NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = H.A.Roth Found 57 matches. 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
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
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
2001RO15 Eur.Phys.J. A 10, 275 (2001) H.A.Roth, S.E.Arnell, D.Foltescu, O.Skeppstedt, J.Blomqvist, G.de Angelis, D.Bazzacco, S.Lunardi Yrast Level Structure of the Neutron-Deficient N = 80 Isotones 146Dy, 147Ho and 148Er up to High-Spin Values NUCLEAR REACTIONS 92Mo(58Ni, 4p), (58Ni, 3p), (58Ni, 2p), E=260 MeV; measured Eγ, Iγ, (charged particle)γ-, (neutron)γ-, γγ-coin. 146Dy, 147Ho, 148Er deduced high-spin levels, J, π, configurations. Comparison with shell model predictions.
doi: 10.1007/s100500170113
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
1999SK04 Nucl.Instrum.Methods Phys.Res. A421, 531 (1999) O.Skeppstedt, H.A.Roth, L.Lindstrom, R.Wadsworth, I.Hibbert, N.Kelsall, D.Jenkins, H.Grawe, M.Gorska, M.Moszynski, Z.Sujkowski, D.Wolski, M.Kapusta, M.Hellstrom, S.Kalogeropoulos, D.Oner, A.Johnson, J.Cederkall, W.Klamra, J.Nyberg, M.Weiszflog, J.Kay, R.Griffiths, J.Garces Narro, C.Pearson, J.Eberth The EUROBALL Neutron Wall - Design and Performance Tests of Neutron Detectors RADIOACTIVITY 246,248Cm(SF); measured neutron spectra; deduced neutron-gamma discrimination features. Neutron wall for Euroball array.
doi: 10.1016/S0168-9002(98)01208-X
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
1998CE03 Eur.Phys.J. A 1, 7 (1998); Erratum Eur.Phys.J. A 2, 111 (1998) J.Cederkall, M.Lipoglavsek, M.Palacz, J.Persson, J.Blomqvist, A.Atac, C.Fahlander, H.Grawe, A.Johnson, W.Klamra, J.Kownacki, A.Likar, L.-O.Norlin, J.Nyberg, R.Schubart, D.Seweryniak, G.de Angelis, P.Bednarczyk, Zs.Dombradi, D.Foltescu, M.Gorska, D.Jerrestam, S.Juutinen, E.Makela, B.M.Nyako, G.Perez, M.de Poli, H.A.Roth, T.Shizuma, O.Skeppstedt, G.Sletten, S.Tormanen Maximum Spin Aligned States in 4798Ag51 NUCLEAR REACTIONS 50Cr(58Ni, np2α), E=261 MeV; measured Eγ, Iγ, γγ-, (evaporated particle)γ-coin. 98Ag deduced levels, possible J, π, configurations.
doi: 10.1007/s100500050024
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
1997CE08 Z.Phys. A359, 227 (1997) J.Cederkall, G.Perez, M.Lipoglavsek, M.Palacz, J.Persson, A.Atac, J.Blomqvist, C.Fahlander, H.Grawe, A.Johnson, 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, B.M.Nyako, M.de Poli, H.A.Roth, T.Shizuma, O.Skeppstedt, G.Sletten, S.Tormanen New Spectroscopic Information on 98Pd NUCLEAR REACTIONS 50Cr(58Ni, 2p2α), E=261 MeV; measured Eγ, Iγ, γγ-coin, γ(θ). 98Pd deduced high-spin levels, J, π, configurations.
doi: 10.1007/s002180050392
1997GO02 Acta Phys.Pol. B28, 303 (1997) M.Gorska, M.Lipoglavsek, H.Grawe, J.Nyberg, A.Atac, A.Axelsson, R.Bark, J.Blomqvist, J.Cederkall, B.Cederwall, G.de Angelis, C.Fahlander, A.Johnson, S.Leoni, A.Likar, M.Matiuzzi, S.Mitarai, L.-O.Norlin, M.Palacz, J.Persson, H.A.Roth, R.Schubart, D.Seweryniak, T.Shizuma, O.Skeppstedt, G.Sletten, W.B.Walters, M.Weiszflog Spectroscopy of the T(z) = 1 Nuclei Close to 100Sn NUCLEAR REACTIONS 46Ti(58Ni, 2nα), E=215 MeV; 50Cr(58Ni, 2nα), E=225 MeV; measured γγ-coin sum spectra, γ(recoil)(t). 98Cd deduced levels, J, π, T1/2, isomers, decay features, B(λ). 102Sn deduced levels, J, π, T1/2, isomers, decay features.
