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NSR database version of April 11, 2024.

Search: Author = T.Weber

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2008MA33      Bull.Rus.Acad.Sci.Phys. 72, 806 (2008)

A.I.Mazur, A.M.Shirokov, J.P.Vary, T.A.Weber, E.A.Mazur

Charge-dependent NN interaction in the J-matrix inverse scattering approach

doi: 10.3103/S1062873808060208
Citations: PlumX Metrics


2008SH16      Phys.Atomic Nuclei 71, 1232 (2008); Yad.Fiz. 71, 1260 (2008)

A.M.Shirokov, J.P.Vary, A.I.Mazur, T.A.Weber

Spectroscopy of light nuclei with realistic NN interaction JISP

NUCLEAR STRUCTURE 3H, 3,4,6He, 6,7Li, 7,8,9,10Be, 9,10,11,12,13B, 10,11,12,13,14C, 12,13,14,15N, 13,14,15,16O; calculated binding energies using bare and effective interaction; 6Li, 10B; calculated rms radii, ground state quadrupole moments, ground and excited state energies; 10B; calculated B(E2) and B(GT) transition strengths; microscopic no-core shell model; realistic NN interaction.

doi: 10.1134/S1063778808070168
Citations: PlumX Metrics


2007BO39      At.Data Nucl.Data Tables 93, 831 (2007)

J.B.Boffard, B.Chiaro, T.Weber, C.C.Lin

Electron-impact excitation of argon: Optical emission cross sections in the range of 300-2500 nm

ATOMIC PHYSICS Ar(e, e'), E=25, 50, 100 eV; measured cross sections and excitation functions.

doi: 10.1016/j.adt.2007.06.004
Citations: PlumX Metrics


2007MA49      Bull.Rus.Acad.Sci.Phys. 71, 754 (2007); Izv.Akad.Nauk RAS, Ser.Fiz. 71, 781 (2007)

A.I.Mazur, A.M.Shirokov, J.P.Vary, T.A.Weber, S.A.Zaitsev, E.A.Mazur

Nonlocal nucleon-nucleon interaction JISP

doi: 10.3103/S1062873807060020
Citations: PlumX Metrics


2007SH27      Bull.Rus.Acad.Sci.Phys. 71, 764 (2007); Izv.Akad.Nauk RAS, Ser.Fiz. 71, 791 (2007)

A.M.Shirokov, J.P.Vary, A.I.Mazur, T.A.Weber

Nonlocal inverse-scattering nucleon-nucleon interaction and spectra of s- and p-shell nuclei

NUCLEAR STRUCTURE H, He, Li, Be, B, C, N, O; calculated binding energies using no-core shell-model.

doi: 10.3103/S1062873807060032
Citations: PlumX Metrics


2007SH52      Phys.Lett. B 644, 33 (2007)

A.M.Shirokov, J.P.Vary, A.I.Mazur, T.A.Weber

Realistic nuclear Hamiltonian: Ab exitu approach

NUCLEAR STRUCTURE 3H, 3,4He, 6He, 6,7Li, 7,8,9,10Be, 9,10,11,12B, 10,11,12,13,14C, 12,13,14,15N, 13,14,15,16O; calculated binding energies with bare JISP16 and effective interaction generated by JISP16, ground and excitation energies. Fully-microscopic no-core shell model (NCSM).

doi: 10.1016/j.physletb.2006.10.066
Citations: PlumX Metrics


2006EL07      Eur.Phys.J. A 28, Supplement 1, 197 (2006)

M.El-Ghazaly, H.Backe, W.Lauth, G.Kube, P.Kunz, A.Sharafutdinov, T.Weber

X-ray phase contrast imaging at MAMI

doi: 10.1140/epja/i2006-09-021-6
Citations: PlumX Metrics


2006LA21      Eur.Phys.J. A 28, Supplement 1, 185 (2006)

W.Lauth, H.Backe, O.Kettig, P.Kunz, A.Sharafutdinov, T.Weber

Coherent X-rays at MAMI

doi: 10.1140/epja/i2006-09-019-0
Citations: PlumX Metrics


2005SH31      Phys.Lett. B 621, 96 (2005)

A.M.Shirokov, J.P.Vary, A.I.Mazur, S.A.Zaytsev, T.A.Weber

Novel NN interaction and the spectroscopy of light nuclei

NUCLEAR STRUCTURE 2H; calculated binding energy, radius, quadrupole moment. 3H, 3,4,6He, 6Li; calculated binding energies. 6He, 6Li; calculated excited states energies, radii, quadrupole moments. Inverse scattering potential.

doi: 10.1016/j.physletb.2005.06.043
Citations: PlumX Metrics


2005SH33      J.Phys.(London) G31, S1283 (2005)

A.M.Shirokov, J.P.Vary, A.I.Mazur, S.A.Zaytsev, T.A.Weber

NN potentials from the J-matrix inverse scattering approach

NUCLEAR STRUCTURE 2,3H, 3,4,6He, 6Li; calculated binding energies. 2H calculated radius, D-state probability. 6He, 6Li; calculated excited states energies, radii, quadrupole moments.

