NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = A.Kerek Found 94 matches. 2015CA09 Phys.Rev. C 92, 014327 (2015) L.Caceres, A.Lepailleur, O.Sorlin, M.Stanoiu, D.Sohler, Zs.Dombradi, S.K.Bogner, B.A.Brown, H.Hergert, J.D.Holt, A.Schwenk, F.Azaiez, B.Bastin, C.Borcea, R.Borcea, C.Bourgeois, Z.Elekes, Zs.Fulop, S.Grevy, L.Gaudefroy, G.F.Grinyer, D.Guillemaud-Mueller, F.Ibrahim, A.Kerek, A.Krasznahorkay, M.Lewitowicz, S.M.Lukyanov, J.Mrazek, F.Negoita, F.de Oliveira, Yu.-E.Penionzhkevich, Zs.Podolyak, M.G.Porquet, F.Rotaru, P.Roussel-Chomaz, M.G.Saint-Laurent, H.Savajols, G.Sletten, J.C.Thomas, J.Timar, C.Timis, Zs.Vajta Nuclear structure studies of 24F NUCLEAR REACTIONS 9Be(36S, X)24O/26F/27Ne/28Ne/29Na/30Na, E=77.6 MeV/nucleon; measured energy loss, TOF, yields using LISE achromatic spectrometer at GANIL facility. C(27Na, 24F), E=54-65 MeV/nucleon, [secondary cocktail beam of 25,26Ne, 27,28Na, 29,30Mg from C(36S, X), E=77.6 MeV/nucleon primary reaction, and separated using ALPHA and SPEG spectrometers]; measured Eγ, Iγ, (particle)γ-, γγ-coin using Chateau de Cristal array. 24F; deduced levels, J, π, branching ratios, configurations. Comparison with shell-model calculations using USDA and USDB interactions, and ab initio shell-model calculations, using interactions derived from chiral NN+3N forces by means of IM-SRG. RADIOACTIVITY 24O(β-), (β-n)[from Be(36S, X), E=77.6 MeV/nucleon using LISE spectrometer at GANIL]; measured Eγ, Iγ, Eβ, βγ-, γγ-coin, (24O)β-correlations, half-life of 24O isotope from (24O)γ-correlated decay curve, β-delayed neutron emission probability Pn using four segmented Ge clover detectors of EXOGAM array for γ rays and DSSSDs for particles. 24F; deduced levels, J, π, branching ratios, β feedings, logft. Comparison with shell-model calculations.
doi: 10.1103/PhysRevC.92.014327
2014VA02 Phys.Rev. C 89, 054323 (2014) Zs.Vajta, M.Stanoiu, D.Sohler, G.R.Jansen, F.Azaiez, Zs.Dombradi, O.Sorlin, B.A.Brown, M.Belleguic, C.Borcea, C.Bourgeois, Z.Dlouhy, Z.Elekes, Zs.Fulop, S.Grevy, D.Guillemaud-Mueller, G.Hagen, M.Hjorth-Jensen, F.Ibrahim, A.Kerek, A.Krasznahorkay, M.Lewitowicz, S.M.Lukyanov, S.Mandal, P.Mayet, J.Mrazek, F.Negoita, Yu.-E.Penionzhkevich, Zs.Podolyak, P.Roussel-Chomaz, M.G.Saint-Laurent, H.Savajols, G.Sletten, J.Timar, C.Timis, A.Yamamoto Excited states in the neutron-rich nucleus 25F NUCLEAR REACTIONS C(26Ne, 25F), (27Na, 25F), (28Na, 25F), [secondary 26Ne, 27,28Na beams from C(36S, X), E=77.5 MeV/nucleon primary reaction], E=54-65 MeV/nucleon; measured Eγ, Iγ, γγ-, (25F)γ-coin, time-of-flight using SPEG magnetic spectrometer and an array of 74 BaF2 crystals for γ-rays at GANIL facility, GEANT4 simulations. 25F; deduced levels, J, π. Comparison with shell-model calculations, coupled-cluster theory, and other data.
doi: 10.1103/PhysRevC.89.054323
2012ST01 Phys.Rev. C 85, 017303 (2012) M.Stanoiu, D.Sohler, O.Sorlin, Zs.Dombradi, F.Azaiez, B.A.Brown, C.Borcea, C.Bourgeois, Z.Elekes, Zs.Fulop, S.Grevy, D.Guillemaud-Mueller, F.Ibrahim, A.Kerek, A.Krasznahorkay, M.Lewitowicz, S.M.Lukyanov, J.Mrazek, F.Negoita, Yu.-E.Penionzhkevich, Zs.Podolyak, M.G.Porquet, P.Roussel-Chomaz, M.G.Saint-Laurent, H.Savajols, G.Sletten, J.Timar, C.Timis Spectroscopy of 26F NUCLEAR REACTIONS C, H(27Na, X), (28Na, X), [27,28Na secondary beams from C(36S, X), E=77.5 MeV/nucleon primary reaction], E=60 MeV/nucleon; measured Eγ, Iγ, σ. 26F; deduced level, J, π, configuration. 7Li, 10,11B, 11C, 23O; measured Eγ. SPEG magnetic spectrometer and BaF2 array at GANIL. Comparison with large scale shell-model calculations.
doi: 10.1103/PhysRevC.85.017303
2009FR04 Acta Phys.Pol. B40, 419 (2009) S.Franchoo, N.L.Achouri, A.Algora, A.Al-Khatib, J.-C.Angelique, F.Azaiez, D.Baiborodin, B.Bastin, D.Beaumel, M.Belleguic, G.Benzoni, Y.Blumenfeld, C.Borcea, R.Borcea, C.Bourgeois, P.Bringel, B.A.Brown, A.Burger, A.Buta, R.Chapman, E.Clement, J.-C.Dalouzy, Z.Dlouhy, Z.Dombradi, A.Drouart, Z.Elekes, C.Engelhardt, S.Fortier, Z.Fulop, L.Gaudefroy, M.Gelin, J.Gibelin, A.Gorgen, S.Grevy, D.Guillemaud-Mueller, F.Hammache, H.Hubel, S.Iacob, F.Ibrahim, K.Kemper, A.Kerek, W.Korten, A.Krasznahorkay, K.-L.Kratz, B.Laurent, M.Lazar, D.Lebhertz, M.Lewitowicz, X.Liang, E.Lienard, S.Lukyanov, S.Mandal, C.Monrozeau, J.Mrazek, L.Nalpas, A.Navin, F.Negoita, F.Nowacki, N.Orr, A.Ostrowski, T.Otsuka, D.Pantelica, Y.Penionzhkevich, J.Piekarewicz, Z.Podolyak, E.Pollacco, F.Pougheon, A.Poves, F.Rotaru, P.Roussel-Chomaz, E.Rich, J.-A.Scarpaci, M.-G.Saint-Laurent, H.Savajols, G.Sletten, D.Sohler, O.Sorlin, M.Stanoiu, I.Stefan, T.Suzuki, C.Theisen, J.Timar, C.Timis, E.Tryggestad, D.Verney, S.Williams, A.Yamamoto Recent Results from GANIL
2008ST18 Phys.Rev. C 78, 034315 (2008) M.Stanoiu, D.Sohler, O.Sorlin, F.Azaiez, Zs.Dombradi, B.A.Brown, M.Belleguic, C.Borcea, C.Bourgeois, Z.Dlouhy, Z.Elekes, Zs.Fulop, S.Grevy, D.Guillemaud-Mueller, F.Ibrahim, A.Kerek, A.Krasznahorkay, M.Lewitowicz, S.M.Lukyanov, S.Mandal, J.Mrazek, F.Negoita, Yu.-E.Penionzhkevich, Zs.Podolyak, P.Roussel-Chomaz, M.G.Saint-Laurent, H.Savajols, G.Sletten, J.Timar, C.Timis, A.Yamamoto Disappearance of the N = 14 shell gap in the carbon isotopic chain NUCLEAR REACTIONS C(24F, X), (25Ne, X), (26Ne, X), (27Na, X), (28Na, X), (29Mg, X), (30Mg, X), E=54-65 MeV/nucleon; measured Eγ, Iγ, γγ-, (particle)γ-coin. 17,18,19,20C; deduced levels, J, π. Comparisons with shell-model calculations.
doi: 10.1103/PhysRevC.78.034315
2006RU07 Phys.Rev. C 73, 044326 (2006) E.Ruchowska, W.A.Plociennik, J.Zylicz, H.Mach, J.Kvasil, A.Algora, N.Amzal, T.Back, M.G.Borge, R.Boutami, P.A.Butler, J.Cederkall, B.Cederwall, B.Fogelberg, L.M.Fraile, H.O.U.Fynbo, E.Hagebo, P.Hoff, H.Gausemel, A.Jungclaus, R.Kaczarowski, A.Kerek, W.Kurcewicz, K.Lagergren, E.Nacher, B.Rubio, A.Syntfeld, O.Tengblad, A.A.Wasilewski, L.Weissman Nuclear structure of 229Th RADIOACTIVITY 229Ac(β-) [from 238U(p, X) and subsequent decay]; measured prompt and delayed Eγ, Iγ, βγ-, γγ-coin. 229Th deduced levels, J, π, T1/2, transition probabilities, rotational band features. Potential energy surface calculations, quasiparticle-plus-phonon model calculations.
