.Koning Photoneutron cross sections for neodymium isotopes: Toward a unified understanding of (γ, n) and (n, γ) reactions in the rare earth region NUCLEAR REACTIONS 143,144,145,146,148Nd(γ, n), E=7.55-13.00 MeV laser Compton scattered (LCS) rays; measured neutron spectra, σ(E) at GACKO (Gamma Collaboration Hutch of Konan University) using SUBARU synchrotron radiation facility; deduced σ(E) for 147Nd(n, γ) by combining present (γ, n) data with existing (n, γ) data for 142,143,144,145,146,148Nd(n, γ), and using γ-SF method. Comparison of σ(E) for 147Nd(n, γ) with JENDL-4.0, ENDF/B-VII.1, and ROSFOND-2010 evaluated libraries. Comparison with predictions of Skyrme-Fock-Bogoliubov (HFB) plus quasiparticle random phase approximation (QRPA) model, and axially symmetric-deformed Gogny HFB plus QRPA model of E1 γ-ray strength using TALYS code. Comparison with previous experimental data.
doi: 10.1103/PhysRevC.91.015808
2015PA35 Phys.Rev. C 92, 024606 (2015) V.Pandey, N.Jachowicz, T.Van Cuyck, J.Ryckebusch, M.Martini Low-energy excitations and quasielastic contribution to electron-nucleus and neutrino-nucleus scattering in the continuum random-phase approximation NUCLEAR REACTIONS 12C(e, e'), E=120, 160, 200, 240, 440, 480, 560, 680, 730, 961, 1108, 1299, 1501, 1930, 2020, 2130, 2500, 3595 MeV; 16O(e, e'), E=700, 737, 880, 1080, 1200, 1500; 40Ca(e, e'), E=739, 841 MeV; calculated double-differential σ(E, θ), longitudinal and transverse responses for 12C(e, e'). Comparison with experimental data. 12C(ν, μ-), E=200, 300, 500, 800, 1500 MeV; calculated double differential cross sections as a function of outgoing muon kinetic energy and cos(θ), Coulomb-longitudinal and transverse contributions to double differential cross sections relevant to muon neutrino accelerator-based neutrino-oscillation experiments. Continuum random-phase approximation (CRPA) approach to quasielastic electron-nucleus and neutrino-nucleus scattering.
doi: 10.1103/PhysRevC.92.024606
2014FI17 Phys.Rev. C 90, 064616 (2014) D.M.Filipescu, I.Gheorghe, H.Utsunomiya, S.Goriely, T.Renstrom, H.-T.Nyhus, O.Tesileanu, T.Glodariu, T.Shima, K.Takahisa, S.Miyamoto, Y.-W.Lui, S.Hilaire, S.Peru, M.Martini, A.J.Koning Photoneutron cross sections for samarium isotopes: Toward a unified understanding of (γ, n) and (n, γ) reactions in the rare earth region NUCLEAR REACTIONS 144,147,148,149,150,152,154Sm(γ, n), E=6-17 MeV; measured E(n), I(n), monochromatic and nonmonochromatic σ(E). Comparison with previous experimental results, and predictions from Skyrme HFB+QRPA using BSk7 interaction, and axially deformed Gogny HFB+QRPA models using D1M interaction. 147,148,149,150,151,152Sm(n, γ), E=0.001-1 MeV; analyzed measured σ(E) with a TALYS calculation using D1M+QRPA calculation for the E1 strength function. 153Sm(n, γ), E=0.001-1 MeV; predicted σ(E) from TALYS calculations using γ-strength function (γSF) approach. Comparison with evaluated libraries JENDL-4.0, ENDF/B-VII.1, ROSFOND-2010.