1997GO18 Phys.Rev.Lett. 79, 2415 (1997) M.Gorska, M.Lipoglavsek, H.Grawe, J.Nyberg, A.Atac, A.Axelsson, R.Bark, J.Blomqvist, J.Cederkall, B.Cederwall, G.de Angelis, C.Fahlander, A.Johnson, S.Leoni, A.Likar, M.Matiuzzi, S.Mitarai, L.-O.Norlin, M.Palacz, J.Persson, H.A.Roth, R.Schubart, D.Seweryniak, T.Shizuma, O.Skeppstedt, G.Sletten, W.B.Walters, M.Weiszflog 4898Cd50: The two-proton-hole spectrum in 50100Sn50 NUCLEAR REACTIONS 46Ti(58Ni, 2nα), E=215, 225 MeV; 50Cr(58Ni, 2n2α), E=215, 225 MeV; measured Eγ, Iγ, γγ-, nγ-, αγ-coin, Iγ vs time; deduced 98Cd production. 98Cd deduced levels, J, π, isomeric state T1/2, B(λ), configurations. Other nuclei compared.
doi: 10.1103/PhysRevLett.79.2415
1997GR07 Phys.Rev. C56, R591 (1997) C.J.Gross, D.Rudolph, W.Satula, J.Alexander, C.Baktash, P.J.Coleman-Smith, D.M.Cullen, R.A.Cunningham, J.D.Garrett, W.Gelletly, A.Harder, M.K.Kabadiyski, I.Lazarus, K.P.Lieb, H.A.Roth, D.G.Sarantites, J.A.Sheikh, J.Simpson, O.Skeppstedt, B.J.Varley, D.D.Warner Identification of Excited States in the T(z) = + 1/2 Nucleus 75Rb: The quest for experimental signatures of collective neutron-proton correlations NUCLEAR REACTIONS 40Ca(40Ca, pα), E=128 MeV; measured Eγ, Iγ, γγγ-coin, (recoil)γ-coin. 75Rb deduced high-spin levels, J, π, configurations. CSM analysis, TRS calculations EUROGAM, RMS.
doi: 10.1103/PhysRevC.56.R591
1997GR12 Z.Phys. A358, 185 (1997) H.Grawe, M.Gorska, M.Lipoglavsek, R.Schubart, A.Atac, A.Axelsson, J.Blomqvist, J.Cederkall, G.de Angelis, M.de Poli, C.Fahlander, A.Johnson, K.H.Maier, L.-O.Norlin, J.Nyberg, D.Foltescu, M.Palacz, J.Persson, M.Rejmund, H.A.Roth, T.Shizuma, O.Skeppstedt, G.Sletten, M.Weiszflog, and the OSIRIS/NORDBALL-PEX/EUROBALL Collaboration Present Status and Future Aspects of Nuclear Structure Close to 100Sn NUCLEAR STRUCTURE 94Pd, 98,96Cd, 92Ru; compiled, reviewed level data, analyses. 99,101,100Cd, 104,106Sn, 90Zr, 48Ca, 56,68Ni; compiled, reviewed B(λ) data. 16O, 40Ca, 56Ni, 100Sn; compiled, reviewed Coulomb shift corrected single particle energies.
doi: 10.1007/s002180050302
1997HA08 Phys.Rev. C55, 1680 (1997) A.Harder, A.Jungclaus, M.K.Kabadiyski, D.Kast, K.P.Lieb, D.Rudolph, M.Weiszflog, T.D.Johnson, G.Winter, C.J.Gross, R.A.Cunningham, W.Gelletly, J.Simpson, D.D.Warner, I.G.Bearden, T.Shizuma, G.Sletten, D.Foltescu, H.A.Roth, O.Skeppstedt, B.J.Varley Rotational bands in 77Rb: Spectroscopy near the Z = 38 deformed shell gap NUCLEAR REACTIONS 40Ca(40Ca, 3p), E=128 MeV; measured γγ-, γγγ-, γ(recoil)-coin, DSA. 77Rb deduced high-spin states, J, π, T1/2, rotational bands, γ-multipolarity, B(λ), transition quadrupole moments, deformation, kinematical, dynamical moment of inertia.