doi: 10.1103/PhysRevC.73.044326
2005SO06 Nucl.Phys. A753, 251 (2005) D.Sohler, M.Palacz, Zs.Dombradi, M.Hjorth-Jensen, C.Fahlander, L.-O.Norlin, J.Nyberg, T.Back, K.Lagergren, D.Rudolph, A.Algora, C.Andreoiu, G.de Angelis, A.Atac, D.Bazzacco, J.Cederkall, B.Cederwall, B.Fant, E.Farnea, A.Gadea, M.Gorska, H.Grawe, N.Hashimoto-Saitoh, A.Johnson, A.Kerek, W.Klamra, J.Kownacki, S.M.Lenzi, A.Likar, M.Lipoglavsek, M.Moszynski, D.R.Napoli, C.Rossi-Alvarez, H.A.Roth, T.Saitoh, D.Seweryniak, O.Skeppstedt, J.Timar, M.Weiszflog, M.Wolinska Maximally aligned states in the proton drip line nucleus 106Sb NUCLEAR REACTIONS 54Fe(58Ni, npα), E=240 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-, (neutron)γ-coin, γ-ray polarization. 106Sb deduced high-spin levels, J, π, configurations. Euroball, ISIS arrays.
doi: 10.1016/j.nuclphysa.2005.02.153
2004SO05 Nucl.Phys. A733, 37 (2004) D.Sohler, J.Timar, Zs.Dombradi, J.Cederkall, J.Huijnen, M.Lipoglavsek, M.Palacz, A.Atac, C.Fahlander, H.Grawe, A.Johnson, A.Kerek, W.Klamra, J.Kownacki, A.Likar, L.-O.Norlin, J.Nyberg, J.Persson, D.Seweryniak, G.de Angelis, P.Bednarczyk, D.Foltescu, D.Jerrestam, S.Juutinen, E.Makela, M.de Poli, H.A.Roth, T.Shizuma, O.Skeppstedt, G.Sletten, S.Tormanen, M.Weiszflog Band-terminating states in 101Ag NUCLEAR REACTIONS 50Cr(58Ni, 3pα), E=261 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-coin. 101Ag deduced high-spin levels, J, π, configurations, band termination. Cranked Nilsson-Strutinsky calculations. Nordball array.
doi: 10.1016/j.nuclphysa2003.12.002
2004ST08 Phys.Rev. C 69, 034312 (2004) M.Stanoiu, F.Azaiez, Zs.Dombradi, O.Sorlin, B.A.Brown, M.Belleguic, D.Sohler, M.G.Saint Laurent, M.J.Lopez-Jimenez, Y.E.Penionzhkevich, G.Sletten, N.L.Achouri, J.C.Angelique, F.Becker, C.Borcea, C.Bourgeois, A.Bracco, J.M.Daugas, Z.Dlouhy, C.Donzaud, J.Duprat, Zs.Fulop, D.Guillemaud-Mueller, S.Grevy, F.Ibrahim, A.Kerek, A.Krasznahorkay, M.Lewitowicz, S.Leenhardt, S.Lukyanov, P.Mayet, S.Mandal, H.van der Marel, W.Mittig, J.Mrazek, F.Negoita, F.De Oliveira-Santos, Zs.Podolyak, F.Pougheon, M.G.Porquet, P.Roussel-Chomaz, H.Savajols, Y.Sobolev, C.Stodel, J.Timar, A.Yamamoto N = 14 and 16 shell gaps in neutron-rich oxygen isotopes NUCLEAR REACTIONS Be(36S, X)20O/21O/22O/23O, E=77.5 MeV/nucleon; H, C(24F, X), (25Ne, X), (26Ne, X), (27Na, X), (28Na, X), (29Mg, X), (30Mg, X)20O/21O/22O/23O/24O, E=54-65 MeV/nucleon; measured Eγ, Iγ, γγ-, (particle)γ-coin. 20,21,22,23,24O deduced levels, J, π, neutron shell gap features. Single-step and double-step fragmentation. Shell model analysis.
doi: 10.1103/PhysRevC.69.034312
2004ST10 Eur.Phys.J. A 20, 95 (2004) M.Stanoiu, F.Azaiez, F.Becker, M.Belleguic, C.Borcea, C.Bourgeois, B.A.Brown, Z.Dlouhy, Z.Dombradi, Z.Fulop, H.Grawe, S.Grevy, F.Ibrahim, A.Kerek, A.Krasznahorkay, M.Lewitowicz, S.Lukyanov, H.van der Marel, P.Mayet, J.Mrazek, S.Mandal, D.Guillemaud-Mueller, F.Negoita, Y.E.Penionzhkevich, Z.Podolyak, P.Roussel-Chomaz, M.G.Saint Laurent, H.Savajols, O.Sorlin, G.Sletten, D.Sohler, J.Timar, C.Timis, A.Yamamoto Study of drip line nuclei through two-step fragmentation NUCLEAR REACTIONS C(25Ne, X), (26Ne, X), (27Na, X), (28Na, X), (29Mg, X), (30Mg, X)17C/18C/19C/20C/22O/24O, E not given; measured Eγ, Iγ, (particle)γ-coin. 17,18,19,20C, 22,24O deduced levels, J, π, configurations. Two-step fragmentation.
doi: 10.1140/epja/i2002-10329-8
2004ST29 Nucl.Phys. A746, 135c (2004) M.Stanoiu, F.Azaiez, Zs.Dombradi, O.Sorlin, B.A.Brown, M.Belleguic, D.Sohler, M.G.Saint Laurent, Y.E.Penionzhkevich, G.Sletten, C.Borcea, C.Bourgeois, A.Bracco, J.M.Daugas, Z.Dlouhy, C.Donzaud, Zs.Fulop, D.Guillemaud-Mueller, S.Grevy, F.Ibrahim, A.Kerek, A.Krasznahorkay, M.Lewitowicz, S.Lukyanov, P.Mayet, S.Mandal, W.Mittig, J.Mrazek, F.Negoita, F.De Oliveira-Santos, Zs.Podolyak, F.Pougheon, P.Roussel-Chomaz, H.Savajols, Y.Sobolev, C.Stodel, J.Timar, A.Yamamoto Study of neutron rich Carbon and Oxygen nuclei up to drip line NUCLEAR STRUCTURE 17,18,19,20C, 23,24O; analyzed data; deduced levels.
doi: 10.1016/j.nuclphysa.2004.09.022
2003SO04 Eur.Phys.J. A 16, 171 (2003) D.Sohler, Zs.Dombradi, J.Blomqvist, J.Cederkall, J.Huijnen, M.Lipoglavsek, M.Palacz, A.Atac, C.Fahlander, H.Grawe, A.Johnson, A.Kerek, W.Klamra, J.Kownacki, A.Likar, L.-O.Norlin, J.Nyberg, J.Persson, D.Seweryniak, G.de Angelis, P.Bednarczyk, D.Foltescu, D.Jerrestam, S.Juutinen, E.Makela, M.de Poli, H.A.Roth, T.Shizuma, O.Skeppstedt, G.Sletten, J.Timar, S.Tormanen, M.Weiszflog Maximally aligned states in 99Ag NUCLEAR REACTIONS 50Cr(58Ni, p2α), E=261 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-coin. 99Ag deduced high-spin levels, J, π, configurations. Nordball array, shell model calculations.
doi: 10.1140/epja/i2002-10092-x
2002SO12 Nucl.Phys. A708, 181 (2002) D.Sohler, M.Palacz, Zs.Dombradi, J.Blomqvist, C.Fahlander, L.-O.Norlin, J.Nyberg, T.Back, K.Lagergren, D.Rudolph, A.Algora, C.Andreoiu, G.de Angelis, A.Atac, D.Bazzacco, J.Cederkall, B.Cederwall, B.Fant, E.Farnea, A.Gadea, M.Gorska, H.Grawe, N.Hashimoto-Saitoh, A.Johnson, A.Kerek, W.Klamra, J.Kownacki, S.M.Lenzi, A.Likar, M.Lipoglavsek, M.Moszynski, D.R.Napoli, C.Rossi-Alvarez, H.A.Roth, T.Saitoh, D.Seweryniak, O.Skeppstedt, J.Timar, M.Weiszflog, M.Wolinska Neutron Excitations Across the N = 50 Shell Gap in 102In NUCLEAR REACTIONS 54Fe(58Ni, np2α), E=240 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-, (neutron)γ-coin, γ-ray polarization. 102In deduced levels, J, π, configurations, transition multipolarities. Euroball and ISIS arrays, neutron wall. Comparison with shell model calculations.
doi: 10.1016/S0375-9474(02)01014-X
2001FA01 Phys.Rev. C63, 021307 (2001) C.Fahlander, M.Palacz, D.Rudolph, D.Sohler, J.Blomqvist, J.Kownacki, K.Lagergren, L.O.Norlin, J.Nyberg, A.Algora, C.Andreoiu, G.de Angelis, A.Atac, D.Bazzacco, L.Berglund, T.Back, J.Cederkall, B.Cederwall, Zs.Dombradi, B.Fant, E.Farnea, A.Gadea, M.Gorska, H.Grawe, N.Hashimoto-Saitoh, A.Johnson, A.Kerek, W.Klamra, S.M.Lenzi, A.Likar, M.Lipoglavsek, M.Moszynski, D.R.Napoli, C.Rossi-Alvarez, H.A.Roth, T.Saitoh, D.Seweryniak, O.Skeppstedt, M.Weiszflog, M.Wolinska Excited States in 103Sn: Neutron single-particle energies with respect to 100Sn NUCLEAR REACTIONS 54Fe(58Ni, n2α), E=240 MeV; measured Eγ, Iγ, (neutron)γ-, (charged particle)γ-, γγ-coin. 103Sn deduced levels, J, π, single particle neutron orbital energies. Comparison with other Sn isotopes and Shell model calculations. Euroball array.
doi: 10.1103/PhysRevC.63.021307
2001PA12 Acta Phys.Pol. B32, 999 (2001) M.Palacz, C.Fahlander, D.Sohler, D.Rudolph, J.Blomqvist, J.Kownacki, K.Lagergren, L.O.Norlin, J.Nyberg, A.Algora, C.Andreoiu, G.De Angelis, A.Atac, D.Bazzacco, L.Berglund, T.Back, J.Cederkall, B.Cederwall, Zs.Dombradi, B.Fant, E.Farnea, A.Gadea, M.Gorska, H.Grawe, N.Hashimoto-Saitoh, A.Johnson, A.Kerek, W.Klamra, S.M.Lenzi, A.Likar, M.Lipoglavsek, M.Moszynski, D.Napoli, C.Rossi-Alvarez, H.Roth, T.Saitoh, D.Seweryniak, O.Skeppstedt, M.Weiszflog, M.Wolinska Investigations of Neutron Deficient Nuclei close to 100Sn with Euroball NUCLEAR REACTIONS 54Fe(58Ni, n2α), E=240 MeV; measured Eγ, Iγ, γγ-, (neutron)γ-, (charged particle)γ-coin. 103Sn deduced levels, possible J, π. Euroball array. Comparison with shell model.