doi: 10.1103/PhysRevC.90.064616
2014MA19 Phys.Rev. C 89, 044306 (2014) Gamow-Teller strength in deformed nuclei within the self-consistent charge-exchange quasiparticle random-phase approximation with the Gogny force NUCLEAR STRUCTURE 90Zr, 114Sn, 208Pb; calculated pnQRPA Fermi and Gamow-Teller (GT) strength distributions, GT widths for Sn isotopes. 76Ge; calculated pnQRPA GT strength distributions as function of deformation. Self-consistent axially symmetric-deformed proton-neutron quasiparticle random-phase approximation (pnQRPA) with the finite-range Gogny force. Analyzed role of deformation. Comparison with experimental data. RADIOACTIVITY 90,92,94,96,98,100,118Kr, 94,96,98,100,102,104,120Sr, 98,100,102,104,106,108,110,122Zr, 104,106,108,110,112,114,124Mo, 126Ru, 128Pd, 130Cd, 132Sn, 178Te, 180Xe, 182Ba, 184Ce, 186Nd, 188Sm, 190Gd, 192Dy, 194Er, 196Yb, 198Hf, 200W, 202Os, 262Pt, 264Hg, 266Pb, 268Po, 270Rn, 272Ra, 274Th, 276U, 278Pu, 280Cm, 282Cf, 284Fm, 286No(β-); calculated β-decay half-lives. Self-consistent axially symmetric-deformed proton-neutron quasiparticle random-phase approximation (pnQRPA) with the finite-range Gogny (D1M) force. Comparison with experimental data, and with previous theoretical calculations.
doi: 10.1103/PhysRevC.89.044306
2014MA38 Nucl.Data Sheets 118, 273 (2014) M.Martini, S.Hilaire, S.Goriely, A.J.Koning, S.Peru Improved Nuclear Inputs for Nuclear Model Codes Based on the Gogny Interaction NUCLEAR STRUCTURE 238U; calculated positive parity level density, temperature (and level density for T=0) below 100 MeV. NUCLEAR REACTIONS 174Yb, 180Hf, 238U(γ, x), E=5-25 MeV; calculated photoabsorption σ using QRPA with broadening. Sn(n, x), E≈90 keV; calculated Maxwell-averaged neutron capture rate for isotopes between 115 and 160 using GLO and QRPA.
doi: 10.1016/j.nds.2014.04.056
2014MA52 Nucl.Data Sheets 120, 133 (2014) Charge-exchange QRPA with the Gogny Force for Axially-symmetric Deformed Nuclei NUCLEAR STRUCTURE 90Zr, 114Sn, 208Pb, 76Ge; calculated isobaric analog and Gamow-Teller resonances, GT strength distributions. Quasiparticle random-phase approximation (QRPA) calculations using finite range Gogny force.
doi: 10.1016/j.nds.2014.07.027
2014MA67 Phys.Rev. C 90, 025501 (2014) Inclusive and pion production neutrino-nucleus cross sections NUCLEAR REACTIONS 12C(ν, ν'), E<1.2 GeV; analyzed experimental inclusive and pion production double-differential cross section data from T2K collaboration and MiniBooNE experiments on 12C and CH2 targets, using a model based on the nuclear response functions, where the quasielastic response is treated in the random phase approximation (RPA). Discussed need for inclusion of the two-pion channel.
doi: 10.1103/PhysRevC.90.025501
2014PA42 Phys.Rev. C 90, 025804 (2014) A.Pastore, M.Martini, D.Davesne, J.Navarro, S.Goriely, N.Chamel Linear response theory and neutrino mean free path using Brussels-Montreal Skyrme functionals
doi: 10.1103/PhysRevC.90.025804
2014PE08 Eur.Phys.J. A 50, 88 (2014) Mean field based calculations with the Gogny force: Some theoretical tools to explore the nuclear structure NUCLEAR STRUCTURE 32Mg, 44S; calculated potential energy surface, deformation, B(E2), rotational moment of inertia, proton and neutron pairing. 32Mg; calculated low-energy levels, J, π. 42Si, 44S, 46Ar, 48Ca, 50Ti, 52Cr; calculated neutron single-particle states, neutron pairing energy vs deformation, mass excess, B(E2). 24O, 26Ne, 28Mg, 30Si, 32S, 34Ar; calculated neutron single-particle states, neutron pairing energy vs deformation, mass excess, B(E2), B(E3). 58Ar, 60Ca, 62Ti, 64Cr, 66Fe, 68Ni, 70Zn, 72Ge, 74Se, 76Kr, 78Sr, 80Zr, 82Mo; calculated neutron pairing energy vs deformation. 78Ni, 100,132Sn, 208Pb; calculated isoscalar GMR, isovector GDR, isoscalar GQR average energy, fraction of EWSR, total, neutron, charge radii. 24O, 22,24,26,28Mg, 26,28,30Si; calculated monopole, quadrupole giant resonance responses vs energy. 238U; calculated monopole, dipole, quadrupole, octupole resonance responses. 174Yb, 180Hf, 238U; calculated photoabsorption σ vs energy. 56,58,60,62,64,66,68,70,72,74,76,78Ni, 100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136,138,140,142,144,146,148,150,152,154,156,158,160,162,164,166,168,170Sn; calculated HFB energy vs deformation, proton pairing energy vs deformation, B(E2). 5DCH (5-dimensional collective Hamiltonian) with account for triaxiality and vibrations, QRPA, HFB. Compared with available data.
