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NSR database version of April 11, 2024.

Search: Author = T.Thomas

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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
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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
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2017DU08      Nucl.Phys. A965, 13 (2017)

H.Duckwitz, P.Petkov, T.Thomas, T.Ahn, A.Blazhev, N.Cooper, C.Fransen, M.Hinton, G.Ilie, J.Jolie, V.Werner

Nuclear structure investigations of 84Sr and 86Sr using γ-ray spectroscopic methods

NUCLEAR REACTIONS 85Rb(p, 2n), E=15 MeV;87Rb(p, 2n), E=16 MeV; measured Eγ, Iγ(θ), γγ-coin using HORUS and YRAST spectrometer of 10 clover detectors. 84,86Sr deduced γ transitions, levels, J, π, branching and mixing ratio, T1/2 using DSA (Doppler Shift Attenuation) method; calculated levels, J, π transition strengths, B(E2), B(M1) using NuShellX@MSU shell model code with Honma residual interaction; deduced mixed symmetry states. Calculations compared with available data.

doi: 10.1016/j.nuclphysa.2017.05.077
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2016FU09      Phys.Rev. C 94, 034318 (2016)

B.Fu, M.Seidlitz, A.Blazhev, M.Bouhelal, F.Haas, P.Reiter, K.Arnswald, B.Birkenbach, C.Fransen, G.Friessner, A.Hennig, H.Hess, R.Hirsch, L.Lewandowski, D.Schneiders, B.Siebeck, T.Steinbach, T.Thomas, A.Vogt, A.Wendt, K.Wolf, K.O.Zell

γ-ray spectroscopy of 33P and 33S after fusion-evaporation reactions

NUCLEAR REACTIONS 26Mg(13C, npα), (13C, 2nα), E=46 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ) level half-lives by DSAM using HORUS array at Cologne tandem accelerator facility. 33P, 33S; deduced levels, J, π, γ-ray branching ratios, multipolarity and mixing ratios for selected γ rays in 33P. Comparison with truncated p-sd-pf shell model calculations using the PSDPF interaction.

doi: 10.1103/PhysRevC.94.034318
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2016MO34      Phys.Rev. C 94, 054323 (2016)

K.Moschner, A.Blazhev, J.Jolie, N.Warr, P.Boutachkov, P.Bednarczyk, K.Sieja, A.Algora, F.Ameil, M.A.Bentley, S.Brambilla, N.Braun, F.Camera, J.Cederkall, A.Corsi, M.Danchev, D.DiJulio, C.Fahlander, J.Gerl, A.Giaz, P.Golubev, M.Gorska, J.Grebosz, T.Habermann, M.Hackstein, R.Hoischen, I.Kojouharov, N.Kurz, N.Marginean, E.Merchan, T.Moller, F.Naqvi, B.S.Nara Singh, C.Nociforo, N.Pietralla, S.Pietri, Zs.Podolyak, A.Prochazka, M.Reese, P.Reiter, M.Rudigier, D.Rudolph, T.Sava, H.Schaffner, L.Scruton, J.Taprogge, T.Thomas, H.Weick, A.Wendt, O.Wieland, H.-J.Wollersheim

Relativistic Coulomb excitation of 88Kr

NUCLEAR REACTIONS 197Au(88Kr, 88Kr'), E=128 MeV/nucleon, [secondary 88Kr beam from 9Be(238U, F), E=650 MeV/nucleon, followed by separation of fragments using FRS separator at GSI]; measured scattered particles, Eγ, (particle)γ-coin using PreSPEC Ge-detector array of EUROBALL Cluster for γ detection and Lund-York-Cologne Calorimeter (LYCCA) for ion detection. 88Kr; deduced levels, B(E2) and B(M1) for second and third 2+ states, mixed-symmetric nature of the third 2+ state. Comparison with IBM-2 model calculations. Systematics of energies, B(E2) and B(M1) for the first and third 2+ states for 88Kr, 90Sr, 92Zr, 94Mo, 96Ru, 98Pd.

doi: 10.1103/PhysRevC.94.054323
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2016TH01      Nucl.Phys. A947, 203 (2016)

T.Thomas, V.Werner, J.Jolie, K.Nomura, T.Ahn, N.Cooper, H.Duckwitz, A.Fitzler, C.Fransen, A.Gade, M.Hinton, G.Ilie, K.Jessen, A.Linnemann, P.Petkov, N.Pietralla, D.Radeck

Nuclear structure of 96, 98Mo: Shape coexistence and mixed-symmetry states

NUCLEAR REACTIONS 96Zr(3He, 3n), E=18 MeV;96Zr(α, 2n), E=16 MeV;measured Eγ, Iγ(θ), γγ-coin using OSIRIS and YRAST Ball spectrometer; deduced γ angular correlations; deduced levels, J, π, branching and E2/M1 mixing ratios, B(M1), B(E2), lifetimes of discrete γ transitions using Doppler Shift Attenuation Method; calculated β, γ deformations using Skyrme energy density functional, IBM-2 configuration mixing; deduced parameters, one- and two-phonon mixed-symmetry states, shape coexistence.

