NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = K.Rudolph Found 37 matches. 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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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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