doi: 10.1088/0954-3899/31/8/006
Citations: PlumX Metrics


2005VA32      Eur.Phys.J. A 25, Supplement 1, 475 (2005)

J.P.Vary, O.V.Atramentov, B.R.Barrett, M.Hasan, A.C.Hayes, R.Lloyd, A.I.Mazur, P.Navratil, A.G.Negoita, A.Nogga, W.E.Ormand, S.Popescu, B.Shehadeh, A.M.Shirokov, J.R.Spence, I.Stetcu, S.Stoica, T.A.Weber, S.A.Zaytsev

Ab initio No-Core Shell Model -- Recent results and future prospects

NUCLEAR STRUCTURE 4He; calculated radius. 6Li, 16O, 48Ar, 48K, 48Ca, 48Sc, 48Ti, 48V, 48Cr, 48Mn; calculated ground-state energies. 16O, 47Ca; calculated excited states energies. No-core shell model.

doi: 10.1140/epjad/i2005-06-214-x
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2004SC25      Nucl.Phys. A737, 306 (2004)

H.Schmidt-Bocking, R.Dorner, O.Jagutzki, T.Jahnke, V.Mergel, L.Ph.H.Schmidt, Th.Weber, A.Czasch, Ch.Wimmer, M.Hattass, A.Knapp, M.Schoffler, C.L.Cocke, M.Prior, A.Kheifets, E.Weigold, F.Afaneh

Many-particle dynamics in atomic and molecular physics investigated with the COLTRIMS-technique: New inside into e-e- correlation

doi: 10.1016/j.nuclphysa.2004.03.093
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2004SH41      Phys.Rev. C 70, 044005 (2004)

A.M.Shirokov, A.I.Mazur, S.A.Zaytsev, J.P.Vary, T.A.Weber

Nucleon-nucleon interaction in the J-matrix inverse scattering approach and few-nucleon systems

NUCLEAR REACTIONS 1H(n, n), E=0-350 MeV; calculated phase shifts. No-core shell model, J-matrix version of inverse scattering theory.

NUCLEAR STRUCTURE 2,3H, 4He; calculated ground-state energies, radii. 4He calculated excited states energies. No-core shell model, J-matrix version of inverse scattering theory.

doi: 10.1103/PhysRevC.70.044005
Citations: PlumX Metrics


2002SH36      Bull.Rus.Acad.Sci.Phys. 65, 1709 (2002)

A.M.Shirokov, J.P.Vary, T.A.Weber, A.I.Mazur

Realistic NN-Interaction in Shell Model

NUCLEAR STRUCTURE 2H; calculated wave function. 3H, 4He; calculated ground-state energies vs model parameters. Phase-equivalent transformations.


2000GA03      Nucl.Phys. A662, 235 (2000)

P.E.Garrett, H.Baltzer, M.Bertschy, D.G.Burke, M.Deleze, S.Drissi, C.Gunther, J.Jolie, J.Kern, H.Lehmann, S.J.Mannanal, J.Manns, U.Muller, J.P.Vorlet, N.Warr, T.Weber

Nuclear Levels in 190Ir Studied with the 192Os(p, 3nγ) and 192Os(d, 4ne-) Reactions

NUCLEAR REACTIONS 192Os(p, 3n), E=18.6, 20.8, 24.2, 27.2, 31.1 MeV; measured Eγ, Iγ(t), γγ-coin. 192Os(d, 4n), E=27.8 MeV; measured E(ce), I(ce), e-e--coin. 190Ir deduced levels J, π, T1/2. Two-quasiparticle-rotor calculations. Enriched targets, Ge detectors, orange spectrometers.

NUCLEAR STRUCTURE 189Os, 190,191Ir; calculated levels, J, π. Particle-rotor calculations.

doi: 10.1016/S0375-9474(99)00365-6
Citations: PlumX Metrics

Data from this article have been entered in the XUNDL database. For more information, click here.


1999KH01      J.Phys.(London) B32, L73 (1999)

Kh.Khayyat, T.Weber, R.Dorner, M.Achler, V.Mergel, L.Spiedlberger, O.Jagutzki, U.Meyer, J.Ullrich, R.Moshammer, W.Schmitt, H.Knudsen, U.Mikkelsen, P.Aggerholm, E.Uggerhoej, S.P.Moeller, V.D.Rodriguez, S.F.C.O'Rourke, R.E.Olson, P.D.Fainstein, J.H.McGuire, H.Schmidt-Bocking

Differential Cross Sections in Antiproton- and Proton-Helium Collisions

ATOMIC PHYSICS 4He(p-bar, p-bar), (p, p), E ≈ 1 MeV; measured recoil momentum following ionization.

doi: 10.1088/0953-4075/32/4/002
Citations: PlumX Metrics


1999WU05      Acta Phys.Pol. B30, 1313 (1999)

M.Wurkner, J.De Boer, J.Choinski, T.Czosnyka, C.Droste, C.Gunther, J.Iwanicki, M.Kisielinski, A.Kordyasz, M.Kowalczyk, H.Kusakari, J.Kvasil, A.I.Levon, M.Loewe, P.J.Napiorkowski, T.Shizuma, G.Sletten, J.Srebrny, M.Sugawara, T.Weber, Y.Yoshizawa

Coulomb Excitation of 231Pa

NUCLEAR REACTIONS 231Pa(32S, 32S'), E=148 MeV; 231Pa(58Ni, 58Ni'), E=255, 260, 261 MeV; measured Eγ, Iγ(θ), (particle)γγ-coin following Coulomb excitation. 231Pa deduced high-spin levels, J, π. Nordball array.