2001PE05 Nucl.Phys. A686, 41 (2001) G.E.Perez, D.Sohler, A.Algora, Zs.Dombradi, B.M.Nyako, J.Timar, L.Zolnai, R.Wyss, J.Cederkall, A.Johnson, A.Kerek, W.Klamra, L.-O.Norlin, M.Lipoglavsek, C.Fahlander, A.Likar, M.Palacz, A.Atac, J.Nyberg, J.Persson, A.Gizon, J.Gizon, A.J.Boston, E.S.Paul, H.Grawe, R.Schubart, D.T.Joss, S.Juutinen, E.Makela, J.Kownacki, M.de Poli, P.Bednarczyk, G.de Angelis, D.Seweryniak, D.Foltescu, H.A.Roth, O.Skeppstedt, D.Jerrestam, T.Shizuma, G.Sletten, S.Tormanen Structure of High-Spin States in 100Pd NUCLEAR REACTIONS 50Cr(58Ni, 4pα), E=261 MeV; 70Zn(36S, 6n), E=130 MeV; measured Eγ, Iγ, γγ-, (particle)γ-coin, γ-ray angular correlation and linear polarization. 100Pd deduced high-spin levels, J, π, multipolarities, terminating bands. Nordball and Eurogam II arrays, cranked mean-field calculations.
doi: 10.1016/S0375-9474(00)00513-3
2000PA16 Nucl.Instrum.Methods Phys.Res. A443, 304 (2000) G.Pausch, H.Prade, M.Sobiella, H.Schnare, R.Schwengner, L.Kaubler, C.Borcan, H.-G.Ortlepp, U.Oehmichen, H.Grawe, R.Schubart, J.Gerl, J.Cederkall, A.Johnson, A.Kerek, W.Klamra, M.Moszynski, D.Wolski, M.Kapusta, A.Axelsson, M.Weiszflog, T.Hartlein, D.Pansegrau, G.de Angelis, S.Ashrafi, A.Likar, M.Lipoglavsek RoSiB - A 4π Silcon Ball for Charged-Particle Detection in EUROBALL NUCLEAR REACTIONS 46Ti(58Ni, xnypzα), E=228 MeV; 58Ni(16O, xnypzα), E=95 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-coin; deduced detector characteristics. Monte Carlo simulation.
doi: 10.1016/S0168-9002(99)01090-6
1999DA10 Phys.Rev. C59, 1956 (1999) I.Danko, D.Sohler, Zs.Dombradi, S.Brant, V.Krstic, J.Cederkall, M.Lipoglavsek, M.Palacz, J.Persson, A.Atac, C.Fahlander, H.Grawe, A.Johnson, A.Kerek, W.Klamra, J.Kownacki, A.Likar, L.-O.Norlin, J.Nyberg, V.Paar, R.Schubart, D.Seweryniak, D.Vretenar, G.de Angelis, P.Bednarczyk, D.Foltescu, D.Jerrestam, S.Juutinen, E.Makela, B.M.Nyako, M.de Poli, H.A.Roth, T.Shizuma, O.Skeppstedt, G.Sletten, S.Tormanen Collective and Broken Pair States of 65, 67Ga NUCLEAR REACTIONS 12C(58Ni, pα), (58Ni, 3p), E=261 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-, (neutron)γ-coin. 65,67Ga deduced high-spin levels, J, π, configurations. Nordball array. NUCLEAR STRUCTURE 65,67Ga; calculated levels, J, π, B(E2), B(M1). Interacting boson-fermion plus interacting pair model.
doi: 10.1103/PhysRevC.59.1956
1999SO08 Phys.Rev. C59, 1324 (1999) D.Sohler, J.Cederkall, M.Lipoglavsek, Zs.Dombradi, M.Gorska, J.Persson, D.Seweryniak, I.Ahmad, A.Atac, R.A.Bark, J.Blomqvist, M.P.Carpenter, B.Cederwall, C.N.Davids, C.Fahlander, S.M.Fischer, H.Grawe, G.Hackman, R.V.F.Janssens, A.Johnson, A.Kerek, W.Klamra, J.Kownacki, C.J.Lister, S.Mitarai, D.Nisius, L.-O.Norlin, J.Nyberg, G.Poli, P.Reiter, J.J.Ressler, H.A.Roth, J.Schwartz, G.Sletten, J.Uusitalo, W.B.Walters, M.Weiszflog Yrast States of the Proton Drip Line Nucleus 106Sb NUCLEAR REACTIONS 54Fe(58Ni, npα), E=261 MeV; measured Eγ, Iγ, (charged particle)γ-, (neutron)γ-, γγ-coin. 106Sb deduced levels, J, π. Cluster detectors, Si-ball. Shell model analysis. RADIOACTIVITY 106Sb(IT) [from 50Cr(58Ni, np), E=220 MeV]; measured Eγ, Iγ(t). 106Sb deduced isomeric state T1/2, ICC. Fragment mass analyzer.
doi: 10.1103/PhysRevC.59.1324
1998SO23 Nucl.Phys. A644, 141 (1998) D.Sohler, Zs.Dombradi, S.Brant, J.Cederkall, M.Lipoglavsek, M.Palacz, V.Paar, J.Persson, A.Atac, C.Fahlander, H.Grawe, A.Johnson, A.Kerek, W.Klamra, J.Kownacki, A.Likar, L.-O.Norlin, J.Nyberg, R.Schubart, D.Seweryniak, G.de Angelis, P.Bednarczyk, D.Foltescu, D.Jerrestam, S.Juutinen, E.Makela, B.M.Nyako, M.de Poli, H.A.Roth, T.Shizuma, O.Skeppstedt, G.Sletten, S.Tormanen Structure of 68As Studied via the 12C(58Ni, pn) Reaction NUCLEAR REACTIONS 12C(58Ni, np), E=261 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-, (neutron)γ-coin, angular distribution ratios. 68As deduced levels, J, π. Enriched targets, Nordball array. Interacting boson-fermion-fermion model calculations.
doi: 10.1016/S0375-9474(98)00575-2
1998SO24 Eur.Phys.J. A 3, 209 (1998) D.Sohler, J.Cederkall, Zs.Dombradi, J.Persson, B.Cederwall, A.Johnson, L.-O.Norlin, M.Weiszflog, A.Atac, J.Blomquist, R.A.Bark, A.Kerek, W.Klamra, J.Kownacki, M.Lipoglavsek, S.Mitarai, J.Nyberg, H.A.Roth, G.Sletten Spectroscopy of Neutron Deficient 108Te NUCLEAR REACTIONS 54Fe(58Ni, 2n2p), E=261 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-, (neutron)γ-coin. 108Te deduced levels, J, π, configurations.
doi: 10.1007/s100500050169
1997KO51 Nucl.Phys. A627, 239 (1997) J.Kownacki, M.Lipoglavsek, L.-O.Norlin, J.Nyberg, D.Seweryniak, J.Cederkall, M.Palacz, J.Persson, A.Atac, B.Cederwall, C.Fahlander, H.Grawe, A.Johnson, A.Kerek, W.Klamra, M.Karny, F.Liden, A.Likar, R.Schubart, R.Wyss, E.Adamides, G.de Angelis, P.Bednarczyk, Zs.Dombradi, D.Foltescu, M.Gorska, E.Ideguchi, D.Jerrestam, R.Julin, S.Juutinen, S.Mitarai, E.Makela, G.Perez, M.Piiparinen, M.de Poli, H.A.Roth, T.Shizuma, O.Skeppstedt, G.Sletten, S.Tormanen, T.Vass, A.Virtanen High-Spin Studies of the Neutron Deficient Nuclei 103In, 105In, 107In, and 109In NUCLEAR REACTIONS 50Cr(58Ni, 2n3p), (58Ni, pα), (58Ni, 3p), E=261 MeV; 54Fe(58Ni, p2α), (58Ni, 5p), (58Ni, 3pα), E=270 MeV; 92Mo(19F, 2p), E=95 MeV; measured Eγ, Iγ(θ), γγ-coin. 103,105,107,109In deduced high-spin levels, J, π, configuration. Shell model, hole-core coupling scheme.
doi: 10.1016/S0375-9474(97)00479-X
1997NO13 Nucl.Phys. A626, 511c (1997) D.Novak, A.Kerek, W.Klamra, L.-O.Norlin, G.Zetterstrom, L.Bagge, A.Kallberg, A.Paal, K.G.Rensfelt, J.Gal, J.Molnar Scraping the CRYRING Beam - A Simple Diagnostic Tool
doi: 10.1016/S0375-9474(97)00576-9
1997PA20 Acta Phys.Pol. B28, 309 (1997) M.Palacz, J.Cederkall, M.Lipoglavsek, J.Persson, A.Atac, J.Blomqvist, H.Grawe, C.Fahlander, J.Iwanicki, A.Johnson, A.Kerek, W.Klamra, J.Kownacki, A.Likar, L.-O.Norlin, J.Nyberg, R.Schubart, D.Seweryniak, Z.Sujkowski, R.Wyss, G.de Angelis, P.Bednarczyk, Zs.Dombradi, D.Foltescu, D.Jerrestam, S.Juutinen, E.Makela, G.Perez, M.de Poli, H.A.Roth, T.Shizuma, O.Skeppstedt, G.Sletten, S.Tormanen, T.Vass In Beam γ-Ray Spectroscopy of Very Neutron Deficient Odd-Cadmium Isotopes NUCLEAR REACTIONS 50Cr(58Ni, n2α), (58Ni, n2pα), (58Ni, n4p), E not given; measured Eγ, Iγ, γγ-coin. 99,101,103Cd deduced high-spin levels, J, π. Results from other Cd isotopes compared. NUCLEAR STRUCTURE 99,101,103Cd; calculated high-spin levels. Shell model.
