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2022CS01      Eur.Phys.J. A 58, 14 (2022)

L.Csige, M.Csatlos, T.Faestermann, D.Habs, M.Hunyadi, A.J.Krasznahorkay, P.G.Thirolf, T.G.Tornyi, H.-F.Wirth

Fission resonances observed in the 237Np(d, pf) reaction and the fission barrier topology of 238Np

NUCLEAR REACTIONS 237Np(d, pF), E=12 MeV; measured reaction products. 238Np; deduced fission resonances. Comparison with TALYS-1.95 calculations, RIPL-3 values. The Tandem accelerator of the Maier-Leibnitz Laboratory in Garching.

doi: 10.1140/epja/s10050-022-00668-z
Citations: PlumX Metrics


2015CS01      Acta Phys.Pol. B46, 559 (2015)

L.Csige, M.Csatlos, T.Faestermann, J.Gulyas, D.Habs, A.Krasznahorkay, P.G.Thirolf, T.G.Tornyi, H.-F.Wirth

Transmission Resonance Spectroscopy of the Doubly Odd 238Np in (d, pf) Reaction

NUCLEAR REACTIONS 237Np(d, p), (d, F), E=12 MeV; measured reaction products; deduced fission probability.

doi: 10.5506/APhysPolB.46.559
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2014IL01      Phys.Rev. C 89, 014313 (2014)

S.Ilieva, M.Thurauf, Th.Kroll, R.Krucken, T.Behrens, V.Bildstein, A.Blazhev, S.Bonig, P.A.Butler, J.Cederkall, T.Davinson, P.Delahaye, J.Diriken, A.Ekstrom, F.Finke, L.M.Fraile, S.Franchoo, Ch.Fransen, G.Georgiev, R.Gernhauser, D.Habs, H.Hess, A.M.Hurst, M.Huyse, O.Ivanov, J.Iwanicki, P.Kent, O.Kester, U.Koster, R.Lutter, M.Mahgoub, D.Martin, P.Mayet, P.Maierbeck, T.Morgan, O.Niedermeier, M.Pantea, P.Reiter, T.R.Rodriguez, Th.Rolke, H.Scheit, A.Scherillo, D.Schwalm, M.Seidlitz, T.Sieber, G.S.Simpson, I.Stefanescu, S.Thiel, P.G.Thirolf, J.Van de Walle, P.Van Duppen, D.Voulot, N.Warr, W.Weinzierl, D.Weisshaar, F.Wenander, A.Wiens, S.Winkler

Coulomb excitation of neutron-rich Cd isotopes

NUCLEAR REACTIONS 108Pd(122Cd, 122Cd'), 64Zn, 104Pd(124Cd, 124Cd'), 64Zn(126Cd, 126Cd'), E=2.85 MeV/nucleon, [secondary 122,124,126Cd beams from 238U(p, X), E=1.2 GeV primary reaction]; measured Eγ, Iγ, particle spectra, γγ-, (particle)γ-coin, γ-ray yields, γ(θ), σ(θ), half-life of first 2+ state of 126Cd by DSAM using REXTRAP and EBIS setup, Miniball array for γ rays and DSSDs for particle detection at REX-ISOLDE-CERN facility. 122,124,126Cd; deduced levels, Coulomb-excitation σ, transition and diagonal matrix elements, static quadrupole moments, and B(E2) for first 2+ states. Comparison with shell model and beyond mean field calculations. Discussed onset of collectivity in the vicinity of Z=50 and N=82 shell closures. Systematics of experimental and theoretical values of B(E2) for first 2+ states in A=116-130 even Cd isotopes.

doi: 10.1103/PhysRevC.89.014313
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Data from this article have been entered in the XUNDL database. For more information, click here.


2013CS01      Acta Phys.Pol. B44, 643 (2013)

L.Csige, D.M.Filipescu, J.Gulyas, M.Gunther, D.Habs, H.J.Karwowski, A.Krasznahorkay, G.C.Rich, P.G.Thirolf

Photofission of 238U Induced by a Quasi-monochromatic, Compton Backscattered γ Beam

NUCLEAR REACTIONS 238U(γ, F), E=4.7-6 MeV; measured fission products; deduced σ. Comparison with EMPIRE 3.1 calculations, available data.

doi: 10.5506/APhysPolB.44.643
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetL0179.


2013CS03      Phys.Rev. C 87, 044321 (2013)

L.Csige, D.M.Filipescu, T.Glodariu, J.Gulyas, M.M.Gunther, D.Habs, H.J.Karwowski, A.Krasznahorkay, G.C.Rich, M.Sin, L.Stroe, O.Tesileanu, P.G.Thirolf

Exploring the multihumped fission barrier of 238U via sub-barrier photofission

NUCLEAR REACTIONS 238U(γ, F), E=4.7-6.0 MeV; measured Eγ, Iγ, photofission σ(E) at the HIγS facility. 238U; deduced triple-humped fission barrier parameters using EMPIRE-3.1 computer code calculations. Comparison with previous experimental studies.

doi: 10.1103/PhysRevC.87.044321
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetL0179.


2012BA40      Phys.Rev. C 86, 034310 (2012)

C.Bauer, T.Behrens, V.Bildstein, A.Blazhev, B.Bruyneel, J.Butterworth, E.Clement, L.Coquard, J.L.Egido, A.Ekstrom, C.R.Fitzpatrick, C.Fransen, R.Gernhauser, D.Habs, H.Hess, J.Leske, T.Kroll, R.Krucken, R.Lutter, P.Marley, T.Moller, T.Otsuka, N.Patronis, A.Petts, N.Pietralla, T.R.Rodriguez, N.Shimizu, C.Stahl, I.Stefanescu, T.Stora, P.G.Thirolf, D.Voulot, J.van de Walle, N.Warr, F.Wenander, A.Wiens

Prolate shape of 140Ba from a first combined Doppler-shift and Coulomb-excitation measurement at the REX-ISOLDE facility

NUCLEAR REACTIONS 96Mo(140Ba, 140Ba'), [140Ba secondary beam from U(p, X), E=1.4 GeV primary beam], E=392 MeV; measured Eγ, Iγ, (particle)γ-coin, yields in different angular ranges, differential σ(θ), half-life of first 2+ state by DSAM using REX-ISOLDE and MINIBALL setup at ISOLDE-CERN. 140Ba; deduced level, E2 matrix element, B(E2), and static quadrupole moment of first 2+ state. Z=56, A=130=146; systematics of energies and B(E2) of first 2+ states. Comparison with Monte Carlo shell-model approach and beyond-mean-field calculations. Gogny energy density functionals and distribution of probability contours in the triaxial (β, γ) plane for 0+, 2+ and 4+ states first two bands.

NUCLEAR MOMENTS 140Ba; measured static quadrupole moment of first 2+ state by reorientation analysis of Coulomb-excitation yields.

doi: 10.1103/PhysRevC.86.034310
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2012CS01      Acta Phys.Pol. B43, 291 (2012)

L.Csige, M.Csatlos, T.Faestermann, J.Gulyas, D.Habs, R.Hertenberger, M.Hunyadi, A.Krasznahorkay, H.J.Maier, P.G.Thirolf, H.F.Wirth

High Resolution Spectroscopy in the Third Minimum of 232Pa

NUCLEAR REACTIONS 231Pa(d, pF)232Pa, E=12 MeV; measured reaction products. 232Pa; deduced fission probability and barrier parameters. Comparison with other experimental data.

doi: 10.5506/APhysPolB.43.291
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2012CS02      Phys.Rev. C 85, 054306 (2012)

L.Csige, M.Csatlos, T.Faestermann, J.Gulyas, D.Habs, R.Hertenberger, M.Hunyadi, A.Krasznahorkay, H.J.Maier, P.G.Thirolf, H.-F.Wirth

Transmission resonance spectroscopy in the third minimum of 232Pa

NUCLEAR REACTIONS 231Pa(d, pF), E=12 MeV; measured E(p), I(p), fission probability using the Garching Q3D spectrograph. 232Pa; deduced transmission fission resonances, J, π, level spacing of J=4 states, superdeformed and hyperdeformed rotational bands, inner and outer fission barrier heights, triple-humped fission barrier, excitation energy of the ground state of the third minimum. Evidence for hyperdeformation. Comparison of experimental fission barrier parameters with TALYS 1.2 nuclear reaction code calculations, and with previous studies.

doi: 10.1103/PhysRevC.85.054306
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2012TH02      Acta Phys.Pol. B43, 227 (2012)

P.G.Thirolf, L.Csige, M.Gunther, D.Habs, A.Krasznahorkay

Perspectives for Spectroscopy of Actinides with Highly Brilliant γ Beams

doi: 10.5506/APhysPolB.43.227
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2011CS04      J.Phys.:Conf.Ser. 312, 092022 (2011)

L.Csige, M.Csatlos, T.Faestermann, Z.Gacsi, J.Gulyas, D.Habs, R.Hertenberger, A.Krasznahorkay, R.Lutter, H.J.Maier, P.G.Thirolf, T.Tornyi, H.-F.Wirth

Hyperdeformed fission resonances and transition states observed in 232U

NUCLEAR REACTIONS 231Pa(3He, df), E=38.1 MeV; measured E(d), I(d, θ=350) using Q3D magnetic spectrograph and position-sensitive light-ion detector, fission fragments, (fragment)d-coin; deduced sharp fission hyperdeformed resonances, fission probability, rotational bands, fission fragments angular distribution for rotational bands; calculated fission fragments angular distribution for rotational bands.

doi: 10.1088/1742-6596/312/9/092022
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2011TH02      Acta Phys.Pol. B42, 843 (2011)

P.G.Thirolf, D.Habs, M.Gross, K.Allinger, J.Bin, A.Henig, D.Kiefer, W.Ma, J.Schreiber

Laser Particle Acceleration: Status and Perspectives for Nuclear Physics

doi: 10.5506/APhysPolB.42.843
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2009CS01      Phys.Rev. C 80, 011301 (2009)

L.Csige, M.Csatlos, T.Faestermann, Z.Gacsi, J.Gulyas, D.Habs, R.Hertenberger, A.Krasznahorkay, R.Lutter, H.J.Maier, P.G.Thirolf, H.-F.Wirth

Hyperdeformed sub-barrier fission resonances observed in 232U

NUCLEAR REACTIONS 231Pa(3He, dF), E=38.1 MeV; measured Ed, (fission)(deuteron)-coin, angular distribution of fission fragments and fission probability. 232U; deduced barrier parameters, hyperdeformed fission resonances, third potential well and rotational band parameters.

doi: 10.1103/PhysRevC.80.011301
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1717. Data from this article have been entered in the XUNDL database. For more information, click here.