1998MA83      Eur.Phys.J. A 3, 263 (1998)

J.Manns, J.Groger, C.Gunther, U.Muller, T.Weber, J.de Boer

Study of 227Th in the 226Ra(α, 3n) Reaction

NUCLEAR REACTIONS 226Ra(α, 3n), E=33 MeV; measured Eγ, Iγ, E(ce), I(ce), γγ-, (ce)γ-coin. 227Th deduced high-spin levels, J, π, rotational bands, B(E1)/B(E2).

doi: 10.1007/s100500050176
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Data from this article have been entered in the XUNDL database. For more information, click here.


1998WE01      Eur.Phys.J. A 1, 39 (1998)

T.Weber, J.Groger, C.Gunther, J.deBoer

Study of the First-Excited K(π) = 0+ and 2+ Bands in 228Th in the 226Ra(α, 2n) Reaction

NUCLEAR REACTIONS 226Ra(α, 2n), E=28 MeV; measured Eγ, Iγ, (ce)γ-coin. 228Th deduced high-spin levels, J, π, vibrational bands.

doi: 10.1007/s100500050029
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Data from this article have been entered in the XUNDL database. For more information, click here.


1998WE13      Eur.Phys.J. A 3, 25 (1998)

T.Weber, J.de Boer, K.Freitag, J.Groger, C.Gunther, P.Herzog, V.G.Soloviev, A.V.Sushkov, N.Yu.Shirikova

Nuclear Levels in 228Th Populated in the Decay of 228Pa (II)

RADIOACTIVITY 228Pa(EC); measured Eγ, Iγ, γγ-coin. 228Th deduced levels, J, π, δ, B(E2), rotational bands.

NUCLEAR STRUCTURE 228Th; calculated levels J, π, transition strengths. Quasiparticle-phonon model.

doi: 10.1007/s100500050146
Citations: PlumX Metrics

Data from this article have been entered in the XUNDL database. For more information, click here.


1997MU08      Phys.Rev. C55, 2267 (1997)

U.Muller, P.Sevenich, K.Freitag, C.Gunther, P.Herzog, G.D.Jones, C.Kliem, J.Manns, T.Weber, B.Will, and the ISOLDE Collaboration

Level Structure of 227Th Investigated in the α Decay of 231U

RADIOACTIVITY 231U(α) [from 232Th(α, 5n), E=53 MeV]; measured Eα, Iα, Eγ, Iγ. 227Ac(β-); 227Th(α) [from 227Ac(β-decay)]; 223Ra(α) [from 227Th(α-decay)]; measured αγ-coin, I(ce), Eα, Iα, oriented nuclei. 227Th deduced levels, J, π, γ-multipolarity, α hindrance factors, reduced transition rates, octupole deformation.

doi: 10.1103/PhysRevC.55.2267
Citations: PlumX Metrics


1997WE05      Z.Phys. A358, 281 (1997)

T.Weber, J.deBoer, K.Freitag, J.Groger, C.Gunther, J.Manns, U.Muller

Variety of Vibrational Excitations in 228Th

RADIOACTIVITY 228Pa(EC); measured γγ-coin. 228Th deduced levels, J, π, K, band structure, moments of inertia.

doi: 10.1007/s002180050330
Citations: PlumX Metrics


1996AC01      Z.Phys. A355, 151 (1996)

B.Ackermann, Ch.Fleischmann, H.Baltzer, J.de Boer, T.Czosnyka, C.Gunther, U.Muller, T.Weber

Investigation of Vibrational Levels in 226Ra by Coulomb Excitation and by the 226Ra(d, pnγ) Reaction

NUCLEAR REACTIONS 226Ra(d, np), E=27 MeV; measured γ(ce)-coin. 226Ra(16O, 16O'), E=63 MeV; 226Ra(32S, 32S'), E=135 MeV; measured γ(scattered particle)-coin following Coulomb excitation. 226Ra deduced levels, J, π, K, B(λ), ratios, band structure.

doi: 10.1007/s002180050092
Citations: PlumX Metrics


1996BA67      Z.Phys. A356, 13 (1996)

H.Baltzer, J.deBoer, A.Gollwitzer, G.Graw, C.Gunther, A.I.Levon, M.Loewe, H.J.Maier, J.Manns, U.Muller, B.D.Valnion, T.Weber, M.Wurkner

Study of Low-Lying 0+ Excitations in 228Th and 232,234,236U in the (p, t) Reaction

NUCLEAR REACTIONS 230,232Th, 234,236,238U(p, t), E=22 MeV; measured triton spectra; deduced relative σ. 228,230Th, 232,234,236U deduced levels, J, π, K.

doi: 10.1007/s002180050142
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0943.