doi: 10.1140/epja/i2014-14088-7
2014PE21 Phys.Scr. 89, 054030 (2014) Microscopic mean field approximation and beyond with the Gogny force NUCLEAR STRUCTURE 24,26,28Mg; calculated B(E0), B(E2) using QRPA. 24O, 26Ne, 28Mg, 30Si, 32S, 34Ar; calculated B(E2), first 2+ state energy using QRPA and using 5DCH (Five Dimension Collective Hamiltonian); compared with data.
doi: 10.1088/0031-8949/89/5/054030
2013MA49 Phys.Rev. C 87, 065501 (2013) Quasielastic and multinucleon excitations in antineutrino-nucleus interactions NUCLEAR REACTIONS 12C(ν-bar, X), E=0.2-2.0 GeV; analyzed quasielastic double differential σ(θ, E) for muonic antineutrino-nucleus collisions from MiniBooNE experiment using the random phase approximation (RPA).
doi: 10.1103/PhysRevC.87.065501
2013UT02 Phys.Rev. C 88, 015805 (2013) H.Utsunomiya, S.Goriely, T.Kondo, C.Iwamoto, H.Akimune, T.Yamagata, H.Toyokawa, H.Harada, F.Kitatani, Y.-W.Lui, A.C.Larsen, M.Guttormsen, P.E.Koehler, S.Hilaire, S.Peru, M.Martini, A.J.Koning Photoneutron cross sections for Mo isotopes: A step toward a unified understanding of (γ, n) and (n, γ) reactions NUCLEAR REACTIONS 94,95,96,97,98,100Mo(γ, n), E=7.55-13.00 MeV laser Compton scattered (LCS) γ rays; measured neutron spectra, σ(E). Comparison with previous experimental measurements, and with predictions of Skyrme Hartree-Fock-Bogoliubov (HFB) plus quasiparticle random phase approximation (QRPA) model, and axially symmetric-deformed Gogny HFB plus QRPA model of E1 γ-ray strength. 94,95,96,97(n, γ); analyzed σ(E) data by combining data from (γ, n), (γ, γ'), (3He, αγ) and (3He, 3He'γ) experiments. 93,99Mo(n, γ); predicted TALYS σ using (γ, γ') and (3He, 3He'γ) data. Comparison with JENDL-4.0, ENDF/B-VII.1, and ROSFOND-2010 evaluated reaction data files.
doi: 10.1103/PhysRevC.88.015805
2012DI03 Phys.Rev. C 85, 031301 (2012) A.Dijon, E.Clement, G.de France, G.de Angelis, G.Duchene, J.Dudouet, S.Franchoo, A.Gadea, A.Gottardo, T.Huyuk, B.Jacquot, A.Kusoglu, D.Lebhertz, G.Lehaut, M.Martini, D.R.Napoli, F.Nowacki, S.Peru, A.Poves, F.Recchia, N.Redon, E.Sahin, C.Schmitt, M.Sferrazza, K.Sieja, O.Stezowski, J.J.Valiente-Dobon, A.Vancraeyenest, Y.Zheng Discovery of a new isomeric state in 68Ni: Evidence for a highly deformed proton intruder state NUCLEAR REACTIONS 70Zn(238U, X)67Ni/68Ni/69Ni/69Cu, E=6.33 MeV/nucleon; measured energy loss, particle spectra, time of flight, Eγ, Iγ, (68Ni)γ-coin, delayed γ, half-life; deduced mass spectra. 68Ni; deduced levels, J, π, isomer, configurations, proton intruder state. 69Cu; deduced isomer half-life. VAMOS spectrometer and EXOGAM array at GANIL facility. Comparison with large-scale shell-model (LSSM) calculations.