2009SC11      Phys.Rev.Lett. 103, 012501 (2009)

W.Schwerdtfeger, P.G.Thirolf, K.Wimmer, D.Habs, H.Mach, T.R.Rodriguez, V.Bildstein, J.L.Egido, L.M.Fraile, R.Gernhauser, R.Hertenberger, K.Heyde, P.Hoff, H.Hubel, U.Koster, T.Kroll, R.Krucken, R.Lutter, T.Morgan, P.Ring

Shape Coexistence Near Neutron Number N = 20: First Identification of the E0 Decay from the Deformed First Excited Jπ = 0+ State in 30Mg

RADIOACTIVITY 30Na(β-); measured Eγ, Iγ; deduced J, π, monopole strength, partial E0 lifetime. Comparison with beyond mean field calculations.

doi: 10.1103/PhysRevLett.103.012501
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Data from this article have been entered in the XUNDL database. For more information, click here.


2009SZ05      Eur.Phys.J. A 42, 319 (2009)

J.Szerypo, V.S.Kolhinen, M.Bussmann, E.Gartzke, D.Habs, J.Neumayr, U.Schramm, C.Schurmann, M.Sewtz, P.G.Thirolf

Status of the Penning trap project in Munich

doi: 10.1140/epja/i2009-10788-3
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2009VA01      Phys.Rev. C 79, 014309 (2009)

J.Van de Walle, F.Aksouh, T.Behrens, V.Bildstein, A.Blazhev, J.Cederkall, E.Clement, T.E.Cocolios, T.Davinson, P.Delahaye, J.Eberth, A.Ekstrom, D.V.Fedorov, V.N.Fedosseev, L.M.Fraile, S.Franchoo, R.Gernhauser, G.Georgiev, D.Habs, K.Heyde, G.Huber, M.Huyse, F.Ibrahim, O.Ivanov, J.Iwanicki, J.Jolie, O.Kester, U.Koster, T.Kroll, R.Krucken, M.Lauer, A.F.Lisetskiy, R.Lutter, B.A.Marsh, P.Mayet, O.Niedermaier, M.Pantea, R.Raabe, P.Reiter, M.Sawicka, H.Scheit, G.Schrieder, D.Schwalm, M.D.Seliverstov, T.Sieber, G.Sletten, N.Smirnova, M.Stanoiu, I.Stefanescu, J.-C.Thomas, J.J.Valiente-Dobon, P.Van Duppen, D.Verney, D.Voulot, N.Warr, D.Weisshaar, F.Wenander, B.H.Wolf, M.Zielinska

Low-energy Coulomb excitation of neutron-rich zinc isotopes

NUCLEAR REACTIONS 120Sn(74Zn, 74Zn'), E=2.87 MeV/nucleon; 120Sn(76Zn, 76Zn'), E=2.83 MeV/nucleon; 108Pd(78ZN, 78Zn'), E=2.87 MeV/nucleon; 108Pd(80Zn, 80Zn'), E=2.79 MeV/nucleon; measured Eγ, Iγ, charged particle spectra, (particle)-γ coin, measured half-lives of first 2+ state, B(E2). 74,76,78,80Zn, 80Ga, 80Rb, 108Pd, 120Sn; deduced levels. Fe, Ni, Zn, Ge, Se; systematics of B(E2) values. Comparison with shell-model calculations.

doi: 10.1103/PhysRevC.79.014309
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Data from this article have been entered in the XUNDL database. For more information, click here.


2008EK01      Phys.Rev.Lett. 101, 012502 (2008)

A.Ekstrom, J.Cederkall, C.Fahlander, M.Hjorth-Jensen, F.Ames, P.A.Butler, T.Davinson, J.Eberth, F.Fincke, A.Gorgen, M.Gorska, D.Habs, A.M.Hurst, M.Huyse, O.Ivanov, J.Iwanicki, O.Kester, U.Koster, B.A.Marsh, J.Mierzejewski, P.Reiter, H.Scheit, D.Schwalm, S.Siem, G.Sletten, I.Stefanescu, G.M.Tveten, J.Van de Walle, P.Van Duppen, D.Voulot, N.Warr, D.Weisshaar, F.Wenander, M.Zielinska

0+gs → 2+1 Transition Strengths in 106Sn and 108Sn

NUCLEAR REACTIONS 58Ni(106Sn, X), E=2.83 MeV/nucleon; 58Ni(108Sn, X), E=2.82 MeV/nucleon; measured Eγ, Iγ following coulomb excitations.106,108Sn; deduced B(E2).

doi: 10.1103/PhysRevLett.101.012502
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Data from this article have been entered in the XUNDL database. For more information, click here.


2008RA03      Phys.Rev.Lett. 100, 012501 (2008)

C.Rauth, D.Ackermann, K.Blaum, M.Block, A.Chaudhuri, Z.Di, S.Eliseev, R.Ferrer, D.Habs, F.Herfurth, F.P.Hessberger, S.Hofmann, H.-J.Kluge, G.Maero, A.Martin, G.Marx, M.Mukherjee, J.B.Neumayr, W.R.Plass, S.Rahaman, D.Rodriguez, C.Scheidenberger, L.Schweikhard, P.G.Thirolf, G.Vorobjev, C.Weber

First Penning Trap Mass Measurements beyond the Proton Drip Line

ATOMIC MASSES 144,145,146,147Ho, 147,148Tm; measured masses using the SHIPTRAP penning trap mass spectrometer.

doi: 10.1103/PhysRevLett.100.012501
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2007BL16      Eur.Phys.J. D 45, 39 (2007)

M.Block, D.Ackermann, K.Blaum, A.Chaudhuri, Z.Di, S.Eliseev, R.Ferrer, D.Habs, F.Herfurth, F.P.Hessberger, S.Hofmann, H.-J.Kluge, G.Maero, A.Martin, G.Marx, M.Mazzocco, M.Mukherjee, J.B.Neumayr, W.R.Plass, W.Quint, S.Rahaman, C.Rauth, D.Rodriguez, C.Scheidenberger, L.Schweikhard, P.G.Thirolf, G.Vorobjev, C.Weber

Towards direct mass measurements of nobelium at SHIPTRAP

doi: 10.1140/epjd/e2007-00189-2
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2007CE02      Phys.Rev.Lett. 98, 172501 (2007)

J.Cederkall, A.Ekstrom, C.Fahlander, A.M.Hurst, M.Hjorth-Jensen, F.Ames, A.Banu, P.A.Butler, T.Davinson, U.Datta Pramanik, J.Eberth, S.Franchoo, G.Georgiev, M.Gorska, D.Habs, M.Huyse, O.Ivanov, J.Iwanicki, O.Kester, U.Koster, B.A.Marsh, O.Niedermaier, T.Nilsson, P.Reiter, H.Scheit, D.Schwalm, T.Sieber, G.Sletten, I.Stefanescu, J.Van de Walle, P.Van Duppen, N.Warr, D.Weisshaar, F.Wenander

Sub-Barrier Coulomb Excitation of 110Sn and Its Implications for the 100Sn Shell Closure

NUCLEAR REACTIONS 58Ni(110Sn, 110Sn'), E=2.82 MeV/nucleon; measured Eγ, Iγ, (particle)γ-coin following Coulomb excitation. 110Sn deduced B(E2) of the first excited 2+ state. MINIBALL array at REX-ISOLDE.

doi: 10.1103/PhysRevLett.98.172501
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Data from this article have been entered in the XUNDL database. For more information, click here.


2007CS02      Acta Phys.Pol. B38, 1503 (2007)

L.Csige, M.Csatlos, T.Faestermann, Z.Gacsi, J.Gulyas, D.Habs, R.Hertenberger, M.Hunyadi, A.Krasznahorkay, R.Lutter, H.J.Maier, P.G.Thirolf, H.-F.Wirth

New Excited States and Fission Resonances in the Actinide Region

NUCLEAR REACTIONS 231Pa(d, pf), E=12 MeV; 231Pa(3He, df), E=38.1 MeV; measured Ep, Ed, fission fragment energies. Deduced prompt fission probabilities as a function of excitation energies.