doi: 10.1103/PhysRevC.55.1680
1997KA07 Z.Phys. A356, 363 (1997) D.Kast, A.Jungclaus, A.Harder, K.P.Lieb, D.Rudolph, R.Schubart, H.Grawe, D.Foltescu, H.A.Roth, O.Skeppstedt, I.Bearden, T.Shizuma First Identification and Shell Model Structure of 92Rh NUCLEAR REACTIONS 58Ni(40Ca, npα), E=180 MeV; measured γγ-coin. 92Rh deduced high-spin levels, J, π, configuration. Shell model.
doi: 10.1007/s002180050190
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
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
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
1996CE03 Phys.Rev. C53, 1955 (1996); Erratum Phys.Rev. C54, 960 (1996) J.Cederkall, M.Lipoglavsek, M.Palacz, J.Persson, A.Atac, C.Fahlander, H.Grawe, A.Johnson, 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, B.M.Nyako, G.Perez, M.de Poli, H.A.Roth, T.Schizuma, O.Skeppstedt, G.Sletten, S.Tormanen First Evidence for Excited States in 101In NUCLEAR REACTIONS 50Cr(58Ni, 2npα), E=261 MeV; measured γ(particle)-, γγ-coin. 101In deduced levels, possible J, π.
doi: 10.1103/PhysRevC.53.1955
1996HA16 Phys.Lett. 374B, 277 (1996) A.Harder, F.Donau, K.P.Lieb, R.A.Cunningham, W.Gelletly, C.J.Gross, F.Hannachi, M.K.Kabadiyski, H.A.Roth, D.Rudolph, J.Simpson, O.Skeppstedt, B.J.Varley, D.D.Warner A New Type of Band Crossing at Large Deformation NUCLEAR REACTIONS 40Ca(40Ca, 3p), E=128 MeV; measured γγγ-coin, DCO ratios. 77Rb deduced high-spin levels, J, π, moments of inertia, band structure, transition quadrupole moments, deformation features. Nilsson-Strutinsky type calculations.
doi: 10.1016/0370-2693(96)00184-0
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
1996LI50 Z.Phys. A356, 239 (1996) M.Lipoglavsek, M.Gorska, J.Nyberg, A.Atac, A.Axelsson, R.A.Bark, J.Blomqvist, J.Cederkall, B.Cederwall, G.de Angelis, C.Fahlander, H.Grawe, A.Johnson, S.Leoni, A.Likar, M.Matiuzzi, S.Mitarai, L.-O.Norlin, M.Palacz, J.Persson, H.A.Roth, R.Schubart, D.Seweryniak, T.Shizuma, O.Skeppstedt, D.Sohler, G.Sletten, W.B.Walters, M.Weiszflog In-Beam Study of 102Sn NUCLEAR REACTIONS 50Cr(58Ni, 2nα), E=225 MeV; measured γ(particle)-, γγ-coin. 102Sn deduced transitions.
doi: 10.1007/s002180050174
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.
1996RU03 Phys.Rev.Lett. 76, 376 (1996) D.Rudolph, C.J.Gross, J.A.Sheikh, D.D.Warner, I.G.Bearden, R.A.Cunningham, D.Foltescu, W.Gelletly, F.Hannachi, A.Harder, T.D.Johnson, A.Jungclaus, M.K.Kabadiyski, D.Kast, K.P.Lieb, H.A.Roth, T.Shizuma, J.Simpson, O.Skeppstedt, B.J.Varley, M.Weiszflog Identification of T = 0 and T = 1 Bands in the N = Z = 37 Nucleus 74Rb NUCLEAR REACTIONS 40Ca(40Ca, npα), E=128 MeV; measured γγ-, γ(particle)-coin. 74Rb deduced high-spin levels, band structure, T.
doi: 10.1103/PhysRevLett.76.376
1995HA13 Phys.Rev. C51, 2932 (1995) A.Harder, M.K.Kabadiyski, K.P.Lieb, D.Rudolph, C.J.Gross, R.A.Cunningham, F.Hannachi, J.Simpson, D.D.Warner, H.A.Roth, O.Skeppstedt, W.Gelletly, B.J.Varley Rotational Bands in 76Rb NUCLEAR REACTIONS 40Ca(40Ca, n3p), E=128 MeV; measured γγ-, γγγ-, (recoil)γ-coin. 76Rb deduced high-spin levels, J, π, band structure. Cranked shell model.