1996GA30      Nucl.Phys. A611, 68 (1996)

P.E.Garrett, N.Warr, H.Baltzer, S.Boehmsdorff, D.G.Burke, M.Deleze, S.Drissi, J.Groger, C.Gunther, J.Kern, S.J.Mannanal, J.Manns, U.Muller, J.-P.Vorlet, T.Weber

Long-Lived Isomers in 190Ir

NUCLEAR REACTIONS 192Os(p, 3n), E=18.6-31.1 MeV; 192Os(d, 4n), E=27.8 MeV; measured Eγ, Iγ vs Ep, (e-e-)-, (eγ)-coin. 190Ir deduced isomers T1/2, J, π, ICC, γ multipolarity. Enriched targets, Ge detector, β-ray spectrometer.

RADIOACTIVITY 190mIr [from 192Os(p, 3n), E=18.6-31.1 MeV]; 192Os(d, 4n), E=27.8 MeV; measured Eγ, Iγ, I(ce), (e-e-)-, (e-γ)-coin, T1/2; deduced log ft. Enriched targets, Ge detector, β-ray spectrometer.

doi: 10.1016/S0375-9474(96)00330-2
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Data from this article have been entered in the XUNDL database. For more information, click here.


1996LE01      Nucl.Phys. A598, 11 (1996)

A.I.Levon, J.de Boer, G.Graw, J.Kvasil, M.Loewe, B.D.Valnion, M.Wurkner, H.Baltzer, C.Gunther, J.Manns, U.Muller, T.Weber

The Structure of the Parity-Doublet Bands in 231Pa

NUCLEAR REACTIONS 231Pa(d, d'), E=27 MeV; measured Ed. 231Pa(p, p'), E=11 MeV; measured Ep. 232Th(p, 2n), E=14 MeV; analyzed data. 231Pa(16O, 16O'), E=85 MeV; 231Pa(32S, 32S'), E=145 MeV; measured Eγ, Iγ following Coulomb excitation. 231Pa deduced levels, J, π, rotational bands, octupole correlations. Q3D magnetic spectrometer, Ge detectors.

RADIOACTIVITY 231U(EC); measured I(ce), (e-γ)-, (e-e-)-coin. 231Pa deduced levels, J, π, band structure, γ-multipolarity, γ-branching ratio. Orange spectrometers, Ge detectors, enriched radioactive targets, mass-separated radioactive sources.

doi: 10.1016/0375-9474(95)00508-0
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Data from this article have been entered in the XUNDL database. For more information, click here.


1995BA42      Z.Phys. A352, 47 (1995)

H.Baltzer, K.Freitag, C.Gunther, P.Herzog, J.Manns, U.Muller, R.Paulsen, P.Sevenich, T.Weber, B.Will

Nuclear Levels in 228Th Populated in the Decay of 228Pa

RADIOACTIVITY 228Pa(EC) [from 232Th(p, 5n), E=40 MeV]; measured Eγ, Iγ, (eγ)-coin, I(ce). 228Th deduced levels, J, π, K, band structure, Iγ, δ, B(λ) ratios, γ multipolarity. Low temperature source orientation.

doi: 10.1007/BF01292760
Citations: PlumX Metrics


1994AC02      Z.Phys. A350, 13 (1994)

B.Ackermann, H.Baltzer, K.Freitag, C.Gunther, P.Herzog, J.Manns, U.Muller, R.Paulsen, P.Sevenich, T.Weber, B.Will, J.de Boer, G.Graw, A.I.Levon, M.Loewe, A.Losch, E.Muller-Zanotti

Experimental Investigation of Vibrational Excitations in 230Th

RADIOACTIVITY 230Pa(β+), (EC), (β-) [from 232Th(p, 3n), E not given]; measured Eγ, Iγ, I(ce). 230Th levels deduced Iγ, γ-multipolarity.

NUCLEAR REACTIONS 230Th(d, np), E=23 MeV; measured (ce)(ce)-, γ(ce)-coin. 232Th(p, t), E=22 MeV; measured σ(θ). 230Th deduced levels, J, π, K, γ-multipolarity, B(λ), high-spin band structure.

doi: 10.1007/BF01285047
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0942.


1994BO27      Nucl.Instrum.Methods Phys.Res. B85, 188 (1994)

W.Bolse, T.Weber

Consequence of the Fractal Nature of the Collision Cascade: End-of-range spikes in ballistic systems

NUCLEAR REACTIONS Ti, N(α, α), E=900 keV; measured Rutherford backscattering spectra; deduced end of ion range spike formation features. Noble gas implantation of TiN on steel, Al.

doi: 10.1016/0168-583X(94)95811-4
Citations: PlumX Metrics


1994OS06      Nucl.Instrum.Methods Phys.Res. B85, 499 (1994)

T.Osipowicz, S.C.Liew, K.K.Loh, I.Orlic, S.M.Tang, Th.Weber

Reconstruction of Ar Depth Profiles from PIXE Measurements

NUCLEAR REACTIONS Ar(α, X), E=1.5, 1.3 MeV; measured X-ray yields, Ar implantation on Al samples; deduced Ar depth profiles reconstruction.

