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NSR database version of April 26, 2024.

Search: Author = K.Rudolph

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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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1395.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2004JE08      Nucl.Phys. A738, 511 (2004)

H.Jeppesen, F.Ames, U.C.Bergmann, M.J.G.Borge, J.Cederkall, S.Emhofer, L.M.Fraile, H.O.U.Fynbo, S.Henry, H.T.Johansson, B.Jonson, M.Meister, T.Nilsson, G.Nyman, M.Pantea, K.Riisager, A.Richter, K.Rudolph, G.Schrieder, T.Siebert, O.Tengblad, E.Tengborn, M.Turrion, R.von Hahn, F.Wenander, B.Wolf, and the ISOLDE and REX-ISOLDE Collaborations

Experimental investigation of the 9Li + d reaction at REX-ISOLDE

NUCLEAR REACTIONS 2H(9Li, p), E=2.36 MeV/nucleon; measured excitation energy spectrum. 10Li deduced excited state.

doi: 10.1016/j.nuclphysa.2004.04.099
Citations: PlumX Metrics


2002SI16      Nucl.Phys. A701, 23c (2002)

C.Signorini, A.Andrighetto, J.Y.Guo, M.Ruan, L.Stroe, F.Soramel, K.E.G.Lobner, L.Muller, D.Pierroutsakou, M.Romoli, K.Rudolph, I.Thompson, M.Trotta, A.Vitturi

The Potential of the Loosely Bound 9Be from 209Bi Elastic Scattering: Unusual behaviour at near threshold energy

NUCLEAR REACTIONS 209Bi(9Be, 9Be), (9Be, 9Be'), E=40, 42, 44, 46, 48 MeV; measured σ(θ); deduced Woods-Saxon potential parameters.

doi: 10.1016/S0375-9474(01)01541-X
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0176.


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
Citations: PlumX Metrics


2000SI19      Phys.Rev. C61, 061603 (2000)

C.Signorini, A.Andrighetto, M.Ruan, J.Y.Guo, L.Stroe, F.Soramel, K.E.G.Lobner, L.Muller, D.Pierroutsakou, M.Romoli, K.Rudolph, I.J.Thompson, M.Trotta, A.Vitturi, R.Gernhauser, A.Kastenmuller

Unusual Near-Threshold Potential Behavior for the Weakly Bound Nucleus 9Be in Elastic Scattering from 209Bi

NUCLEAR REACTIONS 209Bi(9Be, 9Be), E=40-48 MeV; measured σ(θ); deduced optical model parameters, possible coupling to excited states. 209Bi(9Be, 9Be'), E=48 MeV; measured σ(E, θ).

doi: 10.1103/PhysRevC.61.061603
Citations: PlumX Metrics


1999SI06      Eur.Phys.J. A 5, 7 (1999)

C.Signorini, Z.H.Liu, Z.C.Li, K.E.G.Lobner, L.Muller, M.Ruan, K.Rudolph, F.Soramel, C.Zotti, A.Andrighetto, L.Stroe, A.Vitturi, H.Q.Zhang

Does Break-Up Affect 9Be + 209Bi Fusion at the Barrier ?

NUCLEAR REACTIONS 209Bi(9Be, X), E=36-50 MeV; measured α spectra from resuduals decay; deduced fusion σ, barrier parameters, break-up process effects. Coupled channels calculations.

doi: 10.1007/s100500050250
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0683.


1998MO16      Phys.Rev. C58, 739 (1998)

M.Moralles, P.Janker, H.Leitz, K.E.G.Lobner, K.Rudolph, F.J.Schindler, H.-G.Thies, T.Winkelmann, P.R.Pascholati, B.A.Brown

γ-Ray Spectroscopy of 42K and 43K

NUCLEAR REACTIONS 9Be(36S, 2np), (36S, np), E=90, 100, 110 MeV; measured Eγ, Iγ, γγ-, pγ-, (recoil)γ-coin. 42,43K deduced levels, possible J, π.

