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NSR database version of April 29, 2024.

Search: Author = W.Pilz

Found 19 matches.

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1992SC14      Z.Phys. A341, 481 (1992)

A.Schubert, J.Hutsch, K.Moller, W.Neubert, W.Pilz, G.Schmidt, M.Adler, H.Marten

Light Charged Particle Release in 252Cf Spontaneous Fission: Tripartition versus fragment de-excitation

RADIOACTIVITY 252Cf(SF); measured emission probability vs E, θ for p, t, α following SF-decay; deduced emission mechanism differences. Position sensitive parallel-plate avalanche detector. Model comparison.

doi: 10.1007/BF01301393
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset23544.

1991PI02      Z.Phys. A338, 75 (1991)

W.Pilz, W.Neubert

Angular Distributions of Prompt γ-Rays in the Binary and the Light Charged Particle Accompanied Fission Modes of 252Cf

RADIOACTIVITY 252Cf(SF); measured γ(θ) following fission fragment decay, σ(Eγ, θ(γ-light fragment)); deduced equatioral α-particle role.

doi: 10.1007/BF01279117
Citations: PlumX Metrics

1991SC02      Z.Phys. A338, 115 (1991)

A.Schubert, K.Moller, W.Neubert, W.Pilz, G.Schmidt, M.Adler, H.Marten

Light Charged Particle Release in Fission: Tripartition versus Fragment De-Excitation

RADIOACTIVITY 252Cf(SF); measured proton, triton, α-particle energy, θ distribution following fission; deduced light particle emission mechanism.

doi: 10.1007/BF01279123
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset23544.

1989PI08      Z.Phys. A333, 315 (1989)

W.Pilz, W.Neubert, H.Marten, N.F.Bondar

Angular Distributions of Prompt γ-Rays in the Light Charged Particle Accompanied and Binary Fission of 252Cf

RADIOACTIVITY 252Cf(SF); measured γ(θ) vs Eγ; deduced fission mode role.

1986ME04      Radiat.Eff. 93, 153 (1986)

A.Meister, S.Mittag, W.Pilz, D.Seeliger, K.Seidel

Doppler Broadenings of Neutron Resonances in Crystal