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NSR database version of April 11, 2024.

Search: Author = J.Atkinson

Found 13 matches.

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2022KA35      Phys.Rev.Lett. 129, 142502 (2022)

S.Kaur, R.Kanungo, W.Horiuchi, G.Hagen, J.D.Holt, B.S.Hu, T.Miyagi, T.Suzuki, F.Ameil, J.Atkinson, Y.Ayyad, S.Bagchi, D.Cortina-Gil, I.Dillmann, A.Estrade, A.Evdokimov, F.Farinon, H.Geissel, G.Guastalla, R.Janik, R.Knobel, J.Kurcewicz, Y.A.Litvinov, M.Marta, M.Mostazo, I.Mukha, C.Nociforo, H.J.Ong, T.Otsuka, S.Pietri, A.Prochazka, C.Scheidenberger, B.Sitar, P.Strmen, M.Takechi, J.Tanaka, I.Tanihata, S.Terashima, J.Vargas, H.Weick, J.S.Winfield

Proton Distribution Radii of 16-24O: Signatures of New Shell Closures and Neutron Skin

NUCLEAR REACTIONS 12C(16O, X), (18O, X), (19O, X), (20O, X), (21O, X), (22O, X), (23O, X), (24O, X), E<1 GeV/nucleon; measured reaction products. 16,18,20,21,22,23,24O; deduced charge changing σ, root mean square proton and matter radii, neutron skin thickness, shell closure. Comparison with with ab initio calculations employing the chiral NNLO sat interaction, shell model predictions. The fragment separator FRS at GSI.

doi: 10.1103/PhysRevLett.129.142502
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD8052. Data from this article have been entered in the XUNDL database. For more information, click here.

2022RO11      Phys.Rev. C 106, 014618 (2022)

J.L.Rodriguez-Sanchez, J.Benlliure, I.Vidana, H.Lenske, J.Vargas, C.Scheidenberger, H.Alvarez-Pol, J.Atkinson, T.Aumann, Y.Ayyad, S.Beceiro Novo, K.Boretzky, M.Caamano, E.Casarejos, D.Cortina-Gil, P.Diaz Fernandez, A.Estrade, H.Geissel, E.Haettner, A.Kelic-Heil, Yu.A.Litvinov, C.Paradela, D.Perez-Loureiro, S.Pietri, A.Prochazka, M.Takechi, Y.K.Tanaka, H.Weick, J.S.Winfield

Systematic study of Δ(1232) resonance excitations using single isobaric charge-exchange reactions induced by medium-mass projectiles of Sn

NUCLEAR REACTIONS 1H, 12C, Cu, Pb(112Sn, 112In), (112Sn, 112Sb), 1H, C(124Sn, 124Sb), E=1 GeV/nucleon; measured reaction products; deduced total σ, quasielastic and inelastic σ; missing energy spectra. Observed energy shift for the Δ-resonance peak of about 63 ± 5 MeV and quenching of the quasielastic component. Comparison to theoretical predictions using random phase approximation (RPA) with Giessen energy density functional (GiEDF). FRS spectrometer with SIS-18 synchrotron beam (GSI).

doi: 10.1103/PhysRevC.106.014618
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2020RO12      Phys.Lett. B 807, 135565 (2020)

J.L.Rodriguez-Sanchez, J.Benlliure, I.Vidana, H.Lenske, C.Scheidenberger, J.Vargas, H.Alvarez-Pol, J.Atkinson, T.Aumann, Y.Ayyad, S.Beceiro Novo, K.Boretzky, M.Caamano, E.Casarejos, D.Cortina-Gil, P.Diaz Fernandez, A.Estrade, H.Geissel, E.Haettner, A.Kelic-Heil, Yu.A.Litvinov, C.Paradela, D.Perez-Loureiro, S.Pietri, A.Prochazka, M.Takechi, Y.K.Tanaka, H.Weick, J.S.Winfield