doi: 10.1016/0168-583X(94)95871-8
Citations: PlumX Metrics


1991WE03      Nucl.Phys. A522, 443 (1991)

Th.Weber, U.Kneissl, W.Pecho, A.Degener, K.Huber, K.Schaschek, W.Wilke

Fragment Angular Distributions in Electron- and Positron-Induced Fission of 232Th. A Specific Test of Virtual Photon Spectra

NUCLEAR REACTIONS 232Th(e, F), E=8-16 MeV; measured fission fragment σ(θ); deduced angular correlation coefficients, fission channels. Virtual photon spectra tests.

doi: 10.1016/0375-9474(91)90075-H
Citations: PlumX Metrics


1990HE03      Nucl.Phys. A506, 223 (1990)

R.D.Heil, B.Kasten, W.Scharfe, P.A.Butler, H.Friedrichs, S.D.Hoblit, U.Kneissl, S.Lindenstruth, M.Ludwig, G.Muller, H.H.Pitz, K.W.Rose, M.Schumacher, U.Seemann, J.Simpson, P.von Brentano, Th.Weber, C.Wesselborg, A.Zilges

Parity Assignments in Nuclear Resonance Fluorescence Experiments Using Compton Polarimeters

NUCLEAR REACTIONS 142,150Nd, 232Th(γ, γ'), E=4.1 MeV bremsstrahlung; measured Eγ, Iγ, asymmetry, linear polarization. 142,150Nd, 232Th deduced levels, J, π, Γ0, (Γ0)20.

doi: 10.1016/0375-9474(90)90384-X
Citations: PlumX Metrics


1990WE07      Nucl.Phys. A510, 1 (1990)

Th.Weber, R.D.Heil, U.Kneissl, W.Wilke, Th.Kihm, K.T.Knopfle, H.J.Emrich

(e, e'f) Coincidence Experiments on 235U and 238U

NUCLEAR REACTIONS 235,238U(e, e'F), E=78-183 MeV; measured σ(θ(e'), E, θ(fragment)), in-, out-of-plane fission fragment σ(θ), fragment time-of-flight differences. 235,238U deduced multipole strength distributions for giant E0, E1, E2, E3 resonances, fission characteristics.

doi: 10.1016/0375-9474(90)90286-U
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1990WI15      Phys.Rev. C42, 2148 (1990)

W.Wilke, U.Kneissl, Th.Weber, H.Stroher, L.S.Cardman, P.T.Debevec, S.D.Hoblit, R.T.Jones, A.M.Nathan

Photofission of 238U with Monochromatic Gamma Rays in the Energy Range 11-16 MeV

NUCLEAR REACTIONS 238U(γ, F), E=11-16 MeV; measured fission fragment σ(θ), fragment mass distributions; deduced anisotropy, fragment mass asymmetry relationship.

doi: 10.1103/PhysRevC.42.2148
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetL0252.


1989KA16      Phys.Rev.Lett. 63, 609 (1989); Erratum Phys.Rev.Lett. 63, 2695 (1989)

B.Kasten, R.D.Heil, P.v.Brentano, P.A.Butler, S.D.Hoblit, U.Kneissl, S.Lindenstruth, G.Muller, H.H.Pitz, K.W.Rose, W.Scharfe, M.Schumacher, U.Seemann, Th.Weber, C.Wesselborg, A.Zilges

Evidence for a Cluster of Collective 1+ States in 150Nd Near 3 MeV

NUCLEAR REACTIONS 150Nd(γ, γ'), E=2.8-3.1 MeV bremsstrahlung; measured Eγ, Iγ, γ linear polarization, asymmetry. 150Nd deduced levels, J, π, B(λ), (Γ02/Γ). Compton polarimeters.

doi: 10.1103/PhysRevLett.63.609
Citations: PlumX Metrics


1989WE01      Phys.Rev.Lett. 62, 129 (1989)

Th.Weber, R.D.Heil, U.Kneissl, W.Wilke, H.J.Emrich, Th.Kihm, K.T.Knopfle

Evidence for Different Mass Splits in Fission Decays of Giant Multipole Resonances from 235,238U(e, e'f) Reactions

NUCLEAR REACTIONS 235,238U(e, e'F), E=185 MeV; measured fission (fragment)(fragment)-coin. 235,238U deduced giant multipole resonance fission decay features, Γ(S)/Γ(A).

doi: 10.1103/PhysRevLett.62.129
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1989WE02      Phys.Rev.Lett. 62, 690 (1989)

Th.Weber, U.Kneissl, Th.Kihm, K.T.Knopfle

Weber et al. Reply

doi: 10.1103/PhysRevLett.62.690
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1989WE12      Nucl.Phys. A502, 279c (1989)

Th.Weber, W.Wilke, H.J.Emrich, R.D.Heil, Th.Kihm, U.Kneissl, K.T.Knopfle, U.Seemann, F.Steiper, H.Stroher

Evidence for Different Fission Fragment Mass Asymmetries for Specific Nuclear Excitations Studied in (e, e'F) and (γ, F) Reactions