NUCLEAR STRUCTURE 42,43K; calculated levels, J, π. Shell model.

doi: 10.1103/PhysRevC.58.739
Citations: PlumX Metrics


1998SI16      Eur.Phys.J. A 2, 227 (1998)

C.Signorini, Z.H.Liu, A.Yoshida, T.Fukuda, Z.C.Li, K.E.G.Lobner, L.Muller, Y.H.Pu, K.Rudolph, F.Soramel, C.Zotti, J.L.Sida

Fusion Around the Barrier in 11, 9Be + 209Bi

NUCLEAR REACTIONS 209Bi(9Be, X), E=37.5-45.0 MeV; measured fusion σ. 209Bi(11Be, X), E(cm) ≈ 36-50 MeV; analyzed fusion σ; deduced halo related effects. Coupled channels calculations.

doi: 10.1007/s100500050111
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0564.


1998SI38      Nuovo Cim. 111A, 917 (1998)

C.Signorini, Z.H.Liu, A.Yoshida, T.Fukuda, Z.C.Li, K.E.G.Lobner, L.Muller, Y.H.Pu, K.Rudolph, F.Soramel, C.Zotti, A.Andrighetto, J.L.Sida

Fusion Cross-Sections Around the Barrier in 11, 9Be + 209Bi

NUCLEAR REACTIONS 209Bi(9Be, X), (11Be, X), E(cm)=35-50 MeV; measured fusion σ; deduced barrier distributions. Comparison with model predictions.

doi: 10.1007/BF03035978
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1996SC18      Nucl.Phys. A603, 77 (1996)

F.J.Schindler, C.V.K.Baba, T.Beha, S.Issmer, Th.Kerscher, H.Leitz, K.E.G.Lobner, M.Moralles, K.Rudolph, H.-G.Thies, C.Zotti

Semiclassical Description of Transfer Reactions at Near-Barrier Energies for the Systems 32S + 102,104Ru

NUCLEAR REACTIONS 102,104Ru(32S, X), E=106-130 MeV; measured transfer, σ(θ); deduced slope anomalies, transfer form factors, fusion σ(E), barrier distributions. Semi-classical coupled-channels approximation.

doi: 10.1016/0375-9474(96)00104-2
Citations: PlumX Metrics


1994GA06      Nucl.Phys. A569, 603 (1994)

E.N.Gazis, R.Vlastou, C.T.Papadopoulos, A.E.Aravantinos, E.Adamides, A.C.Xenoulis, U.Lenz, K.E.G.Lobner, K.Rudolph, S.J.Skorka, H.G.Thies

Investigation on Some 16O + 12C Resonances by the pn to d Competition Ratio Technique

NUCLEAR REACTIONS 12C(16O, np), (16O, d), E=26-31, 44-48 MeV; measured relative σ(E) for pn-, d-emission; calculated relative σ(E) for pn-, d-emission.

doi: 10.1016/0375-9474(94)90321-2
Citations: PlumX Metrics


1993CO11      Z.Phys. A346, 217 (1993)

L.Corradi, S.J.Skorka, T.Winkelmann, K.Balog, P.Janker, H.Leitz, U.Lenz, K.E.G.Lobner, K.Rudolph, M.Steinmayer, H.G.Thies, B.Million, D.R.Napoli, A.M.Stefanini, S.Beghini, G.Montagnoli, F.Scarlassara, C.Signorini, F.Soramel

Correlations between Nucleon Transfer and Fusion at Near-Barrier Energies for the Systems 32S + 100,101Ru and 33S + 90,91,92Zr

NUCLEAR REACTIONS 100,101Ru(32S, 32S), (32S, 32S'), (32S, X), E=118, 127 MeV; measured σ(θ), fragment mass spectra. 90,91,92Zr(33S, X), E=112 MeV; analyzed transfer reaction σ(θ), fusion σ(E); deduced multi-nucleon transfer dominance. Coupled-channels formalism.

doi: 10.1007/BF01306082
Citations: PlumX Metrics


1992ST05      Z.Phys. A341, 145 (1992)

M.Steinmayer, K.E.G.Lobner, L.Corradi, U.Lenz, U.Quade, P.R.Pascholati, K.Rudolph, W.Schomburg

Fission and Gamma-Ray Decay of the 238U Shape Isomer

RADIOACTIVITY 238mU [from 238U(d, np), E=18 MeV]; measured γ(ce)-coin; deduced delayed fission T1/2. 238U deduced transitions.