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1997PA25 Nucl.Phys. A624, 210 (1997) M.Palacz, J.Cederkall, M.Lipoglavsek, J.Persson, A.Atac, J.Blomqvist, H.Grawe, C.Fahlander, J.Iwanicki, A.Johnson, A.Kerek, J.Kownacki, A.Likar, L.-O.Norlin, J.Nyberg, R.Schubart, D.Seweryniak, Z.Sujkowski, R.Wyss, G.de Angelis, P.Bednarczyk, Zs.Dombradi, D.Foltescu, D.Jerrestam, S.Juutinen, E.Makela, G.Perez, M.de Poli, H.A.Roth, T.Shizuma, O.Skeppstedt, G.Sletten, S.Tormanen, T.Vass In-Beam γ-Ray Spectroscopy of 103Cd NUCLEAR REACTIONS 58Ni(50Cr, 4pnγ), E=216-261 MeV; measured γγ-coin, Eγ, Iγ. 103Cd deduced high-spin levels, J, π, band structure.
doi: 10.1016/S0375-9474(97)00325-4
1997PA34 Nucl.Phys. A627, 162 (1997) M.Palacz, D.Seweryniak, A.Atac, J.Blomqvist, B.Cederwall, C.Fahlander, A.Johnson, A.Kerek, J.Kownacki, L.-O.Norlin, J.Nyberg, R.Wyss, E.Ideguchi, R.Julin, S.Juutinen, S.Mitarai, M.Piiparinen, G.Sletten, S.Tormanen, A.Virtanen In-Beam γ-Ray Spectroscopy of 56Co NUCLEAR REACTIONS 32S(27Al, n2p), E=95 MeV; measured Eγ, Iγ, γγ-coin. 56Co deduced high-spin levels, J, π, configurations, particle-hole excitations. Shell model calculations.
doi: 10.1016/S0375-9474(97)00507-1
1997PE25 Nucl.Phys. A627, 101 (1997) J.Persson, J.Cederkall, M.Lipoglavsek, M.Palacz, A.Atac, J.Blomqvist, C.Fahlander, H.Grawe, A.Johnson, A.Kerek, W.Klamra, J.Kownacki, A.Likar, L.-O.Norlin, J.Nyberg, R.Schubart, D.Seweryniak, G.de Angelis, P.Bednarczyk, Zs.Dombradi, D.Foltescu, D.Jerrestam, S.Juutinen, E.Makela, G.Perez, M.de Poli, H.A.Roth, T.Shizuma, O.Skeppstedt, G.Sletten, S.Tormanen, T.Vass In-Beam γ-Ray Spectroscopy of 102Cd NUCLEAR REACTIONS 58Ni(50Cr, 2pα), E=261 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ). 102Cd deduced high-spin levels, J, π, transitions multipolarity. Shell model calculations.
doi: 10.1016/S0375-9474(97)00405-3
1997SO06 Z.Phys. A357, 239 (1997) D.Sohler, Zs.Dombradi, S.Brant, J.Cederkall, M.Lipoglavsek, M.Palacz, V.Paar, J.Persson, A.Atac, C.Fahlander, H.Grawe, A.Johnson, A.Kerek, W.Klamra, J.Kownacki, A.Likar, L.-O.Norlin, J.Nyberg, R.Schubart, D.Seweryniak, G.de Angelis, P.Bednarczyk, D.Foltescu, M.Fayez-Hassan, D.Jerrestam, S.Juutinen, E.Makela, B.M.Nyako, M.de Poli, H.A.Roth, T.Shizuma, O.Skeppstedt, G.Sletten, S.Tormanen Spectroscopy of Neutron Deficient 65Ge NUCLEAR REACTIONS 12C(58Ni, nα), E=261 MeV; measured γγ-coin, Iγ(θ). 65Ge deduced high-spin levels, J, π. Interacting boson-fermion model.
doi: 10.1007/s002180050238
1996KO23 Acta Phys.Pol. B27, 87 (1996) J.Kownacki, A.Atac, J.Cederkall, B.Cederwall, C.Fahlander, H.Grawe, E.Ideguchi, A.Johnson, R.Julin, S.Juutinen, M.Karny, A.Kerek, W.Klamra, A.Likar, M.Lipoglavsek, L.-O.Norlin, J.Nyberg, S.Mitarai, E.Makela, M.Palacz, J.Persson, M.Piiparinen, D.Seweryniak, R.Schubart, G.Sletten, S.Tormanen, A.Virtanen, R.Wyss The Isospin Dependent p-n Multiplets in the Region of Doubly Magic 100Sn NUCLEAR REACTIONS 50Cr, 54Fe(58Ni, X), E=261, 270 MeV; measured γγ-coin, γγ(θ). 102,104,106,108In deduced levels, configurations. Information on 99Cd, 101In, 106,107,108Sb, 108,109Te also obtained.
1996LI06 Phys.Rev.Lett. 76, 888 (1996) M.Lipoglavsek, J.Cederkall, M.Palacz, J.Persson, A.Atac, J.Blomqvist, C.Fahlander, H.Grawe, A.Johnson, A.Kerek, W.Klamra, J.Kownacki, A.Likar, L.-O.Norlin, J.Nyberg, R.Schubart, D.Seweryniak, G.de Angelis, P.Bednarczyk, Zs.Dombradi, D.Foltescu, D.Jerrestam, S.Juutinen, E.Makela, G.Perez, M.de Poli, H.A.Roth, T.Shizuma, O.Skeppstedt, G.Sletten, S.Tormanen, T.Vass Stability of 50100Sn50 Deduced from Excited States in 4899Cd51 NUCLEAR REACTIONS 50Cr(58Ni, X), E=261 MeV; measured Eγ, Iγ, γγ-coin, neutron, α-particle multiplicity intensity ratios for 99,101Cd, 105,103,104In, 98Ag, 97Pd, 95Rh. 99Cd deduced high-spin levels, J, π, T1/2, B(λ) in one case.
doi: 10.1103/PhysRevLett.76.888
1996PA30 Nucl.Phys. A608, 227 (1996) M.Palacz, J.Cederkall, M.Lipoglavsek, J.Persson, A.Atac, J.Blomqvist, H.Grawe, C.Fahlander, A.Johnson, A.Kerek, J.Kownacki, A.Likar, L.-O.Norlin, J.Nyberg, R.Schubart, D.Seweryniak, Z.Sujkowski, R.Wyss, G.de Angelis, P.Bednarczyk, Zs.Dombradi, D.Foltescu, D.Jerrestam, S.Juutinen, E.Makela, G.Perez, M.de Poli, H.A.Roth, T.Shizuma, O.Skeppstedt, G.Sletten, S.Tormanen, T.Vass In-Beam γ-Ray Spectroscopy of 101Cd NUCLEAR REACTIONS 58Ni(50Cr, n2pα), E=261 MeV; measured γγ-coin, γγ(θ), γγ(t). 101Cd deduced high-spin levels, J, π, B(λ). Shell model calculations.
doi: 10.1016/S0375-9474(96)00287-4
1996PE13 Acta Phys.Pol. B27, 171 (1996) J.Persson, J.Cederkall, M.Lipoglavsek, M.Palacz, A.Atac, C.Fahlander, H.Grawe, A.Johnson, A.Kerek, W.Klamra, J.Kownacki, A.Likar, L.-O.Norlin, J.Nyberg, R.Schubart, D.Seweryniak, G.De Angelis, P.Bednarczyk, Zs.Dombradi, D.Foltescu, D.Jerrestam, S.Juutinen, E.Makela, G.Perez, M.De Poli, H.A.Roth, T.Shizuma, O.Skeppstedt, G.Sletten, S.Tormanen, T.Vass New Spectroscopic Data on 102Cd NUCLEAR REACTIONS 50Cr(58Ni, 2pα), E=261 MeV; measured particle gated projection γ spectra. 102Cd deduced levels, J, π, band structure, configuration.