2007KR19      Eur.Phys.J. Special Topics 150, 127 (2007)

Th.Kroll, T.Behrens, R.Krucken, V.Bildstein, R.Gernhauser, P.Maierbeck, I.Stefanescu, O.Ivanov, J.Van de Walle, N.Warr, P.A.Butler, J.Cederkall, P.Delahaye, L.M.Fraile, G.Georgiev, U.Koster, T.Sieber, D.Voulot, F.Wenander, P.E.Kent, A.Ekstrom, K.-H.Speidel, J.Leske, S.Schielke, D.Habs, R.Lutter, P.Thirolf, H.Scheit, T.Davinson, and the REX-ISOLDE and MINIBALL Collaboration

Coulomb excitation of neutron-rich 138, 140, 142Xe at REX-ISOLDE

NUCLEAR REACTIONS 96Mo(138Xe, 138Xe'), (140Xe, 140Xe'), (142Xe, 142Xe'), E=2.84 MeV/nucleon; measured Eγ, Iγ. 138,140,142Xe; deduced B(E2).

doi: 10.1140/epjst/e2007-00284-6
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Data from this article have been entered in the XUNDL database. For more information, click here.


2007MA92      Eur.Phys.J. A 34, 341 (2007)

A.Martin, D.Ackermann, G.Audi, K.Blaum, M.Block, A.Chaudhuri, Z.Di, S.Eliseev, R.Ferrer, D.Habs, F.Herfurth, F.P.Hessberger, S.Hofmann, H.-J.Kluge, M.Mazzocco, M.Mukherjee, J.B.Neumayr, Yu.Novikov, W.Plass, S.Rahaman, C.Rauth, D.Rodriguez, C.Scheidenberger, L.Schweikhard, P.G.Thirolf, G.Vorobjev, C.Weber

Mass measurements of neutron-deficient radionuclides near the end-point of the rp-process with SHIPTRAP

ATOMIC MASSES 99,101,103Ag, 101,102,103,104Cd, 102,103,104,105In, 105,106Sn, 107,109,111Sb, 109,110,111,112Te, 111,112,113I, 113Xe; measured and evaluated masses using the SHIPTRAP Penning trap mass spectrometer. 104Sn, 105Sb, 108Te, 109I, 112Xe, 113Cs; evaluated masses.

NUCLEAR STRUCTURE 102,103,104,105In, 104,105,106Sn, 105,106,107Sb, 109I; deduced proton separation energies from mass measurements using the SHIPTRAP facility.

doi: 10.1140/epja/i2007-10520-5
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2007ST03      Phys.Rev.Lett. 98, 122701 (2007)

I.Stefanescu, G.Georgiev, F.Ames, J.Aysto, D.L.Balabanski, G.Bollen, P.A.Butler, J.Cederkall, N.Champault, T.Davinson, A.De Maesschalck, P.Delahaye, J.Eberth, D.Fedorov, V.N.Fedosseev, L.M.Fraile, S.Franchoo, K.Gladnishki, D.Habs, K.Heyde, M.Huyse, O.Ivanov, J.Iwanicki, J.Jolie, B.Jonson, Th.Kroll, R.Krucken, O.Kester, U.Koster, A.Lagoyannis, L.Liljeby, G.Lo Bianco, B.A.Marsh, O.Niedermaier, T.Nilsson, M.Oinonen, G.Pascovici, P.Reiter, A.Saltarelli, H.Scheit, D.Schwalm, T.Sieber, N.Smirnova, J.Van De Walle, P.Van Duppen, S.Zemlyanoi, N.Warr, D.Weisshaar, F.Wenander

Coulomb Excitation of 68, 70Cu: First Use of Postaccelerated Isomeric Beams

NUCLEAR REACTIONS 120Sn(68Cu, 68Cu'), (70Cu, 70Cu'), E=2.83 MeV/nucleon; measured Eγ, Iγ, (particle)γ-coin following projectile Coulomb excitation. 68,70Cu deduced transitions B(E2). Isomeric beams, comparison with large-scale shell model calculations.

doi: 10.1103/PhysRevLett.98.122701
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Data from this article have been entered in the XUNDL database. For more information, click here.


2007VA20      Phys.Rev.Lett. 99, 142501 (2007)

J.Van de Walle, F.Aksouh, F.Ames, T.Behrens, V.Bildstein, A.Blazhev, J.Cederkall, E.Clement, T.E.Cocolios, T.Davinson, P.Delahaye, J.Eberth, A.Ekstrom, D.V.Fedorov, V.N.Fedosseev, L.M.Fraile, S.Franchoo, R.Gernhauser, G.Georgiev, D.Habs, K.Heyde, G.Huber, M.Huyse, F.Ibrahim, O.Ivanov, J.Iwanicki, J.Jolie, O.Kester, U.Koster, T.Kroll, R.Krucken, M.Lauer, A.F.Lisetskiy, R.Lutter, B.A.Marsh, P.Mayet, O.Niedermaier, T.Nilsson, M.Pantea, O.Perru, R.Raabe, P.Reiter, M.Sawicka, H.Scheit, G.Schrieder, D.Schwalm, M.D.Seliverstov, T.Sieber, G.Sletten, N.Smirnova, M.Stanoiu, I.Stefanescu, J.-C.Thomas, J.J.Valiente-Dobon, P.Van Duppen, D.Verney, D.Voulot, N.Warr, D.Weisshaar, F.Wenander, B.H.Wolf, M.Zielinska

Coulomb Excitation of Neutron-Rich Zn Isotopes: First Observation of the 2+1 State in 80Zn

NUCLEAR REACTIONS 108Pd, 120Sn(74Zn, 74Zn'), (76Zn, 76Zn'), (78Zn, 78Zn'), (80Zn, 80Zn'), E=2.79-2.87 MeV/nucleon; measured Eγ, Iγ. 74,76,78,80Zn deduced B(E2).

doi: 10.1103/PhysRevLett.99.142501
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Data from this article have been entered in the XUNDL database. For more information, click here.


2006BU34      Int.J. Mass Spectrom. 251, 179 (2006)

M.Bussmann, U.Schramm, D.Habs, V.S.Kolhinen, J.Szerypo

Stopping highly charged ions in a laser-cooled one component plasma of 24Mg+ ions

doi: 10.1016/j.ijms.2006.01.042
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2006EK01      Phys.Scr. T125, 190 (2006)

A.Ekstrom, J.Cederkall, A.Hurst, C.Fahlander, A.Banu, P.Butler, J.Eberth, M.Gorska, D.Habs, M.Huyse, O.Kester, O.Niedermaier, T.Nilsson, M.Pantea, H.Scheit, D.Schwalm, G.Sletten, D.P.Ushasi, P.van Duppen, N.Warr, D.Weisshaar, and the IS418/REX-ISOLDE/ISOLDE Collaborations

Coulomb excitation of 110Sn using REX-ISOLDE

NUCLEAR REACTIONS 58Ni(110Sn, 110Sn'), E=2.8 MeV/nucleon; measured Eγ, Iγ, (particle)γ-coin following projectile Coulomb excitation. 110Sn deduced transition B(E2).

doi: 10.1088/0031-8949/2006/T125/045
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2006JE02      Phys.Lett. B 635, 17 (2006)

H.B.Jeppesen, A.M.Moro, T.Nilsson, F.Ames, P.van den Bergh, U.C.Bergmann, G.Bollen, M.J.G.Borge, J.Cederkall, P.Van Duppen, S.Emhofer, O.Forstner, L.M.Fraile, H.O.U.Fynbo, J.Gomez-Camacho, D.Habs, R.von Hahn, G.Huber, M.Huyse, H.T.Johansson, B.Jonson, O.Kester, H.Lenske, L.Liljeby, M.Meister, G.Nyman, M.Oinonen, M.Pantea, H.Podlech, U.Ratzinger, K.Reisinger, K.G.Rensfelt, R.Repnow, K.Riisager, A.Richter, K.Rudolph, H.Scheit, A.Schempp, P.Schmidt, G.Schrieder, D.Schwalm, T.Sieber, H.Simon, O.Tengblad, E.Tengborn, M.Turrion, L.Weissman, F.Wenander, B.Wolf

Investigation of the 9Li + 2H → 8Li + t reaction at REX-ISOLDE

NUCLEAR REACTIONS 2H(9Li, 8Li), E=2.36 MeV/nucleon; measured particle spectra, σ(θ). 8Li levels deduced energies, spectroscopic factors. Comparison with optical model calculations, post-accelerated radioactive beam.

doi: 10.1016/j.physletb.2006.02.034
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2006NE08      Eur.Phys.J. A 29, 369 (2006)

F.Nebel, J.Szerypo, E.Zech, T.Faestermann, R.Groetzschel, M.Gross, D.Habs, R.Krucken, P.Maier-Komor, P.G.Thirolf, A.Yakushev

Radioactivity distribution at MAFF

doi: 10.1140/epja/i2006-10093-9
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2006RA38      Int.J. Mass Spectrom. 251, 146 (2006)

S.Rahaman, M.Block, D.Ackermann, D.Beck, A.Chaudhuri, S.Eliseev, H.Geissel, D.Habs, F.Herfurth, F.P.Hessberger, S.Hofmann, G.Marx, M.Mukherjee, J.B.Neumayr, M.Petrick, W.R.Plass, W.Quint, C.Rauth, D.Rodriguez, C.Scheidenberger, L.Schweikhard, P.G.Thirolf, C.Weber

On-line commissioning of SHIPTRAP

ATOMIC MASSES 147,148Er, 147Ho; measured masses and time of flight using the Penning-trap mass spectrometer SHIPTRAP. Nuclides produced at SHIP facility.

doi: 10.1016/j.ijms.2006.01.049
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2006SR01      Nucl.Phys. A766, 25 (2006)

J.Srebrny, T.Czosnyka, Ch.Droste, S.G.Rohozinski, L.Prochniak, K.Zajac, K.Pomorski, D.Cline, C.Y.Wu, A.Backlin, L.Hasselgren, R.M.Diamond, D.Habs, H.J.Korner, F.S.Stephens, C.Baktash, R.P.Kostecki

Experimental and theoretical investigations of quadrupole collective degrees of freedom in 104Ru