doi: 10.1007/BF01298474
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1990CO06      Z.Phys. A335, 55 (1990)

L.Corradi, S.J.Skorka, U.Lenz, K.E.G.Lobner, P.R.Pascholati, U.Quade, K.Rudolph, W.Schomburg, M.Steinmayer, H.G.Thies, G.Montagnoli, D.R.Napoli, A.M.Stefanini, A.Tivelli, S.Beghini, F.Scarlassara, C.Signorini, F.Soramel

Near-Barrier Transfer and Fusion of the Systems 33S + 90,91,92Zr

NUCLEAR REACTIONS, ICPND 90,91,92Zr(33S, X), E=110.6-118.7 MeV; measured σ(fragment θ, E), fragment mass spectra; deduced reaction, fusion σ.


1990MA49      Nucl.Phys. A515, 433 (1990)

G.Martinez, G.Barreau, A.Sicre, T.P.Doan, P.Audouard, B.Leroux, W.Arafa, R.Brissot, J.P.Bocquet, H.Faust, P.Koczon, M.Mutterer, F.Gonnenwein, M.Asghar, U.Quade, K.Rudolph, D.Engelhardt, E.Piasecki

Mass and Nuclear Charge Yields for 237Np(2n(th), f) at Different Fission Fragment Kinetic Energies

NUCLEAR REACTIONS 239Np(n, F), E=thermal; measured light fission product mass versus kinetic energies; deduced fractional independent fission yields, odd-even effects of elements, isotones. Double neutron capture on 237Np target.

doi: 10.1016/0375-9474(90)90593-B
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22179.


1990ST29      Z.Phys. A337, 371 (1990)

M.Steinmayer, K.E.G.Lobner, L.Corradi, U.Lenz, P.R.Pascholati, U.Quade, K.Rudolph, W.K.Schomburg, S.J.Skorka

Isomeric State at 945.3 keV in 237Np

NUCLEAR REACTIONS 238U(p, 2n), E=12.6 MeV; measured γ(electron)-coin, γ(electron)(t). 237Np deduced isomer, T1/2, decay, J, π, configuration, transitions γ-multipolarity, hindrance factors.


1989DJ01      Nucl.Phys. A496, 346 (1989)

M.Djebara, M.Asghar, J.P.Bocquet, R.Brissot, J.Crancon, Ch.Ristori, E.Aker, D.Engelhardt, J.Gindler, B.D.Wilkins, U.Quade, K.Rudolph

Mass and Nuclear-Charge Yields for 249Cf(n(th), F) at Different Fission-Product Kinetic Energies

NUCLEAR REACTIONS 249Cf(n, F), E=thermal; measured light fission product mass, nuclear-charge distributions vs kinetic energies; deduced fractional independent yields, odd-even effects, mean kinetic energies of masses, elements and isotones.

doi: 10.1016/0375-9474(89)90179-6
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22116.


1988QU05      Nucl.Phys. A487, 1 (1988)

U.Quade, K.Rudolph, S.Skorka, P.Armbruster, H.-G.Clerc, W.Lang, M.Mutterer, C.Schmitt, J.P.Theobald, F.Gonnenwein, J.Pannicke, H.Schrader, G.Siegert, D.Engelhardt

Nuclide Yields of Light Fission Products from Thermal-Neutron Induced Fission of 233U at Differenct Kinetic Energies

NUCLEAR REACTIONS, Fission 233U(n, F), E=thermal; measured fission fragment mass, nuclear charge distributions vs kinetic energy; deduced independent, fractional independent yields, odd-even effects, average kinetic energies of the elements, reaction Q.

doi: 10.1016/0375-9474(88)90127-3
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22130.