1995CE01 Nucl.Phys. A581, 189 (1995) J.Cederkall, B.Cederwall, A.Johnson, D.Seweryniak, J.Nyberg, L.-O.Norlin, J.Blomqvist, C.Fahlander, R.Wyss, A.Kerek, J.Kownacki, A.Atac, E.Adamides, E.Ideguchi, R.Julin, S.Juutinen, W.Karczmarczyk, S.Mitarai, M.Piiparinen, R.Schubart, G.Sletten, S.Tormanen, A.Virtanen First Observation of Excited States in 108Sb NUCLEAR REACTIONS 54Fe(58Ni, n3p), E=270 MeV; measured Eγ, γγ(θ) (γγ)(particle)-coin. 108Sb deduced high-spin levels, B(M1)/B(E2) ratios, configurations. Total Routhian surfaces calculations.
doi: 10.1016/0375-9474(94)00443-Q
1995DO13 Phys.Rev. C51, 2394 (1995) Zs.Dombradi, B.M.Nyako, G.E.Perez, A.Algora, C.Fahlander, D.Seweryniak, J.Nyberg, A.Atac, B.Cederwall, A.Johnson, A.Kerek, J.Kownacki, L.-O.Norlin, R.Wyss, E.Adamides, E.Ideguchi, R.Julin, S.Juutinen, W.Karczmarczyk, S.Mitarai, M.Piiparinen, R.Schubart, G.Sletten, S.Tormanen, A.Virtanen High-Spin Spectroscopy of 109Te NUCLEAR REACTIONS 54Fe(58Ni, n2p), E=270 MeV; measured γγ-coin, Eγ, Iγ. 109Te deduced levels, J, π, high-spin band structure, configurations. Particle-vibration coupling model, total Routhian surface calculations.
doi: 10.1103/PhysRevC.51.2394
1995FO20 Phys.Scr. T56, 79 (1995) B.Fogelberg, M.Hellstrom, D.Jerrestam, H.Mach, J.Blomqvist, A.Kerek, L.O.Norlin, J.P.Omtvedt The Doubly Closed Shell Nucleus 132Sn: Collectivity and p-h states RADIOACTIVITY 132In(β-) [from 235U(n, F), E=thermal]; measured γγ-coin, βγγ(t). 132Sn deduced levels, J, π, T1/2, collectivity, other shape features. Model comparison.
doi: 10.1088/0031-8949/1995/T56/012
1995JE04 Nucl.Phys. A593, 162 (1995) D.Jerrestam, B.Fogelberg, A.Kerek, W.Klamra, F.Liden, L.O.Norlin, J.Kownacki, D.Seweryniak, Z.Zelazny, C.Fahlander, J.Nyberg, M.Guttormsen, J.Rekstad, T.Spedstad-Tveter, A.Gizon, J.Gizon, R.Bark, G.Sletten, M.Piiparinen, Z.Preibisz, T.F.Thorsteinsen, E.Ideguchi, S.Mitarai In-Beam Spectroscopic Studies of the Nucleus 105Cd NUCLEAR REACTIONS 106Cd(p, np), E=30 MeV; 106Cd(3He, 2n2p), E=75 MeV; 92Zr(16O, 3n), E=77 MeV; 76Ge(34S, 5n), E=148 MeV; measured γγ, γγ(particle)-coin, Eγ, Iγ, DCO ratios. 105Cd deduced levels, J, π, band structure, configuration. Compton suppressed Ge-detector array. Model calculations.
doi: 10.1016/0375-9474(95)00334-W
1995KL02 Z.Phys. A352, 117 (1995) W.Klamra, E.Adamides, A.Atac, R.A.Bark, B.Cederwall, C.Fahlander, B.Fogelberg, A.Gizon, J.Gizon, H.Grawe, E.Ideguchi, D.Jerrestam, A.Johnson, R.Julin, S.Juutinen, W.Kaczmarczyk, A.Kerek, J.Kownacki, S.Mitarai, L.O.Norlin, J.Nyberg, M.Piiparinen, R.Schubart, D.Seweryniak, G.Sletten, S.Tormanen, A.Virtanen, R.Wyss High Spin Band Structures in 104Cd NUCLEAR REACTIONS 92Zr(16O, xn), E=83 MeV; 76Ge(34S, xn), E=148 MeV; 54Fe(58Ni, X), E=270 MeV; measured γγ-coin. 104Cd deduced high-spin levels, J, π, configuration, band structure.
doi: 10.1007/BF01298895
1995MA49 Nucl.Phys. A588, 179c (1995) H.Mach, B.Fogelberg, M.Hellstrom, D.Jerrestam, J.Blomqvist, A.Kerek, L.O.Norlin, J.P.Omtvedt, K.I.Erokhina, V.I.Isakov Detailed Spectroscopy of Doubly-Magic 132Sn and Its Neighbours; Perspective for further studies at PIAFE RADIOACTIVITY 132In(β-); 132Sn(β-) [from 132In(β--decay)]; 123Sb(β-) [from 132Sn(β--decay)]; analyzed β-decay data; 132Sn deduced levels, J, π, configuration. 132Sb deduced levels, J, π, configuration, δ(E2/M1), B(λ).
doi: 10.1016/0375-9474(95)00136-O
1995SE08 Nucl.Phys. A589, 175 (1995) D.Seweryniak, J.Kownacki, L.-O.Norlin, C.Fahlander, A.Atac, J.Blomqvist, B.Cederwall, H.Grawe, A.Johnson, A.Kerek, J.Nyberg, R.Schubart, E.Adamides, E.Ideguchi, R.Julin, S.Juutinen, W.Karczmarczyk, S.Mitarai, M.Piiparinen, G.Sletten, S.Tormanen, A.Virtanen In-Beam Study of 102In, 104In and 106In NUCLEAR REACTIONS 54Fe(58Ni, np2α), (58Ni, n3pα), (58Ni, n5p), E=270 MeV; measured Eγ, Iγ, γγ(θ), γγ-coin. 102,104,106In deduced levels, J, π. Enriched target, array of Compton-suppressed Ge detectors, charged-particle detectors, neutron detectors. Shell-model calculations.
doi: 10.1016/0375-9474(95)00060-E
1994DO22 Z.Phys. A350, 3 (1994) Zs.Dombradi, B.M.Nyako, G.E.Perez, A.Algora, C.Fahlander, D.Seweryniak, J.Nyberg, A.Atac, B.Cederwall, A.Johnson, A.Kerek, J.Kownacki, L.-O.Norlin, R.Wyss, E.Adamides, E.Ideguchi, R.Julin, S.Juutinen, W.Karczmarczyk, S.Mitarai, M.Piiparinen, R.Schubart, G.Sletten, S.Tormanen, A.Virtanen Identification and Spectroscopy of the 108Te Nucleus NUCLEAR REACTIONS 54Fe(58Ni, X), E=270 MeV; measured γγ(particle)-coin, Iγ. 108Te deduced high-spin levels, J, π, γ-multipolarity.
1994FA12 Nucl.Phys. A577, 773 (1994) C.Fahlander, D.Seweryniak, J.Nyberg, Zs.Dombradi, G.E.Perez, M.Jozsa, B.M.Nyako, A.Atac, B.Cederwall, A.Johnson, A.Kerek, J.Kownacki, L.-O.Norlin, R.Wyss, E.Adamides, E.Ideguchi, R.Julin, S.Juutinen, W.Karczmarczyk, S.Mitarai, M.Piiparinen, R.Schubart, G.Sletten, S.Tormanen, A.Virtanen In-Beam Spectroscopy of 110Te NUCLEAR REACTIONS 54Fe(58Ni, 2p), E=270 MeV; measured Eγ, Iγ, Iγγ(θ), γγ-coin. 110Te deduced high-spin levels, J, π, experimental routhians, aligned angular momentum. Enriched target, array of Compton-suppressed Ge detectors, neutron, charged particle detectors. Cranked shell model calculations.
doi: 10.1016/0375-9474(94)90944-X
1994FO14 Phys.Rev.Lett. 73, 2413 (1994) B.Fogelberg, M.Hellstrom, D.Jerrestam, H.Mach, J.Blomqvist, A.Kerek, L.O.Norlin, J.P.Omtvedt Detailed Spectroscopy of the Doubly Closed Shell Nucleus 132Sn: First observation of octupole collectivity RADIOACTIVITY 132In(β-) [from 235U(n, F), E=thermal]; measured γγ-coin, γγ(θ), βγγ(t). 132Sn deduced levels, J, π, shape features.
doi: 10.1103/PhysRevLett.73.2413
1994KA32 Z.Phys. A350, 179 (1994) M.Karny, J.Kownacki, D.Seweryniak, A.Atac, B.Cederwall, C.Fahlander, A.Johnson, A.Kerek, L.-O.Norlin, J.Nyberg, E.Adamides, E.Ideguchi, R.Julin, S.Juutinen, W.Karczmarczyk, S.Mitarai, M.Piiparinen, R.Schubart, G.Sletten, S.Tormanen, A.Virtanen Excited States of 111I and the Observation of a 21 ns Isomer NUCLEAR REACTIONS 54Fe(58Ni, X), E=220 MeV; measured γγ-, γγ(particle)-coin. 111I deduced levels, possible high-spin J, π. Shell model comparison.
doi: 10.1007/BF01289577
1994SE01 Phys.Lett. 321B, 323 (1994) D.Seweryniak, J.Cederkall, B.Cederwall, J.Blomqvist, C.Fahlander, A.Johnson, L.-O.Norlin, J.Nyberg, A.Atac, A.Kerek, J.Kownacki, R.Wyss, E.Adamides, H.Grawe, E.Ideguchi, R.Julin, S.Juutinen, W.Karczmarczyk, S.Mitarai, M.Piiparinen, R.Schubart, G.Sletten, S.Tormanen, A.Virtanen In-Beam Spectroscopy at the Proton-Drip Line. First Observation of Excited States in 106Sb and 107Sb NUCLEAR REACTIONS 54Fe(58Ni, X), E=270 MeV; measured γγ(θ), γγ(particle)-coin. 106,107Sb deduced levels, J, π. Shell model comparison.