doi: 10.1103/PhysRevC.51.2932
1995RO06 J.Phys.(London) G21, L1 (1995) H.A.Roth, S.E.Arnell, J.Blomqvist, D.Foltescu, T.Kuroyanagi, S.Mitarai, A.Nilsson, J.Nyberg, O.Skeppstedt First Observation of the Neutron-Deficient Nucleus 93Rh NUCLEAR REACTIONS 58Ni(40Ca, 2n3p), E=187 MeV; measured Eγ, Iγ, (particle)γ-, γγ-coin. 93Rh deduced high-spin levels, J, π. Enriched target, Ge detector array, particle-multiplicity filter.
doi: 10.1088/0954-3899/21/2/001
1995RU03 Nucl.Phys. A587, 181 (1995) D.Rudolph, A.Harder, T.D.Johnson, K.P.Lieb, R.Schubart, D.Foltescu, H.A.Roth, O.Skeppstedt, I.G.Bearden, T.Shizuma, G.Sletten, H.Grawe, J.Persson, D.Seweryniak Multiparticle-Hole States of High-Spin in N < 50, A ≈ 90 Nuclei: 1. The transitional nucleus 4389Tc46 NUCLEAR REACTIONS 58Ni(40Ca, p2α), E=180 MeV; measured γγ-, (particle)γγ-coin. 89Tc deduced high-spin levels, J, π. Shell model.
doi: 10.1016/0375-9474(94)00825-8
1995SU27 J.Phys.Soc.Jpn. 64, 329 (1995) M.Sugawara, S.Mitarai, T.Kuroyanagi, J.Mukai, H.Tomura, T.Morikawa, D.Jerrestam, J.Nyberg, G.Sletten, A.Atac, N.Gjorup, A.Virtanen, S.-E.Arnell, O.Skeppstedt, H.A.Roth, D.Foltescu High Spin States in 79Rb NUCLEAR REACTIONS 58Ni(28Si, 3pα), E=128 MeV; measured γγ-coin. 79Rb deduced high-spin levels, J, π, band structure.
doi: 10.1143/JPSJ.64.329
1994AR33 Phys.Rev. C49, 51 (1994) S.E.Arnell, D.Foltescu, H.A.Roth, O.Skeppstedt, J.Blomqvist, A.Nilsson, T.Kuroyanagi, S.Mitarai, J.Nyberg Yrast Level Structure of the Neutron Deficient N = 49 Isotones 92Tc, 93Ru, 94Rh, and 95Pd up to High Angular Momentum NUCLEAR REACTIONS 58Ni(40Ca, X), E=180 MeV; measured γγ-coin, Eγ, Iγ. 92Tc, 93Ru, 94Rh, 95Pd deduced high-spin levels, J, π, band structure, configuration.
doi: 10.1103/PhysRevC.49.51
1994GR01 Phys.Rev. C49, R580 (1994) C.J.Gross, C.Baktash, D.M.Cullen, R.A.Cunningham, J.D.Garrett, W.Gelletly, F.Hannachi, A.Harder, M.K.Kabadiyski, K.P.Lieb, W.Nazarewicz, H.A.Roth, D.Rudolph, D.G.Sarantites, J.A.Sheikh, J.Simpson, O.Skeppstedt, B.J.Varley, D.D.Warner Identical Bands in 77Sr, 78Sr, and 78Rb: Evidence for a very good spectator orbital NUCLEAR REACTIONS 40Ca(40Ca, xnyp), E=128 MeV; measured Eγ, DCO ratios, γγ-, γγγ-, (recoil)γ-coin. 77,78Sr deduced, levels, J, π, relative spin alignments.
doi: 10.1103/PhysRevC.49.R580
1994MU02 Nucl.Phys. A568, 202 (1994) J.Mukai, A.Odahara, H.Tomura, S.Suematsu, S.Mitarai, T.Kuroyanagi, D.Jerrestam, J.Nyberg, G.Sletten, A.Atac, S.E.Arnell, H.A.Roth, O.Skeppstedt High-Spin States in the Odd-Odd Nucleus 82Y NUCLEAR REACTIONS 58Ni(28Si, n3p), E=100, 102, 128 MeV; measured Eγ, Iγ, Iγ(θ), (particle)γ-, γγ-coin. 82Y deduced levels, J, π. Enriched target, Ge detector array, particle-multiplicity filter.