NUCLEAR REACTIONS 236U(e, e'F), E not given; measured fission fragment σ(θ). 235,238U(e, e'F), E=185 MeV; measured fission fragment spectra; deduced symmetric, asymmetric fission yield ratios, excitation multipolarity role.

doi: 10.1016/0375-9474(89)90668-4
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1988WE18      Phys.Lett. 215B, 469 (1988)

Th.Weber, R.D.Heil, U.Kneissl, W.Wilke, H.J.Emrich, Th.Kihm, K.T.Knopfle

Near Barrier Fission Channels (J(π), K) in 238U for Spins J(π) = 0+, 1-, and 2+ from (e, e'f) Angular Correlation Measurements

NUCLEAR REACTIONS 238U(e, e'F), E=185 MeV; measured fission (fragment)(fragment)(θ), in-plane, out-of-plane; deduced partial fission channel σ. 238U levels deduced fission barriers.

doi: 10.1016/0370-2693(88)91343-3
Citations: PlumX Metrics


1988WI15      Phys.Lett. 207B, 385 (1988)

W.Wilke, R.D.Heil, U.Kneissl, U.Seemann, F.Steiper, H.Stroher, T.Weber

Angular Distributions of Photofission Fragments of Particular Mass

NUCLEAR REACTIONS 236U(γ, F), E=16 MeV bremsstrahlung; measured fission fragment σ(θ), mass distribution. 236U deduced fission mechanism.

doi: 10.1016/0370-2693(88)90669-7
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1988WI20      Nucl.Instrum.Methods Phys.Res. A272, 785 (1988)

W.Wilke, H.Bruckel, R.D.Heil, U.Kneissl, H.Stroher, Th.Weber

A 4π Double Obelisk of Position Sensitive PPACs for New Vistas in Photofission Experiments

NUCLEAR REACTIONS 238U(γ, F), E=5.6-16 MeV bremsstrahlung; measured fission fragment spectra, σ(θ), mass distribution. Position sensitive detectors, 4π array.

doi: 10.1016/0168-9002(88)90760-7
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1987WE09      Phys.Rev.Lett. 59, 2028 (1987)

Th.Weber, R.D.Heil, U.Kneissl, W.Pecho, W.Wilke, H.J.Emrich, Th.Kihm, K.T.Knopfle

Multipole Strength Distributions and Form Factors for E1, E2/E0, and E3 from 238U(e, e'f) Coincidence Experiments

NUCLEAR REACTIONS 238U(e, e'F), E=78, 183, 124 MeV; measured fission (fragment)(fragment)-coin. 238U deduced multipole strength distributions, form factors.

doi: 10.1103/PhysRevLett.59.2028
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1987WI15      Nucl.Phys. A473, 129 (1987)

Ch.Winter, B.Krusche, K.P.Lieb, T.Weber, G.Hlawatsch, T.von Egidy, F.Hoyler

Spectroscopy of 88Sr with the 87Sr(n, γ) and 87Sr(d, p) Reactions

NUCLEAR REACTIONS 87Sr(n, γ), E=thermal; measured Eγ, Iγ. 87Sr(d, p), E=20 MeV; measured σ(E(p)). 88Sr deduced levels, neutron binding energy, level density, γ transition strengths, branching ratios.

doi: 10.1016/0375-9474(87)90158-8
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1985DR01      Nucl.Phys. A437, 253 (1985)

J.Drexler, R.D.Heil, K.Huber, U.Kneissl, G.Mank, R.Ratzek, H.Ries, T.Weber, W.Wilke, B.Fischer, H.Hollick

The ' Isomeric Shelf ' in the Deep Subbarrier Photofission of 238U

NUCLEAR REACTIONS 238U(γ, F), E=3.9-4.3 MeV bremsstrahlung; measured T1/2, isomeric to prompt yield ratio. Depleted targets.

doi: 10.1016/0375-9474(85)90087-9
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1985HE21      Nucl.Instrum.Methods 239, 545 (1985)

R.D.Heil, J.Drexler, K.Huber, U.Kneissl, G.Mank, H.Ries, H.Stroher, T.Weber, W.Wilke

A Compact Time-of-Flight Spectrometer for Electrofission Studies

RADIOACTIVITY 252Cf(SF); measured fission fragment velocities, masses, energies before neutron emission.

doi: 10.1016/0168-9002(85)90034-8
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1984BE54      Phys.Lett. 149B, 59 (1984)

U.E.P.Berg, C.Blasing, J.Drexler, R.D.Heil, U.Kneissl, W.Naatz, R.Ratzek, S.Schennach, R.Stock, T.Weber, H.Wickert, B.Fischer, H.Hollick, D.Kollewe

Photoexcitation of Low-Lying Collective States in 156,158,160Gd

NUCLEAR REACTIONS 156,158,160Gd(γ, γ'), E=2.8-3.4 MeV bremsstrahlung; measured Eγ, Iγ. 156,158,160Gd levels deduced Γγ, B(M1), transition collectivity.

doi: 10.1016/0370-2693(84)91551-X
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1984CO06      Lett.Nuovo Cim. 39, 119 (1984)