NUCLEAR REACTIONS 104Ru(208Pb, 208Pb'), E=954 MeV; 104Ru(136Xe, 136Xe'), E=525 MeV; 104Ru(58Ni, 58Ni'), E=165, 190 MeV; measured Eγ, Iγ, (particle)γ -coin following Coulomb excitation. 104Ru deduced levels, J, π, E2 and M1 matrix elements, quadrupole collectivity. Comparison with model predictions.

doi: 10.1016/j.nuclphysa.2005.11.013
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2005BL30      Eur.Phys.J. A 25, Supplement 1, 49 (2005)

M.Block, D.Ackermann, D.Beck, K.Blaum, M.Breitenfeldt, A.Chauduri, A.Doemer, S.Eliseev, D.Habs, S.Heinz, F.Herfurth, F.P.Hessberger, S.Hofmann, H.Geissel, H.-J.Kluge, V.Kolhinen, G.Marx, J.B.Neumayr, M.Mukherjee, M.Petrick, W.Plass, W.Quint, S.Rahaman, C.Rauth, D.Rodriguez, C.Scheidenberger, L.Schweikhard, M.Suhonen, P.G.Thirolf, Z.Wang, C.Weber, and the SHIPTRAP Collaboration

The ion-trap facility SHIPTRAP: Status and perspectives

doi: 10.1140/epjad/i2005-06-013-5
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2005CS01      Phys.Lett. B 615, 175 (2005)

M.Csatlos, A.Krasznahorkay, P.G.Thirolf, D.Habs, Y.Eisermann, T.Faestermann, G.Graw, J.Gulyas, M.N.Harakeh, R.Hertenberger, M.Hunyadi, H.J.Maier, Z.Mate, O.Schaile, H.-F.Wirth

Resonant tunneling through the triple-humped fission barrier of 236U

NUCLEAR REACTIONS 235U(d, pF), E=9.73 MeV; measured Ep, prompt fission probability vs excitation energy. 236U deduced hyperdeformed rotational bands, fission barrier features, resonant tunneling.

doi: 10.1016/j.physletb.2005.04.042
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2005HA63      Eur.Phys.J. A 25, Supplement 1, 57 (2005)

D.Habs, M.Gross, S.Heinz, O.Kester, V.S.Kolhinen, J.Neumayr, U.Schramm, T.Schatz, J.Szerypo, P.Thirolf, C.Weber

Development of a Penning trap system in Munich

doi: 10.1140/epjad/i2005-06-196-7
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2005NI09      Nucl.Phys. A752, 273c (2005)

O.Niedermaier, H.Scheit, V.Bildstein, H.Boie, J.Fitting, R.von Hahn, F.Kock, M.Lauer, U.K.Pal, H.Podlech, R.Repnow, D.Schwalm, C.Alvarez, F.Ames, G.Bollen, S.Emhofer, D.Habs, O.Kester, R.Lutter, K.Rudolph, M.Pasini, P.G.Thirolf, B.H.Wolf, J.Eberth, G.Gersch, H.Hess, P.Reiter, O.Thelen, N.Warr, D.Weisshaar, F.Aksouh, P.Van den Bergh, P.Van Duppen, M.Huyse, O.Ivanov, P.Mayet, J.Van de Walle, J.Aysto, P.A.Butler, J.Cederkall, P.Delahaye, H.O.U.Fynbo, L.M.Fraile, O.Forstner, S.Franchoo, U.Koster, T.Nilsson, M.Oinonen, T.Sieber, F.Wenander, M.Pantea, A.Richter, G.Schrieder, H.Simon, T.Behrens, R.Gernhauser, T.Kroll, R.Krucken, M.Munch, T.Davinson, J.Gerl, G.Huber, A.Hurst, J.Iwanicki, B.Jonson, P.Lieb, L.Liljeby, A.Schempp, A.Scherillo, P.Schmidt, G.Walter

The neutron-rich Mg isotopes: first results from MINIBALL at REX-ISOLDE

NUCLEAR REACTIONS Ni(30Mg, 30Mg'), E=2.25 MeV/nucleon; measured Eγ, Iγ, (particle)γ-coin following projectile Coulomb excitation. 30Mg deduced transition, B(E2).

doi: 10.1016/j.nuclphysa.2005.02.071
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2005NI11      Phys.Rev.Lett. 94, 172501 (2005)

O.Niedermaier, H.Scheit, V.Bildstein, H.Boie, J.Fitting, R.von Hahn, F.Kock, M.Lauer, U.K.Pal, H.Podlech, R.Repnow, D.Schwalm, C.Alvarez, F.Ames, G.Bollen, S.Emhofer, D.Habs, O.Kester, R.Lutter, K.Rudolph, M.Pasini, P.G.Thirolf, B.H.Wolf, J.Eberth, G.Gersch, H.Hess, P.Reiter, O.Thelen, N.Warr, D.Weisshaar, F.Aksouh, P.Van den Bergh, P.Van Duppen, M.Huyse, O.Ivanov, P.Mayet, J.Van de Walle, J.Aysto, P.A.Butler, J.Cederkall, P.Delahaye, H.O.U.Fynbo, L.M.Fraile, O.Forstner, S.Franchoo, U.Koster, T.Nilsson, M.Oinonen, T.Sieber, F.Wenander, M.Pantea, A.Richter, G.Schrieder, H.Simon, T.Behrens, R.Gernhauser, T.Kroll, R.Krucken, M.Munch, T.Davinson, J.Gerl, G.Huber, A.Hurst, J.Iwanicki, B.Jonson, P.Lieb, L.Liljeby, A.Schempp, A.Scherillo, P.Schmidt, G.Walter

"Safe" Coulomb Excitation of 30Mg

NUCLEAR REACTIONS Ni(30Mg, 30Mg'), E=2.25 MeV/nucleon; measured Eγ, Iγ, (particle)γ-coin following projectile Coulomb excitation. 30Mg transition deduced B(E2).

doi: 10.1103/PhysRevLett.94.172501
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2005SC27      Eur.Phys.J. A 25, Supplement 1, 397 (2005)

H.Scheit, O.Niedermaier, V.Bildstein, H.Boie, J.Fitting, R.von Hahn, F.Kock, M.Lauer, U.K.Pal, H.Podlech, R.Repnow, D.Schwalm, C.Alvarez, F.Ames, G.Bollen, S.Emhofer, D.Habs, O.Kester, R.Lutter, K.Rudolph, M.Pasini, P.G.Thirolf, B.H.Wolf, J.Eberth, G.Gersch, H.Hess, P.Reiter, O.Thelen, N.Warr, D.Weisshaar, F.Aksouh, P.Van den Bergh, P.Van Duppen, M.Huyse, O.Ivanov, P.Mayet, J.Van de Walle, J.Aysto, P.A.Butler, J.Cederkall, P.Delahaye, H.O.U.Fynbo, L.M.Fraile, O.Forstner, S.Franchoo, U.Koster, T.Nilsson, M.Oinonen, T.Sieber, F.Wenander, M.Pantea, A.Richter, G.Schrieder, H.Simon, T.Behrens, R.Gernhauser, T.Kroll, R.Krucken, M.Munch, T.Davinson, J.Gerl, G.Huber, A.Hurst, J.Iwanicki, B.Jonson, P.Lieb, L.Liljeby, A.Schempp, A.Scherillo, P.Schmidt, G.Walter

Coulomb excitation of neutron-rich beams at REX-ISOLDE

NUCLEAR REACTIONS Ni(30Mg, 30Mg'), E=2.2 MeV/nucleon; measured Eγ, Iγ, (particle)γ-coin following projectile Coulomb excitation.2Hmeasured Eγ, Iγ, γγ-, (particle)γ-coin. 30Mg deduced transitions B(E2). 31Mg deduced transitions. Miniball array.

doi: 10.1140/epjad/i2005-06-165-2
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2004CE06      Nucl.Phys. A746, 17c (2004)

J.Cederkall, F.Ames, P.Butler, P.Delahaye, V.Fedoseev, M.Lindroos, T.Nilsson, T.Sieber, F.Wenander, M.Pantea, S.Emhofer, D.Habs, O.Kester, K.Rudolph, R.von Hahn, O.Niedermaier, H.Scheit, D.Schwalm, P.van Duppen, M.Huyse, B.Jonsson, G.Nyman, J.Eberth, P.Reiter, D.Weisshaar, and the REX-ISOLDE Collaboration

REX-ISOLDE - experiences from the first year of operation

doi: 10.1016/j.nuclphysa.2004.09.014
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2004FA31      Nucl.Phys. A746, 22c (2004)

T.Faestermann, W.Assmann, L.Beck, H.Bongers, W.Carli, M.Gross, R.Grossmann, D.Habs, P.Hartung, S.Heinz, P.Juttner, O.Kester, R.Krucken, H.-J.Maier, P.Maier-Komor, F.Nebel, F.Ospald, M.Pasini, M.Schumann, J.Szerypo, P.G.Thirolf, F.Tralmer, E.Zech

The Munich Accelerator for Fission Fragments - MAFF

doi: 10.1016/j.nuclphysa.2004.09.106
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2004PA41      Nucl.Phys. A746, 397c (2004)

M.Pasini, O.Kester, D.Habs, M.Gross, T.Sieber, H.J.Maier, W.Assmann, R.Krucken, T.Faestermann, A.Schempp, U.Ratzinger, C.P.Safvan

Radioactive ion beam acceleration at MAFF

doi: 10.1016/j.nuclphysa.2004.09.116
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2003KR23      Acta Phys.Hung.N.S. 18, 323 (2003)