doi: 10.1103/PhysRevC.85.031301
2012PA11 Phys.Rev. C 85, 054317 (2012) A.Pastore, D.Davesne, Y.Lallouet, M.Martini, K.Bennaceur, J.Meyer Nuclear response for the Skyrme effective interaction with zero-range tensor terms. II. Sum rules and instabilities
doi: 10.1103/PhysRevC.85.054317
2012PA32 Phys.Rev. C 86, 044308 (2012) A.Pastore, M.Martini, V.Buridon, D.Davesne, K.Bennaceur, J.Meyer Nuclear response for the Skyrme effective interaction with zero-range tensor terms. III. Neutron matter and neutrino propagation
doi: 10.1103/PhysRevC.86.044308
2011MA18 Phys.Rev. C 83, 034309 (2011) Low-energy dipole excitations in neon isotopes and N = 16 isotones within the quasiparticle random-phase approximation and the Gogny force NUCLEAR STRUCTURE 24O, 18,20,22,24,26,28,30Ne, 28Mg, 30Si; calculated B(E1) distributions, neutron and proton ground state density profiles, particle-hole configurations and energies for low-energy dipole excitation (GDR), neutron and proton transition densities. Fully consistent axially-symmetric-deformed quasiparticle random phase approximation (QRPA) approach based on Hartree-Fock-Bogolyubov (HFB) states.
doi: 10.1103/PhysRevC.83.034309
2011MA68 Phys.Rev. C 84, 055502 (2011) M.Martini, M.Ericson, G.Chanfray Neutrino quasielastic interaction and nuclear dynamics NUCLEAR REACTIONS 12C(ν, ν), E=0.2-2 GeV; analyzed quasielastic double differential σ(θ) data from MiniBooNE experiment; compared with RPA calculations.
doi: 10.1103/PhysRevC.84.055502
2011PE01 Phys.Rev. C 83, 014314 (2011) S.Peru, G.Gosselin, M.Martini, M.Dupuis, S.Hilaire, J.-C.Devaux Giant resonances in 238U within the quasiparticle random-phase approximation with the Gogny force NUCLEAR STRUCTURE 238U; calculated Kπ=0-, 0+, 1-, 1+ eigenvalues, B(E0), B(E1), B(E2) and B(E3) strengths for dipole, monopole, quadrupole, and octupole giant resonances and low-energy states. Fully consistent microscopic axially-symmetric deformed quasiparticle random-phase approximation (QRPA) approach using a finite-range Gogny force for Hartree-Fock-Bogolyubov mean field and QRPA matrix. Comparison with experimental data.
doi: 10.1103/PhysRevC.83.014314
2010MA19 Phys.Rev. C 81, 045502 (2010) M.Martini, M.Ericson, G.Chanfray, J.Marteau Neutrino and antineutrino quasielastic interactions with nuclei NUCLEAR REACTIONS 12C(ν, X), (ν-bar, X), E=0.05-1.2 GeV; calculated quasielastic σ and differential σ versus energy transfer using framework of the nuclear response functions treated in the random phase approximation (RPA). Comparison with experimental data.
doi: 10.1103/PhysRevC.81.045502
2009DA15 Phys.Rev. C 80, 024314 (2009); Erratum Phys.Rev. C 84, 059904 (2011) D.Davesne, M.Martini, K.Bennaceur, J.Meyer Nuclear response for the Skyrme effective interaction with zero-range tensor terms
doi: 10.1103/PhysRevC.80.024314
2009MA69 Phys.Rev. C 80, 065501 (2009) M.Martini, M.Ericson, G.Chanfray, J.Marteau Unified approach for nucleon knock-out and coherent and incoherent pion production in neutrino interactions with nuclei NUCLEAR REACTIONS 12C(ν, π), E<1.5 GeV; calculated σ and differential σ using theory of nuclear response in random phase approximation. Comparison with experimental data.
doi: 10.1103/PhysRevC.80.065501
2008MA48 Nucl.Phys. A813, 212 (2008) M.Martini, V.De Donno, C.Maieron, G.Co A particle-hole model approach for hypernuclei NUCLEAR STRUCTURE 12C, 16O, 40Ca, 90Zr, 208Pb; calculated levels, J, π, B(E1), B(M1), configurations of hypernuclei using a particle-hole model. Comparison with a mean field model and experimental data.