B.C.Cook, T.A.Weber

An Analysis for the Charge and Point Proton Distribution of 3He with Minimal Systematic Error

NUCLEAR MOMENTS 3He(e, e), E not given; analyzed form factor data. 3He deduced charge, point proton distribution, method dependent error estimate.

doi: 10.1007/BF02800292
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1984DR04      Nucl.Instrum.Methods 220, 409 (1984)

J.Drexler, R.D.Fischer, R.Heil, K.Huber, U.Kneissl, G.Mank, R.Ratzek, H.Ries, H.Stroher, T.Weber, W.Wilke

Arrangements of Parallel Plate Avalanche Detectors for Electrofission and Photofission experiments

NUCLEAR REACTIONS 232Th(e+, F), (e-, F), E=9 MeV; measured fission fragment σ(θ). Parallel plate avalanche detectors.

RADIOACTIVITY 252Cf(SF); measured fission fragment tof spectra. Parallel plate avalanche detectors.

doi: 10.1016/0167-5087(84)90303-X
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1984RI08      Phys.Rev. C29, 2346 (1984)

H.Ries, G.Mank, J.Drexler, R.Heil, K.Huber, U.Kneissl, R.Ratzek, H.Stroher, T.Weber, W.Wilke

Absolute Photofission Cross Sections for 235,238U in the Energy Range 11.5-30 MeV

NUCLEAR REACTIONS 238,235U(γ, F), E=11.5-30 MeV; measured absolute fission σ(E). Quasimonoenergetic photons from positron annihilation, multiple parallel plate detectors.

doi: 10.1103/PhysRevC.29.2346
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetM0503.


1984ST07      Nucl.Phys. A419, 295 (1984)

H.Stroher, J.Drexler, R.Heil, K.Huber, U.Kneissl, G.Mank, R.Ratzek, H.Ries, T.Weber, W.Wilke, H.J.Maier

Fission Barriers of Preactinide Nuclei from Electrofission Experiments

NUCLEAR REACTIONS 182,184,186W, Pt, 209Bi(e, F), E=25-55 MeV; measured electron induced fission σ(E); deduced fission barriers B. Natural, enriched targets. Statistical model analysis.

doi: 10.1016/0375-9474(84)90394-4
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1984WE05      Z.Phys. A315, 125 (1984)

T.Weber, J.Drexler, R.D.Heil, K.Huber, U.Kneissl, G.Mank, H.Ries, H.Stroher, W.Wilke

A New Method to Test Virtual Photon Spectra

NUCLEAR REACTIONS 232Th(e-, F), E=9 MeV; 232Th(e+, F), E=16 MeV; measured fission fragment σ(θ), anisotropy.

doi: 10.1007/BF01436220
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1983DR14      Nucl.Phys. A411, 17 (1983)

J.Drexler, R.Heil, K.Huber, U.Kneissl, G.Mank, R.Ratzek, H.Ries, H.Stroher, T.Weber, W.Wilke

The Decay of Uranium Shape Isomers Investigated by Photonuclear Reactions

NUCLEAR REACTIONS 238U(γ, γ'), E=12 MeV bremsstrahlung; measured isomer T1/2, isomeric to prompt yield ratio; deduced isomeric fission cross section. 238U deduced isomer decay branching ratio. Natural target.

doi: 10.1016/0375-9474(83)90505-5
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1979BA54      Nucl.Instrum.Methods 163, 377 (1979)

R.Bass, J.Idzko, H.Pelz, K.Stelzer, T.Weber, R.Weniger

Symmetrical Four-Crystal Compton Polarimeter for Gamma Rays: Design and Application

RADIOACTIVITY 24,25Mg, 152Eu, 56Co; measured asymmetry (Eγ). Four crystal Compton polarimeter.

NUCLEAR REACTIONS 107,109Ag(α, α'γ), E=2.5 MeV; 28Si, Fe(p, p'γ), E=3.10 MeV; 24Mg(p, p'γ), E=2.01, 6.06 MeV; 31P(α, pγ), E=6.30, 7.00 MeV; measured linear polarization, polarization sensitivity. 36Ar(α, pγ), 92Zr(p, nγ), E not given; measured γ(θ), linear polarization P(θγ). 39K level deduced J, π, δ. 92Nb level deduced J, π ≠ 0-; four crystal Compton polarimeter.

doi: 10.1016/0029-554X(79)90122-8
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1979GM02      Czech.J.Phys. B29, 155 (1979); Erratum Czech.J.Phys. B29, 1308 (1979)

M.Gmitro, E.Tinkova, A.Rimini, T.Weber

Positive Parity Giant Multipole Resonances in 16O

NUCLEAR STRUCTURE 16O; calculated T=0, 1, GMR strength distribution for positive pariy J=0 to 4 states. Shell model n particle-n hole.

doi: 10.1007/BF01957544
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1977GM01      Lett.Nuovo Cim. 20, 449 (1977)

M.Gmitro, E.Tinkova, A.Rimini, T.Weber

Spreading of the Giant Quadrupole Resonance in 16O

NUCLEAR STRUCTURE 16O; calculated distribution of isoscalar GQR.