A.Krasznahorkay, M.Csatlos, L.Csige, Y.Eisermann, T.Faestermann, Z.Gacsi, G.Graw, J.Gulyas, D.Habs, M.N.Harakeh, M.Heil, R.Hertenberger, F.Kappeler, A.Krasznahorkay, Jr., M.J.Maier, Z.Mate, R.Reifarth, P.G.Thirolf, J.Timar, H.F.Wirth

Hyperdeformation and Clustering in the Actinide Region

NUCLEAR REACTIONS 235U(d, pF), E=9.75 MeV; measured Ep, fission fragment spectra. 236U deduced hyperdeformed states, α-decay features. 232Th(n, F), E ≈ 1.6 MeV; measured fission fragments mass distributions, kinetic energy; deduced cluster effects.

doi: 10.1556/APH.18.2003.2-4.34
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2003TH14      Acta Phys.Hung.N.S. 18, 317 (2003)

P.G.Thirolf, D.Gassmann, D.Habs, M.Hunyadi, A.Krasznahorkay, E.Mergel, H.Hubel, D.Pansegrau, D.Schwalm, M.J.Chromik, M.Csatlos, J.Domscheit, Y.Eisermann, T.Faestermann, G.Graw, A.Gorgen, J.Gulyas, K.Hauschild, R.Hertenberger, T.Hartlein, F.Kock, A.Lopez-Martens, Z.Mate, H.J.Maier, A.Metz, S.Neumann, A.Neusser, P.Reiter, G.Schonwasser, H.Scheit

Detailed Spectroscopy of Superdeformed Actinide Nuclei

NUCLEAR REACTIONS 238U(α, 2nF), E=25 MeV; analyzed Eγ, Iγ, (fission fragment)γ-coin. 239Pu(d, pF), E=12.5 MeV; analyzed Ep, (fission fragment)p-coin. 240Pu deduced level structure in superdeformed second minimum.

doi: 10.1556/APH.18.2003.2-4.33
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2002KE06      Nucl.Phys. A701, 71c (2002)

O.Kester, D.Habs, M.Gross, H.J.Maier, P.G.Thirolf, T.Sieber, T.Faestermann, T.von Egidy, U.Koster

RNB Production with Thermal Neutrons

doi: 10.1016/S0375-9474(01)01551-2
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2002RE20      Nucl.Phys. A701, 209c (2002)

P.Reiter, J.Eberth, H.Faust, S.Franchoo, J.Gerl, C.Gund, D.Habs, M.Huyse, A.Jungclaus, K.P.Lieb, H.Scheit, D.Schwalm, H.G.Thomas, P.van Duppen, D.Weisshaar

The MINIBALL Array

doi: 10.1016/S0375-9474(01)01576-7
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2002SC27      Nucl.Phys. A701, 579c (2002)

J.Schonfelder, D.Ackermann, H.Backe, G.Bollen, J.Dilling, A.Dretzke, O.Engels, J.Estermann, D.Habs, S.Hofmann, F.P.Hessberger, H.-J.Kluge, W.Lauth, W.Ludolphs, M.Maier, G.Marx, R.B.Moore, W.Quint, D.Rodriguez, M.Sewtz, G.Sikler, C.Toader, Chr.Weber

SHIPTRAP - A Capture and Storage Facility for Heavy Radionuclides at GSI

doi: 10.1016/S0375-9474(01)01648-7
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2002SI17      Nucl.Phys. A701, 656c (2002)

T.Sieber, O.Kester, D.Habs, S.Emhofer, K.Rudolph, H.Bongers, A.Schempp, U.Ratzinger

Design and Status of the Front Part of the REX-ISOLDE Linac

doi: 10.1016/S0375-9474(01)01662-1
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2001AM12      Hyperfine Interactions 132, 469 (2001)

F.Ames, P.Schmidt, O.Forstner, G.Bollen, O.Engels, D.Habs, G.Huber, and the REX ISOLDE Collaboration

Space-Charge Effects with REXTRAP

doi: 10.1023/A:1011922811309
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2001BA65      Nucl.Phys. A690, 215c (2001)

H.Backe, A.Dretzke, D.Habs, M.Hies, G.Kube, H.Kunz, W.Lauth, H.J.Maier, R.Repnow, M.Sewtz, N.Trautmann

Stability of Superdeformation for Americium Fission Isomers as Function of the Neutron Number

NUCLEAR MOMENTS 240,242,242Am; measured fission isomer isotope shifts; deduced quadrupole moments, deformation.

doi: 10.1016/S0375-9474(01)00944-7
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2001GA05      Phys.Lett. 497B, 181 (2001)

D.Gassmann, P.G.Thirolf, E.Mergel, D.Habs, M.Chromik, J.Domscheit, A.Gorgen, K.Hauschild, H.Hubel, M.Hunyadi, A.Krasznahorkay, A.Lopez-Martens, S.Neumann, A.Neusser, D.Pansegrau, P.Reiter, H.Scheit, G.Schonwasser, D.Schwalm

Conversion Electron Spectroscopy in the Superdeformed Minimum of 240Pu

NUCLEAR REACTIONS 238U(α, 2n), E=25 MeV; measured prompt Eγ, Iγ, E(ce), I(ce), (ce)γ-coin in coincidence with delayed fission. 240Pu deduced superdeformed fission isomer levels, J, π, collective features, E0 transitions. Mini-orange spectrometers.

doi: 10.1016/S0370-2693(00)01353-8
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Data from this article have been entered in the XUNDL database. For more information, click here.


2001HA32      Prog.Part.Nucl.Phys. 46, 343 (2001)

D.Habs, F.Ames, W.Assmann, S.Emhofer, O.Engels, M.Gross, O.Kester, H.J.Maier, P.Reiter, T.Sieber, P.Thirolf, and the REX-ISOLDE and MAFF-Collaboration

The REX-ISOLDE-Project and the Munich Accelerator for Fission Fragments MAFF

doi: 10.1016/S0146-6410(01)00141-7
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2001HU05      Acta Phys.Pol. B32, 699 (2001)

M.Hunyadi, D.Gassmann, A.Krasznahorkay, D.Habs, M.Csatlos, Y.Eisermann, T.Faestermann, G.Graw, J.Gulyas, R.Hertenberger, H.J.Maier, Z.Mate, A.Metz, P.Thirolf, M.Chromik, S.Y.van der Werf

Superdeformed Rotational Bands in 240Pu

NUCLEAR REACTIONS 239Pu(d, pF), E=12.5 MeV; measured proton spectra, (fission fragment)(proton)-coin. 240Pu deduced fission resonance features, superdeformed band.


2001HU12      Phys.Lett. 505B, 27 (2001)

M.Hunyadi, D.Gassmann, A.Krasznahorkay, D.Habs, P.G.Thirolf, M.Csatlos, Y.Eisermann, T.Faestermann, G.Graw, J.Gulyas, R.Hertenberger, H.J.Maier, Z.Mate, A.Metz, M.J.Chromik

Excited Superdeformed Kπ = 0+ Rotational Bands in β-vibrational Fission Resonances of 240Pu

NUCLEAR REACTIONS 239Pu(d, pF), E=12.5 MeV; measured fission fragment and proton spectra, (proton)(fragment)-coin. 240Pu deduced β-vibrational fission resonance features, excited superdeformed bands J, π, energy.

doi: 10.1016/S0370-2693(01)00341-0
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Data from this article have been entered in the XUNDL database. For more information, click here.


2001KR05      Acta Phys.Pol. B32, 657 (2001)

A.Krasznahorkay, D.Habs, M.Hunyadi, D.Gassmann, M.Csatlos, Y.Eisermann, T.Faestermann, G.Graw, J.Gulyas, R.Hertenberger, H.J.Maier, Z.Mate, A.Metz, J.Ott, P.Thirolf, S.Y.van der Werf

Superdeformation, Hyperdeformation and Clustering in the Actinide Region

NUCLEAR REACTIONS 238U(α, 2n), E=25 MeV; measured Eγ, Iγ, E(ce), I(ce), delayed fission. 240Pu deduced levels, J, π built on fission isomer. 239Pu(d, pF), E=12.5 MeV; 233,235U(d, pF), E not given; measured proton spectra, (fission fragment)(proton)-coin. 240Pu, 234,236U deduced fission isomer deformation features.


2001KR17      Acta Phys.Hung.N.S. 13, 111 (2001)

A.Krasznahorkay, D.Habs, M.Hunyadi, D.Gassmann, M.Csatlos, Y.Eisermann, T.Faestermann, G.Graw, J.Gulyas, R.Hertenberger, H.J.Maier, Z.Mate, A.Metz, J.Ott, P.G.Thirolf, S.Y.van der Werf

Hyperdeformation and Clusterization in the Actinide Region

NUCLEAR REACTIONS 233,235U(d, pF), E=9.7, 12.5 MeV; measured proton spectra, fission fragment spectra, mass distributions. 234,236U deduced fission probabilities, hyperdeformation.

doi: 10.1556/APH.13.2001.1-3.12
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2001MA98      Hyperfine Interactions 132, 463 (2001)

G.Marx, D.Ackermann, J.Dilling, F.P.Hessberger, S.Hofmann, H.-J.Kluge, R.Mann, G.Munzenberg, Z.Qamhieh, W.Quint, D.Rodriguez, M.Schadel, J.Schonfelder, G.Sikler, C.Toader, C.Weber, O.Engels, D.Habs, P.Thirolf, H.Backe, A.Dretzke, W.Lauth, W.Ludolphs, M.Sewtz, and the SHIPTRAP Collaboration

Status of the SHIPTRAP Project: A capture and storage facility for heavy radionuclides from SHIP

doi: 10.1023/A:1011904231676
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2001ME23      Acta Phys.Hung.N.S. 13, 199 (2001)