doi: 10.1016/0370-2693(94)90250-X
1993JO07 Nucl.Phys. A557, 401c (1993) A.Johnson, D.Seweryniak, B.Cederwall, J.Nyberg, A.Atac, J.Blomqvist, J.Cederkall, C.Fahlander, M.Karny, A.Kerek, J.Kownacki, L.-O.Norlin, R.Wyss, E.Adamides, H.Grawe, E.Ideguchi, R.Julin, S.Juutinen, W.Karczmarczyk, S.Mitarai, M.Piiparinen, R.Schubart, G.Sletten, S.Tormanen, A.Virtanen High-Spin Studies Near 100Sn with NORDBALL: New results on 102In, 104In and 108Sb NUCLEAR REACTIONS 54Fe(58Ni, xnyp), E=270 MeV; measured γγ(particle)-coin, γγ(θ), Iγ. 104,102In, 108Sb deduced levels, J, π.
doi: 10.1016/0375-9474(93)90557-E
1993KO10 Acta Phys.Pol. B24, 409 (1993) J.Kownacki, D.Seweryniak, B.Cederwall, J.Nyberg, J.Blomqvist, C.Fahlander, A.Johnson, A.Kerek, L.-O.Norlin, E.Adamides, A.Atac, H.Grawe, E.Ideguchi, R.Julin, S.Juutinen, W.Karczmarczyk, S.Mitarai, M.Piiparinen, R.Schubart, G.Sletten, S.Tormanen, A.Virtanen In-Beam Spectroscopy Close to the Proton Drip Line NUCLEAR REACTIONS 19F(92Mo, xnyp), (96Ru, xnyp), E not given; 58Ni(54Fe, xnyp), E=220 MeV; measured γγ-coin. 102,104In deduced levels, J, π, configuration.
1993SE05 Z.Phys. A345, 243 (1993) D.Seweryniak, B.Cederwall, J.Nyberg, C.Fahlander, A.Johnson, A.Kerek, J.Kownacki, L.-O.Norlin, E.Adamides, A.Atac, J.Blomqvist, H.Grawe, E.Ideguchi, R.Julin, S.Juutinen, W.Karczmarczyk, S.Mitarai, M.Piiparinen, R.Schubart, G.Sletten, S.Tormanen, A.Virtanen In-Beam γ-Ray Spectroscopy of 102In NUCLEAR REACTIONS 54Fe(58Ni, X), E=270 MeV; measured γγ(particle)-coin, γγ(θ), Eγ, Iγ. 102In deduced levels, possible J, π.
doi: 10.1007/BF01293351
1988AR09 Z.Phys. A330, 69 (1988) S.E.Arnell, S.Mattsson, H.A.Roth, M.Rydehell, O.Skeppstedt, J.Nyberg, A.Johnson, A.Kerek, A.Nilsson, L.Westerberg Non-Equilibrium Neutron Emission in α-Induced Reactions on 124Sn NUCLEAR REACTIONS, ICPND 124Sn(α, 2n), (α, 3n), (α, 4n), (α, 5n), E=35-57 MeV; measured σ(E), γ-multiplicities vs E, γn-coin.
1987AR19 Phys.Scr. 36, 214 (1987) S.E.Arnell, S.Mattsson, H.A.Roth, M.Rydehell, O.Skeppstedt, A.Johnson, J.Nyberg, A.Kerek, A.Nilsson Interpretation of the Residue Mass Distribution from 12C + 64Zn Collisions at E(12C) = 118 MeV NUCLEAR REACTIONS 64Zn(12C, X), E=118 MeV; measured (particle)γ-coin, ejectile spectra, γ multiplicities; deduced relative residue yield for X=Co-As.
doi: 10.1088/0031-8949/36/2/004
1986BJ01 Nucl.Phys. A453, 463 (1986) T.Bjornstad, M.J.G.Borge, J.Blomqvist, R.D.Von Dincklage, G.T.Ewan, P.Hoff, B.Jonson, K.Kawade, A.Kerek, O.Klepper, G.Lovhoiden, S.Mattsson, G.Nyman, H.L.Ravn, G.Rudstam, K.Sistemich, O.Tengblad, and the ISOLDE Collaboration The Doubly Closed Shell Nucleus 50132Sn82 RADIOACTIVITY 132In(β-) [from U(p, F)]; measured Eγ, Iγ, I(ce), E(n), T1/2, γγ-, βγ-coin; deduced Qβ. 132Sn deduced level scheme, B(E2), neutron separation energy, ICC. Uranium carbide target. Ge(Li), Si(Li), 3He ion chamber, plastic scintillator telescope detectors. On-line mass separation.
doi: 10.1016/0375-9474(86)90447-1
1986NY01 Phys.Scr. 33, 206 (1986) J.Nyberg, A.Johnson, S.A.Hjorth, A.Kerek, C.G.Linden, S.E.Arnell, S.Mattsson, H.A.Roth, O.Skeppstedt Angular Momentum Transfer in Reactions Induced by 14N Ions on 154Sm NUCLEAR REACTIONS 154Sm(14N, 7np), (14N, 8np), (14N, 9np), (14N, xnd), (14N, xnp), (14N, xnt), E=151 MeV; measured proton spectra, (γ-multiplicity)(charged particle)-coin; deduced reaction mechanism. 158Er deduced <Mγ> vs spin.
doi: 10.1088/0031-8949/33/3/004
1985BL16 Z.Phys. A322, 169 (1985) J.Blomqvist, S.A.Hjorth, A.Johnson, A.Kerek, W.Klamra, A.Nilsson, J.Nyberg, S.E.Arnell, S.Mattsson, H.Roth, O.Skeppstedt In-Beam γ-Ray Spectroscopy on 56Ni NUCLEAR REACTIONS 54Fe(α, 2n), E=35 MeV; measured γγ-coin. 56Ni deduced levels, J, π, configurations, yrast band. Shell model. NUCLEAR STRUCTURE 56Ni; calculated levels. Shell model.
doi: 10.1007/BF01412031
1984KE06 Z.Phys. A317, 169 (1984) A.Kerek, T.Lonnroth, K.Honkanen, E.der Mateosian, P.Thieberger High-Spin Bands in 117,119I and 118Xe NUCLEAR REACTIONS 106Pd(16O, xnyp), E=tandem; 108,110Cd(12C, xnyp), E=cyclotron; measured γ(θ), γγ-coin, σ(Eγ, E). 117,119I, 118Xe deduced levels, J, π, configuration, γ-branching, band structure. Cranking shell model.
doi: 10.1007/BF01421251
1984LO12 ATOMKI Kozlem. 26, 29 (1984) T.Lonnroth, J.Hattula, H.Helppi, S.Juutinen, K.Honkanen, A.Kerek Study of Band Crossings in 130Xe NUCLEAR REACTIONS 130Te(α, 4n), E not given; measured γ-spectra. 130Xe deduced levels, J, π, band structure, γ-multipolarity. Triaxial cranking shell model. In-beam spectroscopy.
1984LO19 Nucl.Phys. A431, 256 (1984) T.Lonnroth, J.Hattula, H.Helppi, S.Juutinen, K.Honkanen, A.Kerek Study of Band Crossings in 130Xe NUCLEAR STRUCTURE 130Xe; calculated levels, band structure; deduced quasiparticle content. Cranked shell model. NUCLEAR REACTIONS 130Te(α, 4n), E=42-51 MeV; measured γγ-coin, Iγ(E), γ(θ). 130Xe deduced levels, J, π, band structure.
doi: 10.1016/0375-9474(84)90174-X
1984NY03 ATOMKI Kozlem. 26, 68 (1984) J.Nyberg, A.Johnson, S.A.Hjorth, A.Kerek, S.E.Arnell, S.Mattsson, H.A.Roth, O.Skeppstedt Angular Momentum Transfer in Partial Fusion Reactions Induced by 14N on 154Sm NUCLEAR REACTIONS 154Sm(14N, 9np), (14N, 8nd), (14N, 7nt), E=154 MeV; measured γ-multiplicity, γp-, γd-, γt-coin; deduced partial fusion angular momentum transfer. Sum rule model.
1983AR14 Phys.Lett. 129B, 23 (1983) S.E.Arnell, S.Mattsson, H.A.Roth, O.Skeppstedt, S.A.Hjorth, A.Johnson, A.Kerek, J.Nyberg, L.Westerberg Charge Particle Production in Peripheral Reactions Induced by 118 MeV 12C Ions on 118Sn NUCLEAR REACTIONS 118Sn(12C, 3nα), (12C, 4nα), (12C, 5nα), (12C, 2n2α), E=118 MeV; measured γ-multiplicities, (particle)γ-coin; deduced fusion reaction mechanism.
doi: 10.1016/0370-2693(83)90720-7
1983BL16 Z.Phys. A314, 199 (1983) J.Blomqvist, A.Kerek, B.Fogelberg The Single Proton Nucleus 133Sb RADIOACTIVITY 133Sn(β-) [from on-line mass separation]; measured Eγ, Iγ, γγ-, βγ-coin; deduced log ft. 133Sb deduced levels, J, π, Iβ, γ-branching, Gamow-Teller transition strength distribution, configurations. Shell model.
doi: 10.1007/BF01879878
1982BJ02 Z.Phys. A306, 95 (1982) T.Bjornstad, J.Blomqvist, G.T.Ewan, B.Jonson, K.Kawade, A.Kerek, S.Mattsson, K.Sistemich Excited States in the Doubly Closed Shell Nucleus 13250Sn82 RADIOACTIVITY 132In [from U(p, X), E=600 MeV]; measured γγ-coin following β-decay; deduced log ft, β-branching, T1/2, Gamow-Teller transition. 132Sn deduced levels, J, π, γ-branching, B(E2), configuration, shell closure.