doi: 10.1016/j.nuclphysa.2015.12.010
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2016UR03      Phys.Rev. C 94, 011302 (2016)

W.Urban, U.Koster, M.Jentschel, P.Mutti, B.Markisch, T.Rzaca-Urban, Ch.Bernards, Ch.Fransen, J.Jolie, T.Thomas, G.S.Simpson

Precise measurement of energies in 115Sn following the (n, γ) reaction

NUCLEAR REACTIONS 114Sn(n, γ), E=cold neutrons; measured primary and secondary Eγ, γγ-coin using eight large Ge detectors at PF1B facility of ILL-Grenoble. 115Sn; deduced levels, S(n).

RADIOACTIVITY 115In(β-); deduced precise Q(β-) for a highly-forbidden β- transition from 115In g.s. parent to a 497, 3/2+ level in 115Sn using precisely measured masses of relevant nuclides and precise energy measurement of the 497.3-keV level in 115Sn from (n, γ).

doi: 10.1103/PhysRevC.94.011302
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2016UR04      Phys.Rev. C 94, 044328 (2016)

W.Urban, K.Sieja, T.Materna, M.Czerwinski, T.Rzaca-Urban, A.Blanc, M.Jentschel, P.Mutti, U.Koster, T.Soldner, G.de France, G.S.Simpson, C.A.Ur, C.Bernards, C.Fransen, J.Jolie, J.-M.Regis, T.Thomas, N.Warr

Low-spin structure of 8635Br51 and 8636Kr50 nuclei: The role of the g7/2 neutron orbital

RADIOACTIVITY 86Se, 86Br(β-)[from 235U(n, γ), E=thermal neutrons from PF1B-ILL-Grenoble facility using Lohengrin fission-fragment separator]; measured Eγ, Iγ, γγ-coin for both decays, γγ(θ) and γγ(linear polarization) for 86Br decay using EXILL array of Ge detectors. 86Br, 86Kr; deduced levels, J, π, conversion coefficients, multipolarities, β feedings, logft. Comparison with large-scale shell-model calculations with refined interactions.

NUCLEAR REACTIONS 235U(n, γ), E=thermal neutrons from PF1B-ILL-Grenoble facility; measured Eγ, Iγ, γγ-coin using EXILL array of Ge detectors, level half-life by γγ(t). 86Br; deduced levels, J, π, B(M2), B(E3).

doi: 10.1103/PhysRevC.94.044328
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2015MA51      Phys.Rev. C 92, 034305 (2015)

T.Materna, W.Urban, K.Sieja, U.Koster, H.Faust, M.Czerwinski, T.Rzaca-Urban, C.Bernards, C.Fransen, J.Jolie, J.-M.Regis, T.Thomas, N.Warr

Low spin structure of 86Se: Confirmation of γ collectivity at N=52

RADIOACTIVITY 86As(β-)[from 235U(n, F), E=thermal followed by mass separation using Lohengrin separator at ILL-Grenoble]; measured Eγ, Iγ, Eβ, βγ-, γγ-coin, γγ(θ). 86Se; deduced levels, J, π, γ collectivity. Comparison with systematics of neighboring nuclides, and with shell-model calculations. 94,96Y, 99Zr; observed γ rays.

NUCLEAR STRUCTURE 86Se; calculated levels, J, π, B(M1), B(E2) using shell model. 84Ge, 86Se, 88Kr, 90Sr, 92Zr; calculated energies of second 2+ and 4+, and first 3+ states. Comparison with experimental values.

doi: 10.1103/PhysRevC.92.034305
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2015ST08      Phys.Rev. C 91, 054326 (2015)

R.Stegmann, C.Bauer, G.Rainovski, N.Pietralla, C.Stahl, S.Bonig, S.Ilieva, A.Blazhev, A.Damyanova, M.Danchev, K.Gladnishki, J.Jolie, R.Lutter, J.Pakarinen, D.Radeck, E.Rapisarda, P.Reiter, M.Scheck, B.Siebeck, T.Stora, P.Thole, T.Thomas, M.Thurauf, M.J.Vermeulen, D.Voulot, N.Warr, F.Wenander, V.Werner, H.De Witte

Evolution of quadrupole collectivity in N=80 isotones toward the Z=64 subshell gap: The B(E2; 2+1 → 0+1) value of 142Sm

NUCLEAR REACTIONS 48Ti, 94Mo(142Sm, 142Sm'), E=405 MeV, [secondary 142Sm beam from Ta(p, X), E=1.4 GeV from PS booster at CERN and using RILIS and GPS setup at ISOLDE-CERN]; measured Eγ, Iγ, (particle)γ-coin, γ-particle yields as function of angle using MINIBALL HPGe-detector array at REX-ISOLDE-CERN facility. Coulomb excitation technique. 142Sm; deduced matrix elements and B(E2) for the first 2+ state in 142Sm. Systematics of B(E2) values for first 2+ state in 130Sn, 132Te, 134Xe, 136Ba, 138Ce, 140Nd, 142Sm. Comparison with shell-model calculations.