E.Mergel, G.Schonwasser, H.Hubel, D.Rossbach, P.G.Thirolf, M.Chromik, D.Gassmann, D.Habs, P.Reiter

A Setup for the Search for E0 Decay of Superdeformed 236U

doi: 10.1556/APH.13.2001.1-3.28
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2001TH16      Acta Phys.Hung.N.S. 13, 93 (2001)

P.G.Thirolf, D.Gassmann, D.Habs, M.J.Chromik, Y.Eisermann, G.Graw, R.Hertenberger, H.J.Maier, A.Metz, P.Reiter, T.Faestermann, A.Krasznahorkay, M.Hunyadi, M.Csatlos, J.Gulyas, Z.Mate, D.Pansegrau, H.Scheit, D.Schwalm, E.Mergel, H.Hubel, A.Gorgen

Detailed Spectroscopy in the Superdeformed Second Minimum of 240Pu

NUCLEAR REACTIONS 238U(α, 2n), E=25 MeV; measured Eγ, Iγ, E(ce), I(ce), (fragment)γ-coin following delayed fission. 240Pu deduced superdeformed levels, J, π, ICC.

doi: 10.1556/APH.13.2001.1-3.11
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2000HA68      Hyperfine Interactions 129, 43 (2000)

D.Habs, O.Kester, T.Sieber, H.Bongers, S.Emhofer, P.Reiter, P.G.Thirolf, G.Bollen, J.Aysto, O.Forstner, H.Ravn, T.Nilsson, M.Oinonen, H.Simon, J.Cederkall, F.Ames, P.Schmidt, G.Huber, L.Liljeby, O.Skeppstedt, K.G.Rensfelt, F.Wenander, B.Jonson, G.Nyman, R.von Hahn, H.Podlech, R.Repnow, C.Gund, D.Schwalm, A.Schempp, K.-U.Kuhnel, C.Welsch, U.Ratzinger, G.Walter, A.Huck, K.Kruglov, M.Huyse, P.Van den Bergh, P.Van Duppen, L.Weissman, A.C.Shotter, A.N.Ostrowski, T.Davinson, P.J.Woods, J.Cub, A.Richter, G.Schrieder, and the REX-ISOLDE Collaboration

The REX-ISOLDE project

doi: 10.1023/A:1012603025802
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2000PA40      Phys.Lett. 484B, 1 (2000)

D.Pansegrau, P.Reiter, D.Schwalm, H.Bauer, J.Eberth, D.Gassmann, D.Habs, T.Hartlein, F.Kock, H.G.Thomas

γ Spectroscopy in the Superdeformed Minimum of 240Pu

NUCLEAR REACTIONS 238U(α, 2n), E=25 MeV; measured Eγ, Iγ, (fragment)γ-coin following compound nucleus fission. 240Pu deduced levels, J, π built on superdeformed shape isomer, fission T1/2. Euroball cluster detectors.

doi: 10.1016/S0370-2693(00)00638-9
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Data from this article have been entered in the XUNDL database. For more information, click here.


1999HU12      Acta Phys.Pol. B30, 1263 (1999)

M.Hunyadi, A.Krasznahorkay, M.Csatlos, Y.Eisermann, T.Faestermann, D.Gassmann, G.Graw, J.Gulyas, D.Habs, R.Hertenberger, H.J.Maier, A.Metz, Z.Mate, J.Ott, P.Thirolf

Multi-Phonon Superdeformed States in 240Pu

NUCLEAR REACTIONS 239Pu(d, pF), E=12.5 MeV; measured proton spectra, p-(Fission fragment)-coin. 240Pu deduced multiphonon superdeformed band.


1999KR16      Phys.Lett. 461B, 15 (1999)

A.Krasznahorkay, D.Habs, M.Hunyadi, D.Gassmann, M.Csatlos, Y.Eisermann, T.Faestermann, G.Graw, J.Gulyas, R.Hertenberger, H.J.Maier, Z.Mate, A.Metz, J.Ott, P.Thirolf, S.Y.van der Werf

On the Excitation Energy of the Ground State in the Third Minimum of 234U

NUCLEAR REACTIONS 233U(d, pF), E=12.5 MeV; measured proton spectra, (fission fragment)(proton)-coin. 234U deduced fission probability vs excitation energy, rotational bands, hyperdeformation, third minimum ground state energy, level density. Comparison with Fermi-gas formula.

doi: 10.1016/S0370-2693(99)00826-6
Citations: PlumX Metrics


1999KR18      Acta Phys.Pol. B30, 1467 (1999)

A.Krasznahorkay, M.Hunyadi, M.Csatlos, Y.Eisermann, T.Faestermann, D.Gassmann, G.Graw, J.Gulyas, D.Habs, R.Hertenberger, H.J.Maier, A.Metz, Z.Mate, J.Ott, P.Thirolf

Hyperdeformed Rotational Bands in 234U

NUCLEAR REACTIONS 233U(d, pF), E=12.5 MeV; measured proton spectrum, p(fission fragment)-coin. 234U deduced hyperdeformed band.


1999VO06      Acta Phys.Slovaca 49, 107 (1999)

T.von Egidy, P.Kienle, U.Koster, D.Habs, M.Gross, O.Kester, H.J.Maier, P.G.Thirolf, and the MAFF Collaboration

The Munich Accelerator for Fission Fragments (MAFF) at the New Reactor FRM II


1998BA04      Phys.Rev.Lett. 80, 920 (1998)

H.Backe, M.Hies, H.Kunz, W.Lauth, O.Curtze, P.Schwamb, M.Sewtz, W.Theobald, R.Zahn, K.Eberhardt, N.Trautmann, D.Habs, R.Repnow, B.Fricke

Isotope Shift Measurements for Superdeformed Fission Isomeric States

NUCLEAR MOMENTS 240m,242mAm; measured fission isomers optical isotope shifts relative to 241,243Am; deduced quadrupole moments. Resonance ionization spectroscopy, buffer gas cell.

doi: 10.1103/PhysRevLett.80.920
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1998KR02      Phys.Rev.Lett. 80, 2073 (1998)

A.Krasznahorkay, M.Hunyadi, M.N.Harakeh, M.Csatlos, T.Faestermann, A.Gollwitzer, G.Graw, J.Gulyas, D.Habs, R.Hertenberger, H.J.Maier, Z.Mate, D.Rudolph, P.Thirolf, J.Timar, B.D.Valnion

Experimental Evidence for Hyperdeformed States in U Isotopes

NUCLEAR REACTIONS 235U(d, pF), E=9.73, 13.0 MeV; measured p-spectra, (fission fragment)p-coin, fission fragment σ(θ). 236U deduced resonances, fission probability vs excitation energy, evidence for hyperdeformation. Results for other U isotopes discussed.

doi: 10.1103/PhysRevLett.80.2073
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1998KR19      Acta Phys.Hung.N.S. 7, 35 (1998)

A.Krasznahorkay, M.Hunyadi, M.Csatlos, A.Balanda, A.Gollwitzer, G.Graw, J.Gulyas, D.Habs, R.Hertenberger, Z.Mate, H.J.Maier, D.Rudolph, P.Thirolf, J.Timar, B.D.Valnion

Hyperdeformed States in the Third Minimum of the Fission Potential

NUCLEAR REACTIONS 235U(d, pF), E=9.7, 13 MeV; measured proton spectra, fission fragments angular distributions, (proton)(fragment)-coin. 234,236U deduced rotational bands, possible hyperdeformed states. Third minimum of fission potential.


1997CU03      Acta Phys.Pol. B28, 367 (1997)

J.Cub, J.Holeczek, S.Wan, T.Aumann, T.Baumann, K.Boretzky, W.Dostal, B.Eberlein, H.Emling, Ch.Ender, Th.W.Elze, H.Geissel, J.Gerl, A.Grunschloss, D.Habs, T.Happ, R.Holzmann, N.Iwasa, M.Kaspar, A.Kleinbohl, F.Kock, O.Koschorrek, J.V.Kratz, G.Kraus, R.Kulessa, Y.Leifels, A.Leistenschneider, G.Munzenberg, F.Nickel, I.Peter, P.Reiter, H.Schaffner, C.Scheidenberger, G.Schrieder, D.Schwalm, R.Schubart, R.Schubert, W.Schwab, H.Simon, G.Stengel, J.Stroth, K.Summerer, A.Surowiec, P.Thirolf, E.Wajda, H.J.Wollersheim, A.Zentek

Invariant-Mass and γ-Ray Spectroscopy using Secondary, Radioactive Ion Beams

NUCLEAR REACTIONS Be(50Ti, X), E=330 MeV/nucleon; measured fragment mass, charge distribution. Pb(18O, 18O'), (46K, 46K'), (27Mg, 27Mg'), (28Mg, 28Mg'), E≈250 MeV/nucleon; measured Eγ, Iγ following projectile Coulomb excitation. Secondary, radioactive beams.


1997HA11      Nucl.Phys. A616, 29c (1997)

D.Habs, O.Kester, G.Bollen, L.Liljeby, K.G.Rensfelt, D.Schwalm, R.von Hahn, G.Walter, P.Van Duppen, and the REX-ISOLDE Collaboration

The REX-ISOLDE Project

NUCLEAR REACTIONS, ICPND U(p, X)25Na/27Na/28Na/29Na/30Na/31Na/32Na/33Na/34Na, E=1 GeV; measured production yields for residual nuclei. Other aspects included, PS-ISOLDE setup, Uc2 target, surface ion source.

doi: 10.1016/S0375-9474(97)00071-7
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1052.