1982KL10 Nucl.Phys. A391, 184 (1982) W.Klamra, J.Bialkowski, C.J.Herrlander, L.Hildingsson, D.Jerrestam, A.Johnson, A.Kerek, J.Kownacki, A.Kallberg, Th.Lindblad, C.G.Linden, T.Vertse Gamma-Gamma Energy Correlations and Moment of Inertia in Light Xe Isotopes NUCLEAR REACTIONS 114,116Cd(12C, xn), E=118 MeV; measured γγ-coin; deduced energy-energy correlation spectra. 118,120,122Xe deduced moment of inertia.
doi: 10.1016/0375-9474(82)90226-3
1982LI05 Nucl.Phys. A378, 364 (1982) Th.Lindblad, L.Hildingsson, D.Jerrestam, A.Kallberg, A.Johnson, C.J.Herrlander, W.Klamra, A.Kerek, C.G.Linden, J.Kownacki, J.Bialkowski, T.Vertse On the Moment of Inertia in Deformed Ba-Xe Nuclei as Deduced from Gamma-Gamma Energy Correlation Experiments NUCLEAR REACTIONS 114,116,118,120,122Sn(12C, xn), (12C, αxn), E=118 MeV; measured γγ-coin; deduced energy-energy correlation spectra, moment of inertia.
doi: 10.1016/0375-9474(82)90599-1
1981HJ01 Z.Phys. A301, 35 (1981) S.A.Hjorth, A.Johnson, A.Kerek, W.Klamra, Th.Lindblad, S.Messelt, C.Pomar, W.Walus, O.Skeppstedt, Z.Sujkowski, A.Zglinski, L.Carlen, H.Ryde, M.Piiparinen On the Decay of Compound Nuclei following Alpha-Particle and 12C Induced Reactions NUCLEAR REACTIONS 192Os, 122Te, 166Er(α, 3n), (α, 4n), (α, 5n), E=51-55 MeV; 176Yb, 164Dy (12C, 8n), (12C, 6nα), 160Gd, 164Dy(12C, 6n), (12C, 7n), 160Gd(12C, 8n), E=118 MeV; measured Eγ, Iγ, γγ-coin; deduced average multiplicity, average side feeding multiplicity, multiplicity distribution second moment. 180Os, 170,169,168Hf, 166Yb, 192Pt, 122Xe deduced spin distribution, decay mechanism. Statistical model calculations. Ge(Li), NaI(Tl) detectors.
doi: 10.1007/BF01412461
1980AU08 Z.Phys. A296, 319 (1980) G.Auger, G.Albouy, C.Roulet, H.Sergolle, A.Kerek, Th.Lindblad On the Yrast Levels of 106-108Sn NUCLEAR REACTIONS 54Fe(58Ni, xnyp), E=290, 320 MeV; measured Eγ, Iγ, γ(t), γγ-, γ(X-ray)-coin. 108,106Sn deduced yrast levels.
doi: 10.1007/BF01438526
1980BJ01 Phys.Lett. 91B, 35 (1980) T.Bjornstad, L.-E.De Geer, G.T.Ewan, P.G.Hansen, B.Jonson, K.Kawade, A.Kerek, W.-D.Lauppe, H.Lawin, S.Mattsson, K.Sistemich Structure of the Levels in the Doubly Magic Nucleus 132Sn RADIOACTIVITY 132mSn [from 235U(n, F), E=th]; 132In [from U(p, X), E=600 MeV]; measured γγ-coin, Iγ, Eγ, Iβ, ICC. 132Sn deduced levels, J, π, γ-branching, T1/2, multipolarity.
doi: 10.1016/0370-2693(80)90656-5
1980DR07 Nucl.Phys. A341, 98 (1980) C.Droste, D.Chlebowska, J.Dobaczewski, F.Donau, A.Kerek, G.Leander, J.Srebrny, W.Walus Collective Quadrupole Dynamics and the Band Structure of the Nucleus 127Cs NUCLEAR REACTIONS 127I(α, 4n), E=43-51 MeV; measured Eγ, Iγ, γγ-coin, σ(E, Eγ, θ), αγ(t). 127Cs deduced levels, μ, J, π, T1/2, B(λ), δ. Ge(Li) detectors. Core-particle coupling model calculations, soft, rigid, triaxial core.
doi: 10.1016/0375-9474(80)90364-4
1977HA04 Nucl.Phys. A276, 299 (1977) Z.Haratym, J.Kownacki, J.Ludziejewski, Z.Sujkowski, L.-E.De Geer, A.Kerek, H.Ryde High-Spin States and Evidence for Particle-Core Coupling in the N = 83 Isotones: 143Nd, 145Sm and 147Gd NUCLEAR REACTIONS 142Ce, 144Nd(α, 3nγ), 144Sm(α, nγ), E=20-43 MeV; measured σ(Eα, Eγ), σ(Eγ, θ), γγ-coin, αγ-delay. 143Nd, 145Sm, 147Gd deduced levels, J, π, T1/2. Enriched targets. Ge(Li) detectors.
doi: 10.1016/0375-9474(77)90385-2
1976DE11 Nucl.Phys. A259, 399 (1976) L.-E.de Geer, A.Kerek, Z.Haratym, J.Kownacki, J.Ludziejewski High-Spin States in 144Nd Observed in the (α, 2nγ) Reaction NUCLEAR REACTIONS 142Ce(α, 2nγ), E=28-40 MeV; measured σ(Eα, Eγ), σ(Eγ, θ), γγ- coin, αγ-delay. 144Nd deduced levels, J, π, δ-mixing, T1/2 upper limit. Enriched target. Ge(Li) detectors.
doi: 10.1016/0375-9474(76)90075-0
1976LU07 Phys.Scr. 14, 133 (1976) J.Ludziejewski, J.Bialkowski, Z.Haratym, L.-E.De Geer, A.Kerek, J.Kozyczkowski The Life-Time Measurements of Some High-Spin States in the 138,139Ce and 141,142Nd Nuclei NUCLEAR REACTIONS 138Ba(α, 4nγ), (α, 3nγ), 142Ce(α, 4nγ), (α, 5nγ), E=51 MeV; measured Eγ, Iγ(t). 138,139Ce, 141,142Nd deduced levels, T1/2.
doi: 10.1088/0031-8949/14/4/002
1975DE13 Nucl.Phys. A246, 104 (1975) L.-E.de Geer, A.Kerek, Z.Haratym, J.Kownacki, J.Ludziejewski High-Spin States in the Single-Closed-Shell Nucleus 142Nd NUCLEAR REACTIONS 140Ce(α, 2nγ), 142Ce(α, 4nγ), E=28-51 MeV; measured σ(Eα, Eγ), σ(Eγ, θ), γγ-coin. 142Nd deduced levels, J, π, γ-mixing. Enriched targets. Ge(Li) detectors.
doi: 10.1016/0375-9474(75)90566-7
1974BL03 Phys.Scr. 9, 321 (1974) J.Blomqvist, S.Borg, A.Kerek, K.-G.Rensfelt, J.Sztarkier The Half-Life of the 6+ State in 134Te and the Effective 1g7/2 Proton Charge RADIOACTIVITY 134Sb; measured γγ(t). 134Te level deduced T1/2.
doi: 10.1088/0031-8949/9/6/002
1974KE08 Nucl.Phys. A224, 367 (1974) Beta Decay Studies in the Vicinity of 132Sn: Excited States in 130Sb, 130Te and 132Te RADIOACTIVITY 130Sn, 130,132Sb; measured T1/2, Eγ, Iγ, I(ce), Eβ, γγ coin, γγ delay. Deduced Q. 130Sb, 130,132Te deduced levels, J, π, T1/2, log ft, ICC, γ-multipolarity.
doi: 10.1016/0375-9474(74)90694-0
1973KE06 Phys.Lett. 44B, 252 (1973) A.Kerek, G.B.Holm, L.-E.De Geer, S.Borg The First Excited State in the Doubly-Closed-Shell Nucleus 132Sn Populated in the 0.12 s β--Decay of 132In RADIOACTIVITY 132In; measured T1/2, Eβ, Eγ. 132Sn deduced level.
doi: 10.1016/0370-2693(73)90217-7
1973KE07 Nucl.Phys. A206, 245 (1973) The Level Structure of the N = 81 and 82 Nucleides 137,138Ba as Investigated in 136Xe(α, xn) Reactions NUCLEAR REACTIONS 136Xe(α, 2nγ), 136Xe(α, 3nγ), E=20-29 MeV; measured σ(E;Eγ, θ(γ)), Doppler-shift, γγ-coin., αγ-delay. 137,138Ba deduced levels, J, π, T1/2. Enriched target, Ge(Li) detectors.
doi: 10.1016/0375-9474(73)90531-9
1973KE12 Nucl.Phys. A209, 520 (1973) A.Kerek, G.B.Holm, S.Borg, P.Carle Excited States in the Two-Neutron-Hole Nucleus 130Sn Observed in the 0.53 sec β- Decay of 130In RADIOACTIVITY 130In [from 235U fission]; measured T1/2, Eγ, Iγ, Eβ-, βγ-coin; deduced log ft, Q. 130Sn deduced levels, J, π. Isotopically separated source, Ge(Li), anthracene detectors. Ge(Li)-anthracene coin.
doi: 10.1016/0375-9474(73)90843-9
1973KE21 Izv.Akad.Nauk SSSR, Ser.Fiz. 37, 1822 (1973); Bull.Acad.Sci.USSR, Phys.Ser. 37, No.9, 28 (1974) 130Te Levels Excited in the β Decay of 130Sb (T1/2 = 40 min) RADIOACTIVITY 130Sb [from 235U(n, F), isotope separator]; measured Eγ, Iγ, γγ(t). 130Te deduced levels, J, π, T1/2, B(λ).
