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NSR database version of April 11, 2024.

Search: Author = W.Assmann

Found 16 matches.

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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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2003KA15      Eur.Phys.J. A 17, 49 (2003)

S.A.Karamian, J.S.Forster, J.U.Andersen, W.Assmann, C.Broude, J.Chevallier, J.S.Geiger, F.Gruner, V.A.Khodyrev, F.Malaguti, A.Uguzzoni

Fission lifetimes of Th nuclei measured by crystal blocking

NUCLEAR REACTIONS W(32S, 32S), (32S, F), E=170-180 MeV; measured scattered particle and fission fragment spectra, blocking pattern due to target crystal; deduced fission lifetime features. 214Th calculated compound nucleus T1/2, fission probability vs energy, spin. Crystal blocking technique.

doi: 10.1140/epja/i2002-10139-0
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1995GR25      Nucl.Instrum.Methods Phys.Res. B101, 422 (1995)

U.Grabowy, H.Busch, A.Gohla, K.-H.Speidel, S.Kremeyer, G.Jakob, K.Freitag, J.Gerber, W.Assmann

Preparation and Analysis of Targets with Implanted Thick Ar Layers for In-Beam γ-Spectroscopy

NUCLEAR REACTIONS 40Ar(62Ni, 62Ni'), E=150 MeV; measured Eγ, Iγ following target Coulomb excitation; deduced Ar content of target. Implantation of 40Ar ions in thick Fe layers.

doi: 10.1016/0168-583X(95)00558-7
Citations: PlumX Metrics

1994AS03      Nucl.Instrum.Methods Phys.Res. B85, 726 (1994)

W.Assmann, P.Hartung, H.Huber, P.Staat, H.Steffens, Ch.Steinhausen

Setup for Materials Analysis with Heavy Ion Beams at the Munich MP Tandem

NUCLEAR REACTIONS 89Y, Ba, Cu, O(16O, 16O), E=30 MeV; measured Rutherford backscattering spectra; deduced material analysis possibilities. Multi-layer YBaCuO target.

doi: 10.1016/0168-583X(94)95911-0
Citations: PlumX Metrics

1990DU04      Phys.Rev.Lett. 65, 297 (1990)

W.Dunnweber, W.Lippich, D.Otten, W.Assmann, K.Hartmann, W.Hering, D.Konnerth, W.Trombik

Quantum-Statistical Interference of Coincident Neutrons from the Compound Nucleus

NUCLEAR REACTIONS 26Mg(18O, xn), E=65, 88 MeV; measured nn-coin yields; deduced 44Ca evaporation chain average Γ.

doi: 10.1103/PhysRevLett.65.297
Citations: PlumX Metrics

1978EV03      Fizika, Suppl. 10, 5 (1978)

D.Evers, W.Assmann, J.Ehrenberg, P.Konrad, K.E.G.Lobner

Evidence for a Non-Statistical Population of High Spin States in 24Mg Via the 12C(13C, n) Reaction

NUCLEAR REACTIONS 12C(13C, n), E(cm)=14.08-15.26 MeV; measured σ(θ). 24Mg levels deduced evidence for non-statistical population mechanism. DWBA, Hauser-Feshbach analysis.

1977EV01      Nucl.Phys. A275, 363 (1977)

D.Evers, C.Ley, E.Spindler, W.Assmann, K.Rudolph, P.Konrad, P.Sperr

The (3He, n) Reaction on 16O and 18O

NUCLEAR REACTIONS 16O(3He, n), E=15, 18, 21 MeV; 18O(3He, n), E=18 MeV; measured σ(θ, En). 18,20Ne deduced levels, J, π. Natural 16O, enriched 18O targets.

doi: 10.1016/0375-9474(77)90458-4
Citations: PlumX Metrics

1977EV02      Z.Phys. A280, 287 (1977)

D.Evers, G.Denhofer, W.Assmann, A.Harasim, P.Konrad, C.Ley, K.Rudolph, P.Sperr

Investigation of High Spin States in 23Na and 23Mg and the 12C + 12C Resonance at E(c.m.) = 19.3 MeV

NUCLEAR REACTIONS 12C(12C, nγ), (12C, pγ), (12C, np), E=19.3 MeV; measured particle γ-coin, DSA. 23Na, 23Mg levels deduced T1/2, J, π. 23Mg deduced resonances, proton branching.