1997HA12      Nucl.Phys. A616, 39c (1997)

D.Habs, O.Kester, P.Thirolf, K.E.G.Lobner, H.J.Maier, D.Rudolph, K.Rudolph, U.Schramm, T.Faestermann, G.Hinderer, P.Kienle, U.Koster, H.-J.Korner, E.Steichele, A.Ulrich, T.von Egidy, H.Faust, M.Gross

The Munich Fission Fragment Accelerator

doi: 10.1016/S0375-9474(97)00072-9
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1997HA43      Z.Phys. A358, 161 (1997)

D.Habs, D.Rudolph, O.Kester, P.Thirolf, P.Reiter, D.Schwalm, G.Walter, P.Van Duppen, J.Eberth, and the REX-ISOLDE and MINIBALL Collaboration

Physics with REX-ISOLDE and MINIBALL

doi: 10.1007/s002180050294
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1996BA52      Hyperfine Interactions 97/98, 535 (1996)

H.Backe, R.-R.Baum, B.Fricke, D.Habs, K.Hellmann, M.Hies, Ch.Illgner, Ch.Krameyer, H.Kunz, W.Lauth, R.Martin, P.Schwamb, W.Theobald, P.Thorle, N.Trautmann

Isotope Shift and Hyperfine Structure Measurements at the 242mAm Fission Isomer

RADIOACTIVITY 242mAm(SF) [from 242Pu(d, 2n), E=12 MeV]; 241,243Am(α); measured hfs, relative isotope shift. 242Am deduced fission isomer quadrupole deformation, quadrupole moment.

doi: 10.1007/BF02150196
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1996FI06      Z.Phys. A355, 401 (1996)

J.B.Fitzgerald, D.Habs, F.Heller, P.Reiter, D.Schwalm, P.Thirolf, A.Wieswesser

Fragment Mass Dependence of the High-Energy γ-Ray Spectrum in Fission

NUCLEAR REACTIONS 197Au(19F, F), 232Th, 238U(18O, F), E=120 MeV; measured high energy γ spectra following fission; deduced fragment mass dependence.

RADIOACTIVITY 252Cf(SF); measured high energy γ spectra following fission; deduced fragment mass dependence.

doi: 10.1007/s002180050129
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1994ME02      Phys.Rev. C49, 743 (1994)

B.Meltzow, E.K.Warburton, Ch.Ender, J.Gerl, D.Habs, U.Lauff, J.Schirmer, D.Schwalm, P.Thirolf

Measurement and Significance of Γ(γ)/Γ for the 7117-keV 4+ Level of 18O

NUCLEAR REACTIONS 12C(7Li, p), (7Li, pγ), E=18 MeV; measured Ep, pγ-coin. 18O level deduced Γγ/Γ, B(λ). Shell model.

doi: 10.1103/PhysRevC.49.743
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1994VO08      Phys.Lett. 325, 300 (1994)

H.von Busch, P.Thirolf, Ch.Ender, D.Habs, F.Kock, Th.Schulze, D.Schwalm

Measurement of the Decay e+e- → 4γ at Rest

doi: 10.1016/0370-2693(94)90015-9
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1993BA79      Hyperfine Interactions 78, 35 (1993)

H.Backe, P.Graffe, D.Habs, M.Hies, Ch.Illgner, H.Kunz, W.Lauth, H.Schope, P.Schwamb, W.Theobald, P.Thorle, N.Trautmann, R.Zahn

Radiation Detected Resonance Ionization Spectroscopy on 208Tl and 242mAm

RADIOACTIVITY 243Am, 242mAm; measured fission isomer resonance ionization signals; deduced large isotope shift. Ultra-sensitive laser spectroscopic method.

doi: 10.1007/BF00568115
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1993KO42      Phys.Lett. 317B, 19 (1993)

W.Korten, T.Hartlein, J.Gerl, D.Habs, D.Schwalm

Observation of a Harmonic Two-Phonon Vibration in a Deformed Nucleus

NUCLEAR REACTIONS 232Th(90Zr, 90Zr'), E=396, 415 MeV; measured γγ-coin following Coulomb excitation. 232Th deduced levels, J, π, K, B(λ), band structure.

doi: 10.1016/0370-2693(93)91563-3
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1992BA67      Hyperfine Interactions 74, 47 (1992)

H.Backe, Th.Blonnigen, M.Dahlinger, U.Doppler, P.Graffe, D.Habs, M.Hies, Ch.Illgner, H.Kunz, W.Lauth, H.Schope, P.Schwamb, W.Theobald, R.Zahn

First Observation of a Resonance Ionization Signal on 242mAm Fission Isomers

RADIOACTIVITY 242mAm(SF) [from 242Pu(d, 2n), E=12 MeV]; measured resonance ionization followed by isomer fission decay. Buffer gas cell, two-step resonance ionization, excimer dye laser combination.

doi: 10.1007/BF02398616
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1991HE10      Phys.Lett. 258B, 275 (1991)

H.-J.Hennrich, G.Breitbach, W.Kuhn, V.Metag, R.Novotny, D.Habs, D.Schwalm

Differences in Angular Momentum Distributions for Near-Barrier Fusion of 32S + 100Mo and 36S + 96Mo

NUCLEAR REACTIONS 100Mo(32S, X), E=99-120 MeV; 96Mo(36S, X), E=107.5-123.5 MeV; measured σ(evaporation residue θ). Coupled-channels analysis.

doi: 10.1016/0370-2693(91)91084-9
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1991KO19      Z.Phys. A339, 217 (1991)

W.Korten, J.Gerl, D.Habs, D.Schwalm

Search for a Transient Electric Field Gradient in the System 90Zr → 148Nd with the Crystal Ball Spectrometer

NUCLEAR REACTIONS 148Nd(90Zr, 90Zr'), E=302 MeV; measured γ(particle)(θ), Eγ, Iγ following Coulomb excitation; deduced transient electric field gradient. Crystal ball spectrometer.

doi: 10.1007/BF01284055
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1990LU02      Z.Phys. A335, 369 (1990)

E.Lubkiewicz, H.Emling, H.Grein, R.Kulessa, R.S.Simon, H.J.Wollersheim, Ch.Ender, J.Gerl, D.Habs, D.Schwalm

Measurement of g-Factors in 160Yb by a γ-γ Coincidence Technique

NUCLEAR REACTIONS, ICPND 64Ni(100Mo, 4n), (100Mo, 3n), (100Mo, 5n), E=430 MeV; measured γγ-coin, residual yields, γγ(θ, φ). 160Yb deduced levels, T1/2, g, transition quadrupole moment. 4π geometry, transient magnetic fields, recoil distance technique.


1990SA14      Phys.Rev. C41, R1901 (1990)

S.J.Sanders, B.B.Back, R.V.F.Janssens, D.G.Kovar, D.Habs, D.Henderson, T.-L.Khoo, H.Korner, G.-E.Rathke, T.F.Wang, F.L.H.Wolfs, K.B.Beard

Additional Evidence for Fusion-Fission in 32S + 24Mg Reactions: Division of excitation energy and spin in the fission fragments

NUCLEAR REACTIONS 24Mg(32S, 12C), E=140 MeV; measured γ(12C)-coin, E(γ); deduced reaction mechanism, scission temperature.

doi: 10.1103/PhysRevC.41.R1901
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1989BR27      Phys.Rev. C40, 2893 (1989)

G.Breitbach, G.Koch, S.Koch, W.Kuhn, A.Ruckelshausen, V.Metag, R.Novotny, S.Riess, D.Habs, D.Schwalm, E.Grosse, H.Stroher

Dominance of Nucleon-Nucleon Bremsstrahlung in Mass-Asymmetric Heavy-Ion Collisions at 15 MeV/Nucleon

NUCLEAR REACTIONS W(16O, Xγ), E=15 MeV/nucleon; measured σ(θγ, Eγ), γ-multiplicity; deduced nucleon-nucleon bremsstrahlung dominance.

doi: 10.1103/PhysRevC.40.2893
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1989GE01      Phys.Rev. C39, 1145 (1989)

J.Gerl, Ch.Ender, D.Habs, W.Korten, E.Schulz, D.Schwalm

Observation of the Ground-State Band of 234Th Using the 232Th(18O, 16O) Reaction

NUCLEAR REACTIONS 232Th(18O, 16O), E=90 MeV; measured E(γ), I(γ), particle spectra, (particle)γ-, γγ-coin. 234Th deduced levels, J, π, rotational band, deformation.

doi: 10.1103/PhysRevC.39.1145
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1989GE06      Z.Phys. A334, 195 (1989)

J.Gerl, W.Korten, D.Habs, D.Schwalm, H.J.Wollersheim

Spectroscopy and Reaction Mechanism of the System 90Zr → 232Th in the Vicinity of the Coulomb Barrier

NUCLEAR REACTIONS 232Th(90Zr, X), (90Zr, 91Zr), (90Zr, 90Zr), (90Zr, 94Zr), E=520 MeV; measured γ(particle)-coin; deduced σ channel dependence, reaction mechanism.