1973KE22 Izv.Akad.Nauk SSSR, Ser.Fiz. 37, 1824 (1973); Bull.Acad.Sci.USSR, Phys.Ser. 37, No.9, 30 (1974) 137Ba and 138Ba Levels Excited in (α, xn) Reactions on 136Xe NUCLEAR REACTIONS 136Xe(α, xnγ), E=20-29 MeV; measured Eγ, Iγ(θ), γγ-coin, Doppler shift. 137,138Ba deduced levels, J, π, γ-branching, T1/2.
1973KE23 Izv.Akad.Nauk SSSR, Ser.Fiz. 37, 1617 (1973); Bull.Acad.Sci.USSR, Phys.Ser. 37, No.8, 48 (1974) A.Kerek, G.B.Holm, P.Carle, J.McDonald 132Sb States of the Proton-Neutron Hole Type Populated in the Decay of The Doubly Magic Nucleus 132Sn RADIOACTIVITY 132Sn; measured Eβ, βγ(t), deduced log ft. 132Sb deduced levels, T1/2, J, π. On-line mass separator.
1973KE24 Izv.Akad.Nauk SSSR, Ser.Fiz. 37, 1620 (1973); Bull.Acad.Sci.USSR, Phys.Ser. 37, No.8, 51 (1974) β Decay of the 7- Isomer (T1/2 = 1.6 min) and Ground (T1/2 = 3.8 min) States of 130Sn; Excited States of 130Sb RADIOACTIVITY 130Sn; measured γγ(t), Eγ, Iγ, I(ce), deduced ICC. 130Sb deduced T1/2 (level), J, π. On-line mass separator, γ-multipolarities.
1973KE25 Izv.Akad.Nauk SSSR, Ser.Fiz. 37, 1622 (1973); Bull.Acad.Sci.USSR, Phys.Ser. 37, No.8, 53 (1974) A.Kerek, P.Carle, S.Borg, J.McDonald The 132Sb → 132Te Decay with T1/2 = 3.4 and 4.9 min RADIOACTIVITY 132Sb; measured βγ(t). Eγ, Iγ, γγ-coin, T1/2, I(ce). 132Te deduced levels T1/2, J, π. On-line mass separator.
1973KE26 Izv.Akad.Nauk SSSR, Ser.Fiz. 37, 1624 (1973); Bull.Acad.Sci.USSR, Phys.Ser. 37, No.8, 55 (1974) A.Kerek, G.B.Holm, S.Borg, P.Carle Excited States of 130Sn Observed in 130In Decay RADIOACTIVITY 130In; measured T1/2, Eβ, Eγ, Iγ, βγ-coin. 130Sn deduced levels, J, π.
1973KE27 Izv.Akad.Nauk SSSR, Ser.Fiz. 37, 1629 (1973); Bull.Acad.Sci.USSR, Phys.Ser. 37, No.8, 59 (1974) A.Kerek, G.B.Holm, L.E.DeGeer, S.Borg First Excited State of the Doubly Magic Nucleus 132Sn, Populated in the β Decay of 132In (T1/2 = 0.12 sec) RADIOACTIVITY 132In; measured T1/2, Eβ, Eγ. 132Sn deduced levels.
1973MC09 Nucl.Phys. A206, 417 (1973) Transition Probability Measurements in 132Te; The Systematics of E2 Transition Rates in Neutron-Rich Even Te Nuclei RADIOACTIVITY 132Sb [from 235U fission]; measured βγ-, γγ-delay, Eγ, ICC, Iγ. 132Te deduced T1/2, ICC, B(E2). Isotopically separated source. Ge(Li), Si(Li), NaI(Tl), plastic detectors.
doi: 10.1016/0375-9474(73)90544-7
1972KE07 Nucl.Phys. A185, 497 (1972) Levels of 128Te Populated in 8.9 h β- Decay of 128Sb RADIOACTIVITY 128Sb[from 235U fission]; measured Eγ, Iγ, I(ce), γγ-coin; deduced log ft. 128Te deduced levels, J, π, α(K), γ-multipolarity. Isotopically separated source, Ge(Li), Si(Li) detectors.
doi: 10.1016/0375-9474(72)90027-9
1972KE19 Nucl.Phys. A194, 64 (1972) A.Kerek, J.Kownacki, A.Marelius, J.Pihl Evidence for Particle-Core Coupling in the 125Te Nucleus NUCLEAR REACTIONS 124Sn(α, 3nγ), E=26-37 MeV; measured σ(E;Eγ, θ), γγ-coin, αγ-delay. 125Te deduced levels, J, π. Enriched target.
doi: 10.1016/0375-9474(72)91052-4
1972KE20 Nucl.Phys. A195, 159 (1972) A.Kerek, G.B.Holm, P.Carle, J.McDonald Proton-Neutron-Hole States in 132Sb Populated in the β-Decay of the Doubly Closed Shell Nucleus 132Sn RADIOACTIVITY 132Sn[from 235U fission]; measured T1/2, Eγ, Iγ, E(ce), I(ce), Eβ, βγ-coin, γγ-coin, βγ-delay; deduced log ft, Q. 132Sb deduced levels, J, π, T1/2, ICC, B(M1), B(E2), γ-multipolarity. Isotopically separated source;Ge(Li), Si(Li), NaI(Tl), plastic, anthracene detectors, Ge(Li)-Ge(Li) coin.
doi: 10.1016/0375-9474(72)90728-2
1972KE21 Nucl.Phys. A195, 177 (1972) A.Kerek, G.B.Holm, S.Borg, L.-E.de Geer Two-Proton and Proton-Neutron States in the Doubly Closed Shell 132Sn Region RADIOACTIVITY 134Sb[from 235U fission]; measured T1/2, Eγ, Iγ, E(ce), I(ce), Eβ-, γγ-coin, γγ-delay; deduced log ft, Q. 134Te deduced levels, J, π, ICC, γ-multipolarity. Isotopically separated source;Ge(Li), Si(Li), anthracene detectors, Ge(Li)-Ge(Li) coin.
doi: 10.1016/0375-9474(72)90729-4
1972KE27 INR-1406 (1972) Fractional Parentage Coefficients for j = 11/2 Orbital
1972KE28 Nucl.Phys. A198, 466 (1972) Properties of 130Te as Observed in the 40 min β-Decay of 130Sb RADIOACTIVITY 130Sb[from 235U fission]; measured Eγ, Iγ, E(ce), I(ce), Eβ-, γγ-coin, βγ-, γγ-delay; deduced Q. 130Te deduced levels, J, π, ICC, T1/2, B(E2). Isotopically separated source, Ge(Li), Si(Li), NaI(Tl), plastic, anthracene detectors, Ge(Li)-Ge(Li) coin.
doi: 10.1016/0375-9474(72)90702-6
1971KE13 Nucl.Phys. A172, 603 (1971) A.Kerek, A.Luukko, M.Grecescu, J.Sztarkier Two- and Tree-Quasiparticle States in 132Xe and 131Xe NUCLEAR REACTIONS 130Te(α, 2nγ), (α, 3nγ), E= 26-39 MeV; measured σ(E; Eγ, θ(γ)), γγ-coin, αγ-delay. 131,132Xe deduced levels, J, π, T1/2.
doi: 10.1016/0375-9474(71)90047-9
1971KE20 Nucl.Phys. A176, 466 (1971) Two-Quasiparticle States in 122,124,126Te. The Level Systematics in Doubly Even Tellurium Nuclei NUCLEAR REACTIONS 120,122,124Sn(α, 2nγ), E=16-30 MeV; measured σ(E;Eγ, θ), γγ-coin. 122,124,126Te deduced levels, J, π. Enriched targets.
doi: 10.1016/0375-9474(71)90928-6
1970KE01 Phys.Lett. 31B, 10 (1970) A.Kerek, C.J.Herrlander, A.Luukko, M.Grecescu A 9/2- Isomeric State in 123Xe NUCLEAR REACTIONS 122Te(α, 3n), E=43 MeV; measured Eγ, Iγ, αγ-delay. 123Xe deduced isomeric state J, π, T1/2. Ge(Li) detector.
doi: 10.1016/0370-2693(70)90005-5
1970RE01 Nucl.Phys. A141, 130 (1970) I.Rezanka, A.Kerek, A.Luukko, C.J.Herrlander High-Spin States in Odd Xe Nuclei NUCLEAR REACTIONS 124,126,128Te(α, 3nγ), E=28-43 MeV; measured σ(Eγ, θ), σ(E;Eγ), αγ-delay. 125,127,129Xe deduced levels, J, π, γ-mixing. Enriched targets.
doi: 10.1016/0375-9474(70)90299-X
1969BE04 Nucl.Phys. A123, 99 (1969) I.Bergstrom, C.J.Herrlander, A.Kerek, A.Luukko Excited Nuclear Levels in Doubly Even Xe Isotopes Populated in (α, 2n) Reactions NUCLEAR REACTIONS Sn, Te(α, 2nγ), E=28 MeV; measured σ(Eγ, θ). 118,120,122,124,126Te, 124,126,128,130,132Xe deduced levels, J, π. Enriched targets.
doi: 10.1016/0375-9474(69)90892-6
1969LU05 Nucl.Phys. A135, 49 (1969) A.Luukko, A.Kerek, I.Rezanka, C.J.Herrlander Levels in Doubly Even Tellurium Isotopes 114,116,118Te Populated in (α, 2n) Reactions NUCLEAR REACTIONS 112,114,116Sn(α, 2nγ), Eα = 28.9, 33.5, 39.1, 43.0 MeV; measured σ(Eγ, θ). 114,116,118Te deduced levels, J, π. Enriched targets.
doi: 10.1016/0375-9474(69)90146-8
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