Study of Δ excitations in medium-mass nuclei with peripheral heavy ion charge-exchange reactions

NUCLEAR REACTIONS C(112Sn, 112In), E=1 GeV/nucleon; analyzed available data; deduced missing spectra, change in the relative magnitude between the contribution of the excitation of the resonance in the target and in the projectile.

doi: 10.1016/j.physletb.2020.135565
Citations: PlumX Metrics

2019BA11      Phys.Lett. B 790, 251 (2019)

S.Bagchi, R.Kanungo, W.Horiuchi, G.Hagen, T.D.Morris, S.R.Stroberg, T.Suzuki, F.Ameil, J.Atkinson, Y.Ayyad, D.Cortina-Gil, I.Dillmann, A.Estrade, A.Evdokimov, F.Farinon, H.Geissel, G.Guastalla, R.Janik, S.Kaur, R.Knobel, J.Kurcewicz, Yu.A.Litvinov, M.Marta, M.Mostazo, I.Mukha, C.Nociforo, H.J.Ong, S.Pietri, A.Prochazka, C.Scheidenberger, B.Sitar, P.Strmen, M.Takechi, J.Tanaka, Y.Tanaka, I.Tanihata, S.Terashima, J.Vargas, H.Weick, J.S.Winfield

Neutron skin and signature of the N = 14 shell gap found from measured proton radii of 17-22N

NUCLEAR REACTIONS C(14N, X), (15N, X), (17N, X), (18N, X), (19N, X), (20N, X), (21N, X), (22N, X), E=851-932 MeV/nucleon; measured reaction products. 14,15,17,18,19,20,21,22N; deduced σ, root mean square point proton and matter radii, unconventional shell gap at N = 14 arising from the attractive proton–neutron tensor interaction. Comparison with ab initio calculations.

doi: 10.1016/j.physletb.2019.01.024
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0941.

2017RO22      Phys.Rev. C 96, 034303 (2017)

J.L.Rodriguez-Sanchez, J.Benlliure, C.A.Bertulani, J.Vargas, Y.Ayyad, H.Alvarez-Pol, J.Atkinson, T.Aumann, S.Beceiro Novo, K.Boretzky, M.Caamano, E.Casarejos, D.Cortina-Gil, J.Diaz-Cortes, P.Diaz Fernandez, A.Estrade, H.Geissel, A.Kelic-Heil, Yu.A.Litvinov, M.Mostazo, C.Paradela, D.Perez-Loureiro, S.Pietri, A.Prochazka, M.Takechi, H.Weick, J.S.Winfield

Knockout and fragmentation reactions using a broad range of tin isotopes

NUCLEAR REACTIONS C(112Sn, X)103Rh/104Rh/105Rh/106Rh/107Rh/105Pd/106Pd/107Pd/108Pd/107Ag/108Ag/109Ag/110Ag/109Cd/110Cd/111Cd, E=1 GeV/nucleon; measured production cross sections of the most neutron-rich residues in the fragmentation of 112Sn beam at GSI. C(124Sn, 123Sn), (124Sn, 123In), (120Sn, 119Sn), (120Sn, 119In), (120Sn, 118Cd), (112Sn, 111Sn), (112Sn, 111In), (110Sn, 109Sn), (110Sn, 109In), (110Sn, 108Cd), E=1 GeV/nucleon; measured One- and two-nucleon-removal cross sections. Comparison with previous experimental data and with Glauber model calculations.

doi: 10.1103/PhysRevC.96.034303
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2016KA37      Phys.Rev.Lett. 117, 102501 (2016)

R.Kanungo, W.Horiuchi, G.Hagen, G.R.Jansen, P.Navratil, F.Ameil, J.Atkinson, Y.Ayyad, D.Cortina-Gil, I.Dillmann, A.Estrade, A.Evdokimov, F.Farinon, H.Geissel, G.Guastalla, R.Janik, M.Kimura, R.Knobel, J.Kurcewicz, Yu.A.Litvinov, M.Marta, M.Mostazo, I.Mukha, C.Nociforo, H.J.Ong, S.Pietri, A.Prochazka, C.Scheidenberger, B.Sitar, P.Strmen, Y.Suzuki, M.Takechi, J.Tanaka, I.Tanihata, S.Terashima, J.Vargas, H.Weick, J.S.Winfield