RADIOACTIVITY 142Pm, 142,142mEu, 142Sm(EC), (β+); measured Iγ; deduced 142mEu/142Eu isomeric ratio, and M(142Eu)/M(142Sm).

doi: 10.1103/PhysRevC.91.054326
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2015VA11      Phys.Rev. C 92, 011301 (2015)

P.Van Isacker, J.Jolie, T.Thomas, A.Leviatan

Partial dynamical symmetry in Bose-Fermi systems

NUCLEAR STRUCTURE 195Pt; calculated levels, J, π, B(E2) by generalization of partial dynamical symmetry (PDS) concept to a system of interacting bosons and fermions. Comparison with experimental data.

doi: 10.1103/PhysRevC.92.011301
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2014GL02      Phys.Rev. C 89, 065808 (2014)

J.Glorius, K.Sonnabend, J.Gorres, D.Robertson, M.Knorzer, A.Kontos, T.Rauscher, R.Reifarth, A.Sauerwein, E.Stech, W.Tan, T.Thomas, M.Wiescher

Experimental cross sections of 165Ho(α, n)168Tm and 166Er(α, n)169Yb for optical potential studies relevant for the astrophysical γ process

NUCLEAR REACTIONS 165Ho, 166Er(α, n), E=10.5-15 MeV; measured Eγ, Iγ, σ(E) by activation technique using Tandem accelerator at NSL-Notre Dame. Comparison with predictions from Hauser-Feshbach calculations using TALYS and SMARAGD codes, and with previous experimental results; analyzed α-nucleus optical potential for simulations of astrophysical γ process.

doi: 10.1103/PhysRevC.89.065808
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2119.


2014TH02      Nucl.Phys. A922, 200 (2014)

T.Thomas, C.Bernards, J.-M.Regis, M.Albers, C.Fransen, J.Jolie, S.Heinze, D.Radeck, N.Warr, K.-O.Zell

The structure of 193Au within the Interacting Boson Fermion Model

NUCLEAR REACTIONS 194Pt(p, 2n), E=14 MeV. 193Au measured Eγ, Iγ(θ) , γγ-coin; deduced γ transitions, levels, J, π, δ, branching ratios, B(M1), B(E2); calculated levels, J, π, B(E2) using IBFM. 193Au deduced Bose-Fermi symmetry, IBFM parameters.

doi: 10.1016/j.nuclphysa.2013.12.004
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2014TH07      Nucl.Phys. A925, 96 (2014)

T.Thomas, J.-M.Regis, J.Jolie, S.Heinze, M.Albers, C.Bernards, C.Fransen, D.Radeck

Bose-Fermi symmetry in the odd-even gold isotopes

NUCLEAR REACTIONS 196Pt(p, xnγ), E=14 MeV; measured Eγ, Iγ(θ), γγ-coin using HORUS spectrometer equipped with HPGe. 195Au; deduced levels, J, π, γ transitions. 185,187,189,191,193,195,197,199Au calculated low-lying levels, J, π, γ transitions using IBFM within Spin(6) Bose-Fermi symmetry. Compared with data and Nuclear Data Sheets.

doi: 10.1016/j.nuclphysa.2014.02.002
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2013AL05      Nucl.Phys. A899, 1 (2013); Erratum Nucl.Phys. A947, 260 (2016)

M.Albers, K.Nomura, N.Warr, A.Blazhev, J.Jolie, D.Mucher, B.Bastin, C.Bauer, C.Bernards, L.Bettermann, V.Bildstein, J.Butterworth, M.Cappellazzo, J.Cederkall, D.Cline, I.Darby, S.Das Gupta, J.M.Daugas, T.Davinson, H.De Witte, J.Diriken, D.Filipescu, E.Fiori, C.Fransen, L.P.Gaffney, G.Georgiev, R.Gernhauser, M.Hackstein, S.Heinze, H.Hess, M.Huyse, D.Jenkins, J.Konki, M.Kowalczyk, T.Kroll, R.Krucken, J.Litzinger, R.Lutter, N.Marginean, C.Mihai, K.Moschner, P.Napiorkowski, B.S.Nara Singh, K.Nowak, J.Pakarinen, M.Pfeiffer, D.Radeck, P.Reiter, S.Rigby, L.M.Robledo, R.Rodriguez-Guzman, M.Rudigier, M.Scheck, M.Seidlitz, B.Siebeck, G.S.Simpson, P.Thole, T.Thomas, J.Van de Walle, P.Van Duppen, M.Vermeulen, D.Voulot, R.Wadsworth, F.Wenander, K.Wimmer, K.O.Zell, M.Zielinska