doi: 10.1007/BF02783557
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1975BO19      Nuovo Cim. 25A, 503 (1975)

A.Boiti, A.Rimini, T.Weber

RPA-Oriented Shell Model Study of 56Ni

NUCLEAR STRUCTURE 56Ni; calculated levels, role of 3p-3h configuration.

doi: 10.1007/BF02820861
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1974GM02      Nuovo Cim. 21A, 11 (1974)

M.Gmitro, A.Rimini, T.Weber

The Role of the 4p-4h Excitations in the Microscopic Description of 56Ni

NUCLEAR STRUCTURE 56Ni; calculated levels.

doi: 10.1007/BF02731184
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1973GA05      Phys.Rev. C7, 1454 (1973)

Y.K.Gambhir, A.Rimini, T.Weber

Analysis of (p, t) and (t, p) Reaction Data for Nickel Isotopes with Structure Wave Functions of the Broken-Pair Approximation

NUCLEAR REACTIONS 58,60,62,64,66Ni(p, t), 58,60,62,64Ni(t, p); measured nothing; deduced S.

doi: 10.1103/PhysRevC.7.1454
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1973GM01      Nuovo Cim. 13A, 526 (1973)

M.Gmitro, A.Rimini, T.Weber

On the n-n and n-p Effective Interactions for 1f7/2 Protons and (2p, 1f5/2) Neutrons

NUCLEAR STRUCTURE 58,59,60Ni, 56,57Co, 55,56Fe, 54,55Mn, 53,54Cr; calculated levels, rms radii.

doi: 10.1007/BF02827353
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1971GA06      Phys.Rev. C3, 1965 (1971)

Y.K.Gambhir, A.Rimini, T.Weber

Number-Conserving Shell-Model Calculations for Nickel and Tin Isotopes

NUCLEAR STRUCTURE 58,60,62,64Ni, 116,120,124Sn; calculated levels. Number-conserving shell model.

doi: 10.1103/PhysRevC.3.1965
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1970BO40      Lett.Nuovo Cim. 4, 988 (1970)

S.Boffi, A.Rimini, T.Weber

Note on the Microscopic Description of the Charge Form Factor of 4He

NUCLEAR STRUCTURE 4He; calculated charge form factor.

doi: 10.1007/BF02755259
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1970BO43      Phys.Lett. 33B, 553 (1970)

A.Boiti, M.Gmitro, A.Rimini, T.Weber

On a Completely Microscopic Description of the 2p-1f Shell Nuclei

NUCLEAR STRUCTURE 56Ni; calculated levels. Tamm-Dancoff, 2p-2h approximations.

doi: 10.1016/0370-2693(70)90346-1
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1970GM01      Phys.Rev. C1, 1801 (1970)

M.Gmitro, A.Rimini, P.Rossi, T.Weber

Comparison between the Quasiparticle Tamm-Dancoff and Random-Phase Approximations in Even Tin Isotopes Using Realistic Interactions

NUCLEAR STRUCTURE 116,120Sn; calculated levels. Quasiparticle Tamm-Dancoff, random phase approximations; realistic interactions.

doi: 10.1103/PhysRevC.1.1801
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1970RI07      Phys.Rev. C2, 324 (1970)

A.Rimini, T.Weber

Effect of Particle-Number Projection on the Determination of the Ground State of Superconducting Nuclei

NUCLEAR STRUCTURE 60,62,64Ni, 112,116,120,124Sn; calculated pair distribution coefficients for ground states. BCS, projected BCS theories.

doi: 10.1103/PhysRevC.2.324
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1969AL08      Phys.Rev. 182, 1308 (1969)

R.Alzetta, T.Weber, Y.K.Gambhir, M.Gmitro, J.Sawicki, A.Rimini

Improved Inverse Gap Equation and Quasiparticle Theories of Odd and Even Tin Isotopes

NUCLEAR STRUCTURE 115,116,117,118,119,120,121Sn; calculated levels, S for (d, p), (p, d), (d, t), (p, t) reactions. Quasiparticle theory, inverse gap equation.

doi: 10.1103/PhysRev.182.1308
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1969AL16      Phys.Rev. 185, 1233 (1969)

R.Alzetta, A.Rimini, T.Weber, M.Gmitro, J.Sawicki

Effective N-N Interaction and Electromagnetic Operators Deduced from the Tabakin Potential: Application to Nickel Isotopes

NUCLEAR STRUCTURE 58,59,60,61,62,63,64Ni; calculated levels, B(E2), B(M1). Second Tamm-Dancoff theory, Tabakin potential.

doi: 10.1103/PhysRev.185.1233
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1968GM05      Phys.Rev. 175, 1243 (1968)

M.Gmitro, A.Rimini, J.Sawicki, T.Weber

Microscopic Theory of Effective Operators for Electromagnetic Interactions in Nuclei

doi: 10.1103/PhysRev.175.1243
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1968RI04      Phys.Rev.Letters 20, 676 (1968)

A.Rimini, J.Sawicki, T.Weber

Inelastic Electron Scattering from Even Tin Isotopes and Microscopic Theories of Vibrational States

doi: 10.1103/PhysRevLett.20.676
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