Proton Distribution Radii of 12-19C Illuminate Features of Neutron Halos

NUCLEAR REACTIONS Be(20Ne, X), (40Ar, X)12C/13C/14C/15/16C/17C/18C/19C, E=1 GeV/nucleon; measured reaction products; deduced σ, root-mean-square proton and matter radii, neutron skin thickness. Comparison with ab initio calculations.

doi: 10.1103/PhysRevLett.117.102501
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2311. Data from this article have been entered in the XUNDL database. For more information, click here.

2016SU16      Phys.Rev. C 94, 011602 (2016)

Y.Suzuki, W.Horiuchi, S.Terashima, R.Kanungo, F.Ameil, J.Atkinson, Y.Ayyad, D.Cortina-Gil, I.Dillmann, A.Estrade, A.Evdokimov, F.Farinon, H.Geissel, G.Guastalla, R.Janik, R.Knoebel, J.Kurcewicz, Yu.A.Litvinov, M.Marta, M.Mostazo, I.Mukha, C.Nociforo, H.J.Ong, S.Pietri, A.Prochazka, C.Scheidenberger, B.Sitar, P.Strmen, M.Takechi, J.Tanaka, I.Tanihata, J.Vargas, H.Weick, J.S.Winfield

Parameter-free calculation of charge-changing cross sections at high energy

NUCLEAR REACTIONS 12C(12C, X), E=937, 943 MeV/nucleon; 12C(13C, X), E=828 MeV/nucleon; 12C(14C, X), E=900 MeV/nucleon; 1H(12C, X), E=926 MeV/nucleon; 1H(13C, X), E=815 MeV/nucleon; 1H(14C, X), E=889 MeV/nucleon; 1H(15C, X), E=896 MeV/nucleon; 1H(16C, X), E=897 MeV/nucleon; 1H(17C, X), E=970 MeV/nucleon; 1H(18C, X), (19C, X), E=886 MeV/nucleon; calculated charge-changing σ (CCCS), proton, neutron, and matter radii using Glauber and eikonal formalism and approximations. Comparison with recent new high-energy data measured at the FRS-GSI facility.

doi: 10.1103/PhysRevC.94.011602
Citations: PlumX Metrics

2016TA07      Prog.Theor.Exp.Phys. 2016, 043D05 (2016)

I.Tanihata, S.Terashima, R.Kanungo, F.Ameil, J.Atkinson, Y.Ayyad, D.Cortina-Gil, I.Dillmann, A.Estrade, A.Evdokimov, F.Farinon, H.Geissel, G.Guastalla, R.Janik, R.Knoebel, J.Kurcewicz, Yu.A.Litvinov, M.Marta, M.Mostazo, I.Mukha, C.Nociforo, H.J.Ong, S.Pietri, A.Prochazka, C.Scheidenberger, B.Sitar, P.Strmen, M.Takechi, J.Tanaka, H.Toki, J.Vargas, J.S.Winfield, H.Weick

Observation of large enhancements of charge exchange cross sections with neutron-rich carbon isotopes

NUCLEAR REACTIONS C, H(C, X)12N/13N/14N/15N/16N/17N/18N/19N, E∼950 MeV/nucleon; measured reaction products; deduced σ, Gamow-Teller and/or Fermi transition strengths.

doi: 10.1093/ptep/ptw034
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2358.