Shape dynamics in neutron-rich Kr isotopes: Coulomb excitation of 92Kr, 94Kr and 96Kr

NUCLEAR REACTIONS 194,196Pt(92Kr, 92Kr'), (94Kr, 94Kr'), (96Kr, 96Kr'), E=2.85 MeV/nucleon; measured projectile and target E, I(θ, t) using DSSD, Eγ, Iγ(θ) from Coulomb excitation using HPGe array and considering Doppler correction, (particle)γ-coin; calculated electromagnetic matrix elements, γ-ray yields using CC code GOSIA2, energy vs deformation using IBM-2 with self-consistent constrained HFB with Gogny functional; deduced Coulomb excitation σ, electromagnetic matrix elements using fit to data, B(E2), quadrupole moments, IBM-2 Hamiltonian parameters. 96Kr calculated levels, J, π; deduced shape coexistence.

doi: 10.1016/j.nuclphysa.2013.01.013
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2013DU02      Nucl.Phys. A903, 18 (2013)

H.Duckwitz, M.Pfeiffer, M.Albers, C.Bernards, C.Fransen, J.Jolie, P.Petkov, D.Radeck, T.Thomas, K.O.Zell

Study of vibrational signatures in 102Ru

NUCLEAR REACTIONS 100Mo(α, 2n), E=16 MeV; measured Eγ, Iγ(θ), γγ-coin using HORUS spectrometer. 102Ru deduced levels, J, π, γ-branching ratio, , mixing ratio, T1/2, B(M1), B(E2), partial γ-decay scheme using using DSAM (Doppler shift attenuation method); calculated levels, J, π, γ-branching ratio, B(E2) using IBM with U(5), O(6), U(5)-O(6). Compared also with systematics.

doi: 10.1016/j.nuclphysa.2012.11.013
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2013RU07      Phys.Rev. C 87, 064317 (2013)

M.Rudigier, G.S.Simpson, J.M.Daugas, A.Blazhev, C.Fransen, G.Gey, M.Hackstein, J.Jolie, U.Koster, T.Malkiewicz, T.Materna, M.Pfeiffer, M.Ramdhane, J.-M.Regis, W.Rother, T.Thomas, N.Warr, D.Wilmsen, J.Le Bloas, N.Pillet

Delayed γ-ray and conversion-electron spectroscopy of A=97 fission fragments

NUCLEAR REACTIONS 241Pu, 241Am(n, F), E=thermal; measured Eγ, Iγ, ce, γγ-, (fragment)γ-, (fragment)ce-, (fragment)x ray-coin, γ(t), ce(t), isomer half-lives at ILL, Grenoble using Lohengrin Mass spectrometer. 97Rb, 97Sr; deduced levels, J, π, conversion coefficients, multipolarity, Nilsson configurations. Comparison with HFB and QPRM calculations.

NUCLEAR STRUCTURE 97Rb, 97Sr; calculated levels, J, π, potential energy curves as function of deformations of low-lying 1-qp states. Quasi-particle rotor model and Hartree-Fock-Bogoliubov calculations with D1N Gogny interaction using GAMPN, ASYRMO, and PROBAMO computer codes.

doi: 10.1103/PhysRevC.87.064317
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2013TH09      Phys.Rev. C 88, 044305 (2013)

T.Thomas, K.Nomura, V.Werner, T.Ahn, N.Cooper, H.Duckwitz, M.Hinton, G.Ilie, J.Jolie, P.Petkov, D.Radeck

Evidence for shape coexistence in 98Mo

NUCLEAR REACTIONS 96Zr(α, 2n), E=16 MeV; measured Eγ, γγ-coin, γγ(θ) using YRAST Ball array at WNSL, Yale facility. 98Mo; deduced levels, J, π, mixing ratios, B(E2). Comparison with IBA model calculations. Shape coexistence and configuration mixing.