doi: 10.1007/BF01434357
Citations: PlumX Metrics

1977EV03      Phys.Rev. C15, 1690 (1977)

D.Evers, A.Harasim, R.L.McGrath, W.Assmann

Gamma Spectroscopy of 52Fe, 52Mn, and 52Cr from α + 50Cr Reactions

NUCLEAR REACTIONS 50Cr(α, X), E=23.5, 27.2 MeV; measured relative σ(Eγ), particle-γ triple coin, γγ-coin. 52Cr, 52Mn, 52Fe deduced levels, J, π. 49V, 50Cr, 53Mn, 54Fe deduced transitions. Enriched target.

doi: 10.1103/PhysRevC.15.1690
Citations: PlumX Metrics

1975SP05      Phys.Lett. 57B, 438 (1975)

P.Sperr, D.Evers, A.Harasim, W.Assmann, P.Konrad, K.Rudolph, G.Denhoefer, C.Ley

The Neutron Decay of the Resonance in the 12C + 16O System at E(c.m.) = 19.7 MeV

NUCLEAR REACTIONS 12C(16O, n), E=19.39, 19.70, 20.6, 22.0, 22.6 MeV; measured σ(E, En, θ). 28Si deduced resonances.

doi: 10.1016/0370-2693(75)90262-2
Citations: PlumX Metrics

1974EV02      Nucl.Phys. A230, 109 (1974)

D.Evers, W.Assmann, K.Rudolph, S.J.Skorka, P.Sperr

The (3He, n) Reaction on Even (f, p) Shell Nuclei at 15, 18 and 21 MeV (II)

NUCLEAR REACTIONS 40,42,44,48Ca, 46,48,50Ti, 58,60Ni, 64Zn, 50,52,54Cr, 54Fe(3He, n), E=15, 18, 21 MeV; measured σ(θ, En). 42,44,46,50Ti, 48,50,52Cr, 60,62Zn, 66Ge, 52,54,56Fe, 56Ni deduced levels, J, π. Enriched targets.

doi: 10.1016/0375-9474(74)90533-8
Citations: PlumX Metrics

1974HI06      Nucl.Phys. A232, 157 (1974)

P.Hille, P.Sperr, M.Hille, K.Rudolph, W.Assmann, D.Evers

Spin Dependence of the Nuclear Level Density from Angular Distributions of (α, n) Reactions

NUCLEAR REACTIONS 46Ti, 54,56Fe, 58,60,62Ni, 90Zr, 93Nb, 92Mo, 115In(α, n), E approx 15.3 MeV; 59Co(α, n), E=14.0 MeV; measured σ(En, θ). 49Cr, 57,59Ni, 62Cu, 61,63,65Zn, 93Mo, 96Tc, 95Ru, 118Sb deduced spin cut-off factors. Isotopically separated, natural targets.

doi: 10.1016/0375-9474(74)90650-2
Citations: PlumX Metrics

1974SP03      Phys.Lett. 49B, 345 (1974)

P.Sperr, D.Evers, K.Rudolph, W.Assmann, E.Spindler, P.Konrad, G.Denhofer

Study of the 12C(12C, n)23Mg Reaction Around the Resonance at E(cm) = 19.3 MeV

NUCLEAR REACTIONS 12C(12C, n), E(cm)=19.3 MeV; measured σ(Eγ, En, θ(n)), nγ-coin. 23Mg deduced levels. 24Mg deduced resonance.

doi: 10.1016/0370-2693(74)90177-4
Citations: PlumX Metrics

1972EV02      Nucl.Phys. A198, 268 (1972)

D.Evers, W.Assmann, K.Rudolph, S.J.Skorka, P.Sperr

The (3He, n) Reaction on Even (f, p) Shell Nuclei at 18 and 21 MeV (I)

NUCLEAR REACTIONS 50,52,54Cr, 54,56,58Fe(3He, n), E(3He)=18, 21 MeV; measured σ(θ, En). 52,54,56Fe, 56,58,60Ni deduced levels, J, π. Enriched targets.

doi: 10.1016/0375-9474(72)90784-1
Citations: PlumX Metrics

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