doi: 10.1016/0375-9474(94)90010-8
1994RO08 Phys.Rev. C50, 1330 (1994) H.A.Roth, S.E.Arnell, D.Foltescu, O.Skeppstedt, J.Blomqvist, A.Nilsson, T.Kuroyanagi, S.Mitarai, J.Nyberg Gaps in the Yrast Level Structure of the N = 50 Isotones 93Tc, 94Ru, and 95Rh at High Angular Momentum NUCLEAR REACTIONS 58Ni(40Ca, X), E=180 MeV; measured Eγ, Iγ, γ(θ). 93Tc, 94Ru, 95Rh deduced high-spin levels, J, π, T1/2. Multidetector array NORDBALL including particle selection. Shell model comparison.
doi: 10.1103/PhysRevC.50.1330
1993AR01 Phys.Scr. 47, 142 (1993) S.E.Arnell, D.Foltescu, H.A.Roth, O.Skeppstedt, A.Nilsson, S.Mitarai, J.Nyberg High-Spin States of the Neutron Deficient Isotope 91Tc NUCLEAR REACTIONS 58Ni(40Ca, 3pα), E=180, 187 MeV; measured Eγ, Iγ, γγ-coin, γ anisotropy. 91Tc deduced levels, J, π. Shell model comparison.
doi: 10.1088/0031-8949/47/2/003
1993AR02 Phys.Scr. 47, 355 (1993) S.E.Arnell, D.Foltescu, H.A.Roth, O.Skeppstedt, A.Nilsson, S.Mitarai, J.Nyberg First Information About the Level Structure of 91Ru NUCLEAR REACTIONS 58Ni(40Ca, n2pα), E=187 MeV; measured γγ-coin, Iγ(θ), Eγ, Iγ. 91Ru deduced levels, J, π, configuration. Shell model.
doi: 10.1088/0031-8949/47/3/005
1993AR07 Nucl.Phys. A557, 477c (1993) S.E.Arnell, D.Foltescu, T.Kuroyanagi, S.Mitarai, A.Nilsson, H.A.Roth, O.Skeppstedt In-Beam Gamma Ray Study of Neutron Deficient Nuclei with A ≈ 90 NUCLEAR REACTIONS 58Ni(40Ca, X), E=147-187 MeV; measured γ spectra. 91Tc, 92Ru deduced levels. Shell model. In-beam study. NUCLEAR STRUCTURE 90Mo, 91Tc, 92Ru; calculated levels. Shell model.
doi: 10.1016/0375-9474(93)90564-E
1993AR08 Z.Phys. A346, 111 (1993) S.E.Arnell, D.Foltescu, H.A.Roth, O.Skeppstedt, A.Nilsson, S.Mitarai, J.Nyberg The Level Structure of 92Ru Up to High Spin Values NUCLEAR REACTIONS 58Ni(40Ca, 2pα), E=147, 187 MeV; measured Eγ, Iγ, γγ-coin, γ(θ). 92Ru deduced levels, J, π. Shell model.
doi: 10.1007/BF01294626
1993MI07 Z.Phys. A344, 405 (1993) S.Mitarai, T.Kuroyanagi, A.Odahara, J.Mukai, H.Tomura, S.Suematsu, D.Jerrestam, J.Nyberg, G.Sletten, A.Atac, N.Gjorup, J.Jongman, S.E.Arnell, H.A.Roth, O.Skeppstedt A Rotational Band in 82Zr NUCLEAR REACTIONS 58Ni(28Si, 2n2p), E=128 MeV; measured γγ-coin. 82Zr deduced levels, J, π, band structure.
doi: 10.1007/BF01283195
1993MI11 Nucl.Phys. A557, 381c (1993) S.Mitarai, T.Kuroyanagi, A.Odahara, J.Mukai, H.Tomura, S.Suematsu, T.Morikawa, D.Jerrestam, J.Nyberg, G.Sletten, A.Atac, M.Piiparinen, S.E.Arnell, D.Foltescu, H.A.Roth, O.Skeppstedt Band Structures of Nuclei Around N, Z = 40 Selected by Charged Particle Detection NUCLEAR REACTIONS 58Ni(28Si, 4p), E=128 MeV; 58Ni(32S, 4p), E=125 MeV; measured relative yield with respect to 1p, 2p, 3p exit channels. 58Ni(28Si, pα), E=100 MeV; 58Ni(32S, p2α), (32S, pα), E=120, 125 MeV; measured γγ-, pα-coin. 85Nb, 81Y deduced levels, J, π, yrast band dynamic moment of inertia. 58Ni(28Si, 2n2p), E=128 MeV; measured γ(particle)-coin. 82Zr deduced levels, J, π. 58Ni(32S, 2n2p), E=125 MeV; measured γγ-coin. 86Mo deduced possible yrast level transitions.