NUCLEAR STRUCTURE 96,98,100Mo; calculated potential energy surface contours in (β, γ) plane. 98Mo; calculated levels, J, π, B(E2). Comparison with experimental data. 93,95,97,99Mo; observed γ rays.

doi: 10.1103/PhysRevC.88.044305
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2012AL03      Phys.Rev.Lett. 108, 062701 (2012); Erratum Phys.Rev.Lett. 109, 209904 (2012)

M.Albers, N.Warr, K.Nomura, A.Blazhev, J.Jolie, D.Mucher, B.Bastin, C.Bauer, C.Bernards, L.Bettermann, V.Bildstein, J.Butterworth, M.Cappellazzo, J.Cederkall, D.Cline, I.Darby, S.Das Gupta, J.M.Daugas, T.Davinson, H.De Witte, J.Diriken, D.Filipescu, E.Fiori, C.Fransen, L.P.Gaffney, G.Georgiev, R.Gernhauser, M.Hackstein, S.Heinze, H.Hess, M.Huyse, D.Jenkins, J.Konki, M.Kowalczyk, T.Kroll, R.Krucken, J.Litzinger, R.Lutter, N.Marginean, C.Mihai, K.Moschner, P.Napiorkowski, B.S.Nara Singh, K.Nowak, T.Otsuka, J.Pakarinen, M.Pfeiffer, D.Radeck, P.Reiter, S.Rigby, L.M.Robledo, R.Rodriguez-Guzman, M.Rudigier, P.Sarriguren, M.Scheck, M.Seidlitz, B.Siebeck, G.Simpson, P.Thole, T.Thomas, J.Van de Walle, P.Van Duppen, M.Vermeulen, D.Voulot, R.Wadsworth, F.Wenander, K.Wimmer, K.O.Zell, M.Zielinska

Evidence for a Smooth Onset of Deformation in the Neutron-Rich Kr Isotopes

NUCLEAR REACTIONS 194,196Pt(94Kr, 94Kr'), (96Kr, 96Kr'), 285 MeV/nucleon; measured reaction products, Eγ, Iγ. 94,96Kr; deduced J, π, B(E2), spectroscopic quadrupole moments. Comparison with IBM calculations based on the constrained HFB approach using the microscopic Gogny-D1M energy density functional.

doi: 10.1103/PhysRevLett.108.062701
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2012JO06      J.Phys.:Conf.Ser. 366, 012023 (2012)

J.Jolie, C.Bernards, S.Heinze, J.M.Regis, T.Thomas

Recent advances in the application of dynamical supersymmetry to describe atomic nuclei

doi: 10.1088/1742-6596/366/1/012023
Citations: PlumX Metrics


2011BE36      Phys.Rev. C 84, 047304 (2011)

C.Bernards, W.Urban, M.Jentschel, B.Markisch, J.Jolie, C.Fransen, U.Koster, T.Materna, G.S.Simpson, T.Thomas

γγ angular-correlation analysis of 200Hg after cold-neutron capture

NUCLEAR REACTIONS 199Hg(n, γ), E=cold; measured Eγ, Iγ, γγ-coin, γγ(θ). 200Hg; deduced levels, J, π, multipolarities, mixing ratios.

doi: 10.1103/PhysRevC.84.047304
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2002TO15      Phys.Rev.Lett. 89, 052302 (2002)

J.Tojo, I.Alekseev, M.Bai, B.Bassalleck, G.Bunce, A.Deshpande, J.Doskow, S.Eilerts, D.E.Fields, Y.Goto, H.Huang, V.Hughes, K.Imai, M.Ishihara, V.Kanavets, K.Kurita, K.Kwiatkowski, B.Lewis, W.Lozowski, Y.Makdisi, H.-O.Meyer, B.V.Morozov, M.Nakamura, B.Przewoski, T.Rinckel, T.Roser, A.Rusek, N.Saito, B.Smith, D.Svirida, M.Syphers, A.Taketani, T.L.Thomas, D.Underwood, D.Wolfe, K.Yamamoto, L.Zhu

Measurement of Analyzing Power for Proton-Carbon Elastic Scattering in the Coulomb-Nuclear Interference Region with a 22-GeV/c Polarized Proton Beam

NUCLEAR REACTIONS C(polarized p, p), E at 21.7 GeV/c; measured analyzing power; deduced ratio of spin-flip to nonflip amplitude.

doi: 10.1103/PhysRevLett.89.052302
Citations: PlumX Metrics


1996AN28      Nucl.Instrum.Methods Phys.Res. A383, 13 (1996)