1989GL05      Nucl.Phys. A502, 315c (1989)

P.Glassel, R.Schmid-Fabian, D.Schwalm, D.Habs, H.U.v.Helmolt

252Cf Fission Revisted - New Insights into the Fission Process

RADIOACTIVITY 252Cf(SF); measured Eγ, Iγ, γ-multiplicity following fission fragment decay.

doi: 10.1016/0375-9474(89)90672-6
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1989HA40      Nucl.Phys. A502, 105c (1989)

D.Habs

Spectroscopy of the Second Minimum

NUCLEAR STRUCTURE A ≈ 150; analyzed high spin level systematics; deduced comparison with fission second minimum in actnide region.

doi: 10.1016/0375-9474(89)90657-X
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1989KU02      Phys.Rev.Lett. 62, 1103 (1989)

W.Kuhn, A.Ruckelshausen, R.D.Fischer, G.Breitbach, H.J.Hennrich, V.Metag, R.Novotny, R.V.F.Janssens, T.L.Khoo, D.Habs, D.Schwalm, B.Haas, R.S.Simon

Nuclear-Structure Dependence of Heavy-Ion-Fusion Partial-Wave Distributions

NUCLEAR REACTIONS 92Zr(64Ni, X), E(cm)=138.8 MeV; 96Zr(64Ni, X), E(cm)=139.5 MeV; measured partial fusion σ.

doi: 10.1103/PhysRevLett.62.1103
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1989SC30      Phys.Rev.Lett. 63, 2196 (1989)

J.Schirmer, J.Gerl, D.Habs, D.Schwalm

γ Decay of the Superdeformed Shape Isomer in 236U

NUCLEAR REACTIONS 235U(d, p), E=11 MeV; measured γ time spectra, missing energy vs delayed sum energy. 236U deduced isomer, decay, superdeformation features, γ-decay to fission branching ratio.

doi: 10.1103/PhysRevLett.63.2196
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1988BE40      Z.Phys. A331, 343 (1988)

J.Bendahan, C.Broude, M.Hass, E.Dafni, G.Goldring, J.Gerl, D.Habs, W.Korten, D.Schwalm

Heavy Ion Beam Polarization Produced by the Multi-Tilted-Foil Interaction

NUCLEAR REACTIONS 208Pb(51V, 51V'), E=195 MeV; measured X-rays, γ(particle)-coin, ejectile asymmetry following Coulomb excitation. 51V level deduced nuclear polarization.


1988DA15      Nucl.Phys. A484, 337 (1988)

M.Dahlinger, E.Kankeleit, D.Habs, D.Schwalm, B.Schwartz, R.S.Simon, J.D.Burrows, P.A.Butler

Alternating Parity Bands and Octupole Effects in 221Th and 223Th

NUCLEAR REACTIONS 208Pb(16O, 3n), (18O, 3n), E=78-89 MeV; measured E(γ), I(γ), I(ce), residue(evaporation residue)-coin, γγ(evaporation residue)-, e-γ(evaporation residue), e-e-(evaporation residue)-coin, γ-multiplicicity. 221,223Th deduced levels, J, π, rotational bands, octupole deformations. Ge(Li) detectors, Si(Li)-detectors, enriched targets.

doi: 10.1016/0375-9474(88)90076-0
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1988HE01      Phys.Rev.Lett. 60, 11 (1988)

S.Henss, A.Ruckelshausen, R.D.Fischer, W.Kuhn, V.Metag, R.Novotny, R.V.F.Janssens, T.L.Khoo, D.Habs, D.Schwalm, D.Freeman, G.Duchene, B.Haas, F.Haas, S.Hlavac, R.S.Simon

Measurement of the Nuclear Level Density at High Spins

NUCLEAR REACTIONS 92Zr(64Ni, n), E=239 MeV; measured σ(En), Eγ, Iγ, γ(t). 155Er deduced high-spin level density, parameter.

doi: 10.1103/PhysRevLett.60.11
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1988TH03      Nucl.Phys. A482, 93c (1988)

P.Thirolf, D.Habs, D.Schwalm, R.D.Fisher, V.Metag

Angular Momentum Splitting and Spin Dependence of the Giant Dipole Resonance in Hot Nuclei

NUCLEAR REACTIONS 130Te(34S, xn), E=150 MeV; measured γ(θ), Eγ, Iγ. 164Er deduced GDR parameters, deformation.

doi: 10.1016/0375-9474(88)90578-7
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1987KR19      Nucl.Phys. A474, 412 (1987)

J.Kramp, D.Habs, R.Kroth, M.Music, J.Schirmer, D.Schwalm, C.Broude

Nuclear Two-Photon Decay in 0+ → 0+ Transitions

NUCLEAR REACTIONS 16O(p, p'), E=7.58 MeV; measured E(γ), I(γ), γp-coin, γγ(θ), two-photon relative γ(θ/2), linear polarization. 16O level deduced two-photon decay Γ(γ)/Γ, double E1, M1 transition matrix element ratio. Crystal ball.

doi: 10.1016/0375-9474(87)90625-7
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1987RU02      Phys.Rev.Lett. 58, 1584 (1987)

A.Ruckelshausen, B.Haas, D.Habs, R.V.F.Janssens, T.L.Khoo, W.Kuhn, V.Metag, D.Schwalm, R.S.Simon

Comment on ' Entrance- and Exit-Channel Effects and the Suppression of Neutron Emission from 64Ni + 92Zr → 156Er* '

NUCLEAR REACTIONS 92Zr(64Ni, X), E not given; analyzed data; calculated γ-spectrum. 154Er deduced entry region average spin.

doi: 10.1103/PhysRevLett.58.1584
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1986FI04      Phys.Lett. 171B, 33 (1986)

R.D.Fischer, A.Ruckelshausen, G.Koch, W.Kuhn, V.Metag, R.Muhlhans, R.Novotny, H.Stroher, H.Groger, D.Habs, H.W.Heyng, R.Repnow, D.Schwalm, W.Reisdorf, R.S.Simon

Partial Wave Cross Sections for 34S + 130Te Fusion

NUCLEAR REACTIONS 130Te(34S, xn), E=155 MeV; measured γ(θ), γ-multiplicity, residual relative yield for x=3, 4, 5, 6; deduced fusion, evaporation residue σ. 164Er deduced spin distribution. Crystal ball technique.

doi: 10.1016/0370-2693(86)90992-5
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1986RU02      Phys.Rev.Lett. 56, 2356 (1986)

A.Ruckelshausen, R.D.Fischer, W.Kuhn, V.Metag, R.Muhlhans, R.Novotny, T.L.Khoo, R.V.F.Janssens, H.Groger, D.Habs, H.W.Heyng, R.Repnow, D.Schwalm, G.Duchene, R.M.Freeman, B.Haas, F.Haas, S.Hlavac, R.S.Simon

Unexpected Entrance-Channel Effects in the Decay of the Compound Nucleus 156Er

NUCLEAR REACTIONS 92Zr(64Ni, 4n), (64Ni, 3n), (64Ni, 2n), (64Ni, 2np), (64Ni, nα), (64Ni, 2nα), E=239 MeV; 144Sm(12C, 2n), (12C, 3n), (12C, 4n), (12C, nα), (12C, 2nα), (12C, 2np), E=73.5 MeV; measured evaporation residue yield vs spin. 156Er deduced entrance channel effects in decay.

doi: 10.1103/PhysRevLett.56.2356
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1986SC12      Z.Phys. A323, 489 (1986)

B.Schwartz, Ch.Ender, D.Habs, D.Schwalm, M.Dahlinger, E.Kankeleit, H.Folger, R.S.Simon, H.Backe

In-Beam Spectroscopy of 224Th

NUCLEAR REACTIONS 208Pb(18O, 2n), E=78 MeV; measured I(ce), γ(ce)-, γ(recoil nucleus)-coin. 224Th deduced levels, J, π, γ-branching, B(λ), E1, E2 competition.


1985BO32      Z.Phys. A322, 59 (1985)

W.Bonin, H.Backe, M.Dahlinger, S.Glienke, D.Habs, E.Hanelt, E.Kankeleit, B.Schwartz

Excited States in Neutron Deficient Even-Even Thorium Isotopes (218 ≤ A ≤ 222)

NUCLEAR REACTIONS 209Bi(14N, 5n), E=91 MeV; 208Pb(16O, 4n), E=94 MeV; 208Pb(18O, 4n), E=95 MeV; measured I(ce), αγ-coin, γ(θ). 220,222,218Th deduced levels, J, π, γ-branching, γ-multipolarity, T1/2, B(λ).

doi: 10.1007/BF01412018
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1985DA11      Z.Phys. A321, 535 (1985)

M.Dahlinger, E.Hanelt, E.Kankeleit, B.Schwartz, D.Schwalm, D.Habs, R.S.Simon, H.Backe

Spectroscopy of 221Th

NUCLEAR REACTIONS 208Pb(16O, 3n), E=84.5, 86, 87 MeV; measured Eγ, Iγ, γγ-coin, recoil. 221Th deduced levels, γ-branching, possible J, π, band structure, E1, E2 transitions, < B(E1)/B(E2) >.

doi: 10.1007/BF01411991
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1985KO17      Phys.Rev.Lett. 55, 588 (1985)

D.Konnerth, W.Dunnweber, W.Hering, W.Trautmann, W.Trombik, W.Zipper, D.Habs, W.Hennerici, H.J.Hennrich, R.Kroth, A.Lazzarini, R.Repnow, V.Metag, R.S.Simon

Correlated Spin Orientations in 12C + 12C Molecular Resonances

NUCLEAR REACTIONS, ICPND 12C(12C, 12C'), E(cm)=20-35 MeV; measured (particle)γ-, (particle)(particle)-coin, spin aligned reaction σ(θ); deduced σ(E).

doi: 10.1103/PhysRevLett.55.588
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1984LA22      Phys.Rev.Lett. 53, 1045 (1984)

A.Lazzarini, D.Habs, W.Hennerici, R.Kroth, J.Schirmer, V.Metag

Determination of a Time Scale for the Emission of High-Energy Photons in Heavy-Ion Fusion Reactions

NUCLEAR REACTIONS 58Ni(16O, X), E(cm)=60 MeV; measured γ(charged particle)-coin, particle multiplicity vs Eγ, γ-multiplicity; deduced compound system high energy photon decay time.

doi: 10.1103/PhysRevLett.53.1045
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