doi: 10.1016/0375-9474(93)90555-C
1992AR15 Phys.Scr. 46, 389 (1992) S.E.Arnell, D.Foltescu, H.A.Roth, O.Skeppstedt, A.Nilsson, S.Mitarai, J.Nyberg Nuclear Structure of the Neutron Deficient Isotope 90Mo NUCLEAR REACTIONS 58Ni(40Ca, 4pα), E=180, 187 MeV; measured γγ-coin, γ-anisotropy, Iγ, Eγ. 90Mo deduced levels, possible J, π.
doi: 10.1088/0031-8949/46/5/002
1992DE30 Z.Phys. A343, 121 (1992) G.de Angelis, D.Bazzacco, S.Lunardi, M.A.Cardona, M.De Poli, Y.X.Guo, D.Ackermann, S.E.Arnell, A.Atac, S.Beghini, L.Corradi, A.D'Onofrio, D.Foltescu, E.Ideguchi, A.Nilsson, S.Mitarai, G.Montagnoli, H.Moreno, D.R.Napoli, V.Roca, H.A.Roth, F.Scarlassara, G.F.Segato, C.Signorini, O.Skeppstedt, P.Spolaore, A.M.Stefanini, F.Terrasi Identification of the N = 79 147Er Nucleus Through γ-Recoil Coincidences NUCLEAR REACTIONS 92Mo(58Ni, n2p), E=260 MeV; measured γ(recoil)-, γγ-coin. 147Er deduced levels, J, π, band structure.
doi: 10.1007/BF01291605
1991AR08 Nucl.Instrum.Methods Phys.Res. A300, 303 (1991) S.E.Arnell, H.A.Roth, O.Skeppstedt, J.Bialkowski, M.Moszynski, D.Wolski, J.Nyberg A 2π Neutron and γ-Ray Multiplicity Filter for the NORDBALL Detection System NUCLEAR REACTIONS 27Al(16O, X), E=63 MeV; measured Eγ, Iγ, neutron spectra. 58Ni(28Si, X), E=110 MeV; measured Eγ, Iγ. 2π neutron, γ-ray multiplicity filter.
doi: 10.1016/0168-9002(91)90441-R
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
1986AR20 Phys.Scr. 34, 484 (1986) S.E.Arnell, S.Mattsson, H.A.Roth, M.Rydehell, O.Skeppstedt, A.Johnson, J.Nyberg, L.Westerberg Preequilibrium Reactions with 118 MeV 12C on 118Sn NUCLEAR REACTIONS 118Sn(12C, Xγ), E=118 MeV; measured γ(particle)-coin, fragment spectra, σ(θ), X=4He, Li, 7,9,10Be, B, γ-multiplicities. 121,122,123Xe, 120Te deduced γ-multiplicity yrast transition dependence. Hyperpure Ge, NaI detectors. Sum rule calculations.
doi: 10.1088/0031-8949/34/6A/003
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
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
1983AR19 Phys.Scr. T5, 199 (1983) S.E.Arnell, S.Mattsson, H.A.Roth, O.Skeppstedt, S.A.Hjorth, A.Johnson, Th.Lindblad, J.Nyberg, L.Westerberg Incomplete-Fusion Reactions in the 12C + 118Sn System at E(12C) = 118 MeV NUCLEAR REACTIONS 118Sn(12C, X), E=118 MeV; measured σ(fragment E), relative fragment production σ for X=He, Li, Be, B, γ(fragment)-coin; deduced reaction mechanism. Wilczynski sum rule model.
doi: 10.1088/0031-8949/1983/T5/040
1980RO13 Nucl.Phys. A343, 148 (1980) H.A.Roth, J.E.Christiansson, J.Dubois Cross Sections for 18O+9Be Induced Reactions at Sub-Coulomb Energies NUCLEAR REACTIONS 9Be(18O, X), E(cm)=1.8-6.7 MeV; measured Eγ, Iγ, nγ-coin; deduced production σ for 19O, 21,22,23Ne, 24,25Na, 25Mg, total fusion σ(E), neutron-transfer σ(E). Ge(Li) detector.
doi: 10.1016/0375-9474(80)90646-6
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