J.Antos, H.-Y.Chao, P.Chang, M.-T.Cheng, M.-L.Chu, R.-S.Guo, C.-L.Ho, P.-K.Teng, M.-J.Wang, S.-C.Wu, G.-P.Yeh, P.Yeh, J.Andressen, E.Barsotti, M.Bowden, S.Cihangir, H.Gonzalez, C.Grimm, B.Haynes, M.Hrycyk, J.Howell, D.Husby, W.Knopf, M.Lindenmeyer, P.Ratzmann, J.Sarge, J.Spalding, L.Spiegel, S.Tkaczyk, K.Woodbury, R.Yarema, S.Zimmerman, T.Zimmerman, C.Gay, J.Huth, J.Oliver, M.Spiropulu, R.Stroehmer, Y.Iwata, T.Ohmoto, T.Ohsugi, B.Barnett, J.Skarha, R.Snider, R.Takashima, R.Ely, M.Garcia-Sciveres, C.Haber, O.Milgrome, L.Lu, M.Bailey, N.Bruner, M.Gold, M.Hoeferkamp, J.Matthews, E.Moore, S.Seidel, T.Thomas, S.Worm, L.Yu, T.Kohriki, Y.Unno, N.Tamura, N.Bacchetta, D.Bisello, G.Bolla, J.Boudreau, E.Engels, Jr., B.T.Huffman, P.F.Shepard, R.Rosatti, F.Bedeschi, A.Menzione, G.Punzi, L.Ristori, F.Zetti, D.Bortoletto, A.Garfinkel, A.Hardmann, K.Hoffman, T.Keaffaber, N.M.Shaw, J.Cassada, P.Tipton, J.Conway, J.Done, T.Kamon, B.Tannenbaum, J.Wolinski, D.Benjamin, M.Frautschi, A.Sill, J.F.Hou

The SVX II Silicon Vertex Detector Upgrade at CDF

doi: 10.1016/S0168-9002(96)00688-2
Citations: PlumX Metrics


1980DY01      Phys.Rev. C22, 1509 (1980)

P.Dyer, M.P.Webb, R.J.Puigh, R.Vandenbosch, T.D.Thomas, M.S.Zisman

Charge Distributions for the 86Kr + 139La System at 506, 610, and 710 MeV

NUCLEAR REACTIONS 139La(86Kr, X), E=505, 610, 710 MeV; measured σ(fragment Z), σ(fragment θ, E, Z), fragment charge distribution variance vs energy loss; deduced combined fusion, fission σ, diffusion constants, reaction mechanism. Phenomenological model.

doi: 10.1103/PhysRevC.22.1509
Citations: PlumX Metrics


1980PU01      Nucl.Phys. A336, 279 (1980)

R.J.Puigh, H.Doubre, A.Lazzarini, A.Seamster, R.Vandenbosch, M.S.Zisman, T.D.Thomas

Alignment of Transferred Angular Momentum in Deeply Inelastic Collisions from Discrete γ-Ray Angular Correlations

NUCLEAR REACTIONS 166Er(86Kr, X), E=600 MeV; measured (fragment)γ-coin; deduced in-plane, out-of-plane yield of discrete γ, known multipolarity.

doi: 10.1016/0375-9474(80)90624-7
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1979DY04      Nucl.Phys. A322, 205 (1979)

P.Dyer, R.J.Puigh, R.Vandenbosch, T.D.Thomas, M.S.Zisman, L.Nunnelley

Q- and Z-Dependence of Angular Momentum Transfer in Deeply Inelastic Collisions of 86Kr with 209Bi

NUCLEAR REACTIONS 209Bi(86Kr, F), E=610 MeV; measured σ(EF, θ, φ, Z).

doi: 10.1016/0375-9474(79)90342-7
Citations: PlumX Metrics


1979PU03      Phys.Lett. 86B, 24 (1979)

R.J.Puigh, P.Dyer, R.Vandenbosch, T.D.Thomas, L.Nunnelley, M.S.Zisman

Magnitude and Alignment of Transferred Angular Momentum in Both Quasi And Deeply Inelastic Scattering

NUCLEAR REACTIONS 238U(86Kr, F), E=730 MeV; measured projectile-like fragment, fission fragment (θ, φ); deduced magnitude, alignment of transferred as function of energy loss. Transport model.

doi: 10.1016/0370-2693(79)90612-9
Citations: PlumX Metrics


1978VA07      Phys.Rev. C17, 1672 (1978)

R.Vandenbosch, M.P.Webb, P.Dyer, R.J.Puigh, R.Weisfield, T.D.Thomas, M.S.Zisman

Elastic and Deeply Inelastic Reactions in the 86Kr + 139La System at 505, 610, and 710 MeV

NUCLEAR REACTIONS 139La(86Kr, 86Kr'), (86Kr, X), E=505, 610, 710 MeV; measured elastic, quasielastic, deep inelastic σ(θ), σ(E, θ) for non-elastic products. Elastic scattering optical model analysis.

doi: 10.1103/PhysRevC.17.1672
Citations: PlumX Metrics


1977DY04      Phys.Rev.Lett. 39, 392 (1977)

P.Dyer, R.J.Puigh, R.Vandenbosch, T.D.Thomas, M.S.Zisman

Angular-Momentum Transfer in Deeply Inelastic Scattering of 610-MeV 86Kr by 209Bi

NUCLEAR REACTIONS 209Bi(86Kr, X), E=610 MeV; measured fragment fragment (θ) from fission products.

doi: 10.1103/PhysRevLett.39.392
Citations: PlumX Metrics


1976VA04      Phys.Rev.Lett. 36, 459 (1976)