doi: 10.1016/j.nuclphysa.2008.09.002
2007MA18 Phys.Rev. C 75, 034604 (2007) M.Martini, G.Co, M.Anguiano, A.M.Lallena Superscaling in electroweak excitation of nuclei NUCLEAR REACTIONS 12C, 16O, 40Ca(e, e'), E ≈ 700-1200 MeV; 16O(ν, e), E=300 MeV; calculated σ(E, θ). 16O(ν, e), E=20-300 MeV; calculated total σ. Modified relativistic Fermi gas scaling functions.
doi: 10.1103/PhysRevC.75.034604
2006CH15 Eur.Phys.J. A 27, 191 (2006) G.Chanfray, D.Davesne, M.Ericson, M.Martini Two-pion production processes, chiral symmetry and NN interaction in the medium
doi: 10.1140/epja/i2005-10245-5
2002OK03 Prog.Nucl.Energy 41, 285 (2002) S.Okajima, T.Sakurai, J.F.Lebrat, V.Z.Averlant, M.Martini Summary on International Benchmark Experiments for Effective Delayed Neutron Fraction (βeff)
doi: 10.1016/S0149-1970(02)00015-X
1999AM07 Phys.Rev. D60, 032002 (1999) M.Ambrogiani, S.Bagnasco, W.Baldini, D.Bettoni, G.Borreani, A.Buzzo, R.Calabrese, R.Cester, P.Dalpiaz, X.Fan, G.Garzoglio, K.E.Gollwitzer, A.Hahn, S.Jin, J.Kasper, G.Lasio, M.Lo Vetere, E.Luppi, P.Maas, M.Macri, M.Mandelkern, F.Marchetto, M.Marinelli, W.Marsh, M.Martini, E.Menichetti, R.Mussa, M.M.Obertino, M.Pallavicini, N.Pastrone, C.Patrignani, T.K.Pedlar, J.Peoples, Jr., S.Pordes, E.Robutti, J.Rosen, P.Rumerio, A.Santroni, M.Savrie, J.Schultz, K.K.Seth, G.Stancari, M.Stancari, J.Streets, A.Tomaradze, S.Werkema, G.Zioulas Measurements of the Magnetic Form of the Proton in the Timelike Region at Large Momentum Transfer NUCLEAR REACTIONS 1H(p-bar, ee+), E(cm)=2.9-4.3 GeV; measured σ, invariant mass spectra. 1H deduced magnetic form factor. Non-magnetic spectrometer.
doi: 10.1103/PhysRevD.60.032002
1992AR27 Yad.Fiz. 55, 1568 (1992); Sov.J.Nucl.Phys. 55, 865 (1992) T.Armstrong, D.Bettoni, V.Bharadwaj, C.Biino, G.Borreani, D.Broemmelsiek, A.Buzzo, R.Galabrese, A.Ceccucci, R.Cester, M.Church, P.Dalpiaz, P.F.Dalpiaz, R.Dibenedetto, D.Dimitroyannis, M.Fabbri, J.Fast, E.Ferroni, A.Gianoli, C.M.Ginsburg, K.Gollwitzer, A.Hahn, M.Hasan, S.Hsueh, R.Lewis, E.Luppi, M.Macri, A.M.Majewska, M.Mandelkern, F.Marchetto, M.Marinelli, J.Marques, W.Marsh, M.Martini, M.Masuzawa, E.Minechetti, A.Migliori, R.Mussa, S.Palestini, N.Pastrone, C.Patrignani, J.Peoples, Jr., L.Pesando, R.Petrucci, M.G.Pia, S.Pordes, P.Rapidis, R.Ray, J.Reid, G.Rinaudo, B.Roccuzzo, J.Rosen, A.Santroni, M.Sarmineto, M.Savrie, A.Scalisi, J.Schultz, K.Seth, A.Smith, G.A.Smith, M.Sozzi, S.Trokenheim, M.F.Weber, S.Werkema, Y.Zhang, J.Zhao, G.Zioulas A New Measurement of the Proton Electromagnetic Form Factor in the Time-Like Region at High Energy NUCLEAR REACTIONS 1H(p-bar, e-e+), E not given; measured (e+e-) opening angle σ(θ). 1H deduced electromagnetic form factor.
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