2014ES07      Phys.Rev.Lett. 113, 132501 (2014)

A.Estrade, R.Kanungo, W.Horiuchi, F.Ameil, J.Atkinson, Y.Ayyad, D.Cortina-Gil, I.Dillmann, A.Evdokimov, F.Farinon, H.Geissel, G.Guastalla, R.Janik, M.Kimura, R.Knobel, J.Kurcewicz, Yu.A.Litvinov, M.Marta, M.Mostazo, I.Mukha, C.Nociforo, H.J.Ong, S.Pietri, A.Prochazka, C.Scheidenberger, B.Sitar, P.Strmen, Y.Suzuki, M.Takechi, J.Tanaka, I.Tanihata, S.Terashima, J.Vargas, H.Weick, J.S.Winfield

Proton Radii of 12-17B Define a Thick Neutron Surface in 17B

NUCLEAR REACTIONS C(10B, X), (11B, X), (12B, X), (13B, X), (14B, X), (15B, X), (16B, X), (17B, X), E ∼ 900 MeV/nucleon; measured reaction products. 10,11,12,13,14,15,16,17B; deduced charge-changing σ, proton and matter radii, neutron skin. Glauber model analysis.

doi: 10.1103/PhysRevLett.113.132501
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0749. Data from this article have been entered in the XUNDL database. For more information, click here.

2014TE06      Prog.Theor.Exp.Phys. 2014, 101D02 (2014)

S.Terashima, I.Tanihata, R.Kanungo, A.Estrade, W.Horiuchi, F.Ameil, J.Atkinson, Y.Ayyad, D.Cortina-Gil, I.Dillmann, A.Evdokimov, F.Farinon, H.Geissel, G.Guastalla, R.Janik, M.Kimura, R.Knoebel, J.Kurcewicz, Yu.A.Litvinov, M.Marta, M.Mostazo, I.Mukha, T.Neff, C.Nociforo, H.J.Ong, S.Pietri, A.Prochazka, C.Scheidenberger, B.Sitar, Y.Suzuki, M.Takechi, J.Tanaka, J.Vargas, J.S.Winfield, H.Weick

Proton radius of 14Be from measurement of charge-changing cross sections

NUCLEAR REACTIONS C(7Be, np), (9Be, np), (10Be, np), (11Be, np), (12Be, np), (14Be, np), E=90 MeV/nucleon; measured reaction products; deduced σ, proton and nucleon rms radii. Comparison with Glauber model calculations.

doi: 10.1093/ptep/ptu134
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2350.

1968AT03      Nucl.Phys. A114, 143 (1968)

J.Atkinson, L.G.Mann, K.G.Tirsell, S.D.Bloom

Coulomb Matrix Elements from β-γ (CP) Correlation Measurements in 57Ni and 65Ni

RADIOACTIVITY 57,65Ni[from 54Fe(α, n), 64Ni(n, γ)]; measured βγ-CP (circular-polarization correlation); deduced Coulomb matrix elements. Enriched targets.

doi: 10.1016/0375-9474(68)90821-X
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1961AT02      Phys.Rev. 123, 1850 (1961)

J.H.Atkinson, W.N.Hess, V.Perez-Mendez, R.Wallace

5-Bev Neutron Cross Sections In Hydrogen And Other Elements

NUCLEAR REACTIONS 1H(n, x), C(n, n), C(n, x), 27Al(n, n), 27Al(n, x), Cu(n, n), Cu(n, x), Sn(n, x), Pb(n, n), Pb(n, x), E=5 GeV; measured products, C, Pb, 27Al, Cu; deduced σ, σ(E). Data were imported from EXFOR entry 11112.

doi: 10.1103/PhysRev.123.1850
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset11112.

1956WR22      Proc.Phys.Soc.(London) 69A, 77 (1956)

I.F.Wright, D.R.O.Morrison, J.M.Reid, J.R.Atkinson

The Photodisintegration of Nitrogen

doi: 10.1088/0370-1298/69/2/301
Citations: PlumX Metrics

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Note: The following list of authors and aliases matches the search parameter J.Atkinson: , J.H.ATKINSON, J.R.ATKINSON