R.Vandenbosch, M.P.Webb, T.D.Thomas

Energy Dependence of Deeply Inelastic Scattering of 84Kr from 208Pb

NUCLEAR REACTIONS 208Pb(84Kr, 84Kr'), E=494, 510, 718 MeV; measured σ(E(84Kr'), θ).

doi: 10.1103/PhysRevLett.36.459
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1976VA11      Phys.Rev. C13, 1893 (1976)

R.Vandenbosch, M.P.Webb, T.D.Thomas, S.W.Yates, A.M.Friedman

Elastic Scattering of 84Kr by 208Pb

NUCLEAR REACTIONS 208Pb(84Kr, 84Kr), E=494, 510, 718 MeV; measured σ(θ). Fresnel, parametrized phase shift, optical model analyses.

doi: 10.1103/PhysRevC.13.1893
Citations: PlumX Metrics


1976VA15      Phys.Rev. C13, 143 (1976)

R.Vandenbosch, M.P.Webb, T.D.Thomas

Deeply Inelastic Scattering of 84Kr from 208Pb

NUCLEAR REACTIONS 208Pb(84Kr, X), E=494, 510, 718 MeV; measured σ(θ) for quasielastic, deeply inelastic scattering; deduced integrated σ, compared with optical model absorption σ. Deflection function analysis.

doi: 10.1103/PhysRevC.13.143
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1976VA18      Nucl.Phys. A269, 210 (1976)

R.Vandenbosch, M.P.Webb, T.D.Thomas, M.S.Zisman

Energy, Angular and Charge Distributions for Deeply Inelastic Scattering of Xe by Ta and Pb

NUCLEAR REACTIONS 181Ta, 208Pb(136Xe, X), E=1120 MeV; measured σ(E, Z, θ).

doi: 10.1016/0375-9474(76)90407-3
Citations: PlumX Metrics


1976WE18      Phys.Lett. 62B, 407 (1976)

M.P.Webb, R.Vandenbosch, T.D.Thomas

Nuclear Reactions in the 86Kr + 139La System at 710 MeV

NUCLEAR REACTIONS 139La(86Kr, X), E=710 MeV; measured σ(θ); deduced reaction mechanism.

doi: 10.1016/0370-2693(76)90670-5
Citations: PlumX Metrics


1975RA21      Phys.Rev. C12, 527 (1975)

G.M.Raisbeck, P.Boerstling, R.Klapisch, T.D.Thomas

Li, Be, and B Production in the 3-GeV Proton Bombardment of Ni

NUCLEAR REACTIONS Ni(p, X), E=3 GeV; measured σ(fragment mass, θ) for Li, Be, B.

doi: 10.1103/PhysRevC.12.527
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1972RA12      Phys.Rev. C5, 1402 (1972)

M.Rajagopalan, T.D.Thomas

Emission of Alpha Particles in the Fission of 238U by 16- and 42-MeV Protons

NUCLEAR REACTIONS, Fission 238U(p, F), E=16, 42 MeV; measured σ(E(fragment), Eα, θ(α)), (fragment)(α)-coin.

doi: 10.1103/PhysRevC.5.1402
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1972RA19      Phys.Rev. C5, 2064 (1972)

M.Rajagopalan, T.D.Thomas

Angular Distribution of Alpha Particles Emitted in the Fission of 252Cf

RADIOACTIVITY, Fission 252Cf(SF); measured Iα(θ), (fragment)(γ)(θ).

doi: 10.1103/PhysRevC.5.2064
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1970MO35      Phys.Lett. 33B, 565 (1970)

U.Mosel, T.D.Thomas, P.Riesenfeldt

Ion-Ion Potentials in a Two Center Model

NUCLEAR REACTIONS 12C(12C, X), 16O(16O, X), 18O(18O, X), E not given; calculated interaction potentials.

doi: 10.1016/0370-2693(70)90350-3
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1970RI08      Phys.Rev. C2, 711 (1970)

P.W.Riesenfeldt, T.D.Thomas

Effect of Nuclear Deformability on Reaction Cross Sections

NUCLEAR REACTIONS 238U(HI, X), E=180-420 MeV; calculated σ(E); deduced nuclear deformability effect.

doi: 10.1103/PhysRevC.2.711
Citations: PlumX Metrics


1969DO06      Phys.Rev. 180, 1177 (1969)

S.R.Dolce, W.M.Gibson, T.D.Thomas

Emission Times and Yields of K X Rays Coincident with 252Cf Spontaneous Fission

RADIOACTIVITY, Fission 252Cf; measured K X-ray yields vs fragment mass; deduced K X-ray emission time.

doi: 10.1103/PhysRev.180.1177
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1968AL06      Phys.Rev. 167, 1105 (1968)