1987LO10      Nucl.Instrum.Methods Phys.Res. B26, 301 (1987)

K.E.G.Lobner, U.Lenz, U.Quade, K.Rudolph, W.Schomburg, S.J.Skorka, M.Steinmayer

Munich High-Frequency Recoil Spectrometer

NUCLEAR REACTIONS 24Mg(58Ni, X)76Rb/77Rb/79Rb/77Sr/79Sr/80Sr/76Kr/78Kr/79Y/80Y/80Zr, E=177 MeV; measured residue production σ. Recoil spectrometer.

doi: 10.1016/0168-583X(87)90767-1
Citations: PlumX Metrics


1986CL02      Nucl.Phys. A452, 277 (1986)

H.-G.Clerc, W.Lang, M.Mutterer, C.Schmitt, J.P.Theobald, U.Quade, K.Rudolph, P.Armbruster, F.Gonnenwein, H.Schrader, D.Engelhardt

Cold Fragmentation in Thermal-Neutron-Induced Fission of 233U and 235U

NUCLEAR REACTIONS 233,235U(n, F), E=thermal; measured light fission product mass yields at high kinetic energies; deduced influence of nucleon pairing, reaction Q.

doi: 10.1016/0375-9474(86)90310-6
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22030.


1984SK03      Nuovo Cim. 81A, 331 (1984)

S.J.Skorka, D.Evers, K.E.G.Lobner, R.Pengo, U.Quade, K.Rudolph, I.Weidl

Experiments with the Munich Recoil Spectrometer

NUCLEAR REACTIONS, ICPND 100,98,96,94,92Mo(32S, X), (36S, X), E(cm) ≈ 74-90 MeV; measured fusion σ(E). 12C(16O, p), E(cm)=19-26 MeV; measured σ(Ep), σ(θ) vs E. 27Al deduced high-spin state decay characteristics. Recoil spectrometer.

doi: 10.1007/BF02724173
Citations: PlumX Metrics


1984WE16      Z.Phys. A319, 67 (1984)

I.Weidl, D.Evers, P.Konrad, K.E.G.Lobner, U.Quade, K.Rudolph, S.J.Skorka

Properties of Unbound High-Spin States in 27Al

NUCLEAR REACTIONS 12C(16O, p), E(cm)=18.7-30.1 MeV; measured σ(Ep), σ(θ) vs E, recoil velocity spectra. 27Al deduced resonances, J, π, α-, γ-, n-branching ratios, shape characteristics, (Γγ/Γ), (Γn/Γ).

doi: 10.1007/BF01429769
Citations: PlumX Metrics


1983PE19      Nucl.Phys. A411, 255 (1983)

R.Pengo, D.Everts, K.E.G.Lobner, U.Quade, K.Rudolph, S.J.Skorka, I.Weidl

Nuclear Structure Effects in Sub-Barrier Fusion Cross Sections

NUCLEAR REACTIONS, ICPND 92,94,96,98,100Mo, 100,101,102,104Ru, 103Rh, 104,105,106,110Pd(32S, X), (36S, X), E=72-93 MeV; measured evaporation residues; deduced fusion σ(E) around, below Coulomb barrier, zero-point motion, two-neutron transfer reaction role. Enriched targets, heavy ion recoil spectrometer.

doi: 10.1016/0375-9474(83)90392-5
Citations: PlumX Metrics


1983RU01      Nucl.Instrum.Methods 204, 407 (1983)

K.Rudolph, D.Evers, P.Konrad, K.E.G.Lobner, U.Quade, S.J.Skorka, I.Weidl

The Munich RF-Recoil Spectrometer for the Observation of Heavy-Ion Reaction Products at Zero Degree

NUCLEAR REACTIONS 12C(16O, X), E=53.6 MeV; measured σ(fragment) vs Z, σ(fragment) vs mass for Mg isotopes, (24Mg)(α)-coin; 12C(16O, p), (16O, pn), E=53.6 MeV; measured residual nuclei recoils. 104Ru(36S, X), E=100 MeV; measured evaporation residue transmission. RF recoil spectrometer.

doi: 10.1016/0167-5087(83)90069-8
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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


1976HI13      Nucl.Phys. A266, 253 (1976)

P.Hille, K.Rudolph, M.Hille, P.Sperr, W.Mannhart, H.Munzer, G.Gaul

Fusion Reaction of 35Cl + 48Ti at 104 MeV

NUCLEAR REACTIONS 48Ti(35Cl, X), E=104 MeV; measured total fusion σ(θ), mass distribution. Enriched target.

doi: 10.1016/0375-9474(76)90293-1
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
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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
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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
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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
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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
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