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NSR database version of May 20, 2024.

Search: Author = M.Martini

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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
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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
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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
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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
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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
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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
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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
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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
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2018KA06      J.Phys.(London) G45, 013001 (2018)

T.Katori, M.Martini

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
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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
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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
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2017DE27      Eur.Phys.J. A 53, 170 (2017)

I.Deloncle, S.Peru, M.Martini

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
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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
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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
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2016DE20      Phys.Rev. C 94, 024342 (2016)

A.De Pace, M.Martini

Nuclear response functions with finite-range Gogny force: Tensor terms and instabilities

doi: 10.1103/PhysRevC.94.024342
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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
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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
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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
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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
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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
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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
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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
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Data from this article have been entered in the XUNDL database. For more information, click here.


2015ER01      Phys.Rev. C 91, 035501 (2015)

M.Ericson, M.Martini

Neutrino versus antineutrino cross sections and CP violation

doi: 10.1103/PhysRevC.91.035501
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetK2478.


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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetK2472.


2014MA19      Phys.Rev. C 89, 044306 (2014)

M.Martini, S.Peru, S.Goriely

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
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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
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2014MA52      Nucl.Data Sheets 120, 133 (2014)

M.Martini, S.Goriely, S.Peru

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
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2014MA67      Phys.Rev. C 90, 025501 (2014)

M.Martini, M.Ericson

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
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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
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2014PE08      Eur.Phys.J. A 50, 88 (2014)

S.Peru, M.Martini

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
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2014PE21      Phys.Scr. 89, 054030 (2014)

S.Peru, M.Martini

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
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2013MA49      Phys.Rev. C 87, 065501 (2013)

M.Martini, M.Ericson

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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetK2433.


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
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Data from this article have been entered in the XUNDL database. For more information, click here.


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
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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
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2011MA18      Phys.Rev. C 83, 034309 (2011)

M.Martini, S.Peru, M.Dupuis

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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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