T.Alvager, R.A.Naumann, R.F.Petry, G.Sidenius, T.D.Thomas

On-Line Studies of Mass-Separated Xenon Fission Products

NUCLEAR STRUCTURE 138Cs, 139Ba, 138Xe, 139Xe, 139Cs, 137Xe, 140Xe, 140Ba, 140Cs, 141La, 141Cs, 141Xe, 140La, 141Ba, 142Xe, 142La, 142Cs, 142Ba; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.167.1105
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1968TH04      Phys.Letters 27B, 504 (1968)

T.D.Thomas, G.M.Raisbeck, P.Boerstling, G.T.Garvey, R.P.Lynch

New Isotopes, 19N and 21O, Produced in High-Energy Nuclear Reactions

NUCLEAR STRUCTURE 19N, 21O; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0370-2693(68)90207-4
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1967WH05      Phys.Rev. 154, 1174 (1967)

S.L.Whetstone, T.D.Thomas

Light Charged Particles from Spontaneous Fission of Cf252

RADIOACTIVITY 252Cf(SF); measured decay products. 1,2,3H, 3,4,6,8,10He, Li, Be; deduced energy spectra, total yields.

doi: 10.1103/physrev.154.1174
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1966TH11      Phys.Rev. 144, 1060 (1966)

T.D.Thomas, S.L.Whetstone

Emission of Alpha Particles in the Fission of U238 by 11- to 21-MeV Protons

NUCLEAR REACTIONS 238U(p, F)4He, E=11, 21 MeV; measured reaction products, Eα, Iα; deduced relative yields, emission rate.

doi: 10.1103/physrevc.5.1402
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1965WH10      Phys.Rev.Lett. 15, 298 (1965)

S.L.Whetstone, Jr., T.D.Thomas

Spontaneous Emission of Energetic He6 Particles from Cf252

RADIOACTIVITY 252Cf(SF); measured decay products, Ep, Ip, Eα, Iα. 6,8He; deduced energy spectra for 1,3H, 4,6,8He.

doi: 10.1103/physrevlett.15.298
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1963VI08      Phys.Rev. 129, 2710 (1963)

V.E.Viola, T.D.Thomas, G.T.Seaborg

Angular Distribution of Fragments from Fission Induced by Heavy Ions in Gold and Bismuth

NUCLEAR REACTIONS 197Au(14N, F), 208Bi(16O, F), E<10.2 MeV/nucleon; measured fission fragments; deduced σ(θ), model parameters.

doi: 10.1103/PhysRev.129.2710
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2494.


1962TH08      Phys.Rev. 126, 1805 (1962)

T.D.Thomas, G.E.Gordon, R.M.Latimer, G.T.Seaborg

Spallation-Fission Competition in Astatine Compound Nuclei Formed by Heavy-Ion Bombardments

NUCLEAR REACTIONS 197Au(12C, X), Pt(14N, X)202At/203At/204At/205At/206At/207At/208At/211At/208Po/211Po, E=10.4 MeV/nucleon; measured reaction products; deduced σ, α-decay T1/2. Comparison with available data.

doi: 10.1103/PhysRev.126.1805
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1961LA02      J.Inorg.Nuclear Chem. 17, 1 (1961)

R.M.Latimer, G.E.Gordon, T.D.Thomas

α-Particle Branching Ratios for Neutron-Deficient Astatine Isotopes

NUCLEAR STRUCTURE 202At, 203At, 206At, 204At, 205At; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0022-1902(61)80177-2
Citations: PlumX Metrics


1959GA03      Bull.Am.Phys.Soc. 4, No.4, 293, YA9 (1959)

C.J.Gallagher, Jr., T.D.Thomas

Beta Decay of Bk250 and Bk249


1959GA13      Nuclear Phys. 14, 1 (1959)

C.J.Gallagher, Jr., T.D.Thomas

Vibrational States in U234 Excited by Np234 Decay and Evidence for an E0-Transition between States with I≠ 0

doi: 10.1016/0029-5582(59)90066-5
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1959GO88      UCRL-8867, p.44 (1959)

G.E.Gordon, R.M.Latimer, T.D.Thomas


1958VA38      Phys.Rev. 111, 1358 (1958)

R.Vandenbosch, T.D.Thomas, S.E.Vandenbosch, R.A.Glass, G.T.Seaborg

Spallation-Fission Competition in Heaviest Element; Helium-Ion-Induced Reactions in Uranium Isotopes

doi: 10.1103/PhysRev.111.1358
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1957TH10      Phys.Rev. 106, 1228 (1957)

T.D.Thomas, R.Vandenbosch, R.A.Glass, G.T.Seaborg

Decay Properties of Pu235, Pu237, and a New Isotope Pu233

doi: 10.1103/PhysRev.106.1228
Citations: PlumX Metrics


1957TH37      Thesis, University of California (1957); UCRL-3791 (1957)

T.D.Thomas

Spallation-Fission Competition from the Compound System U233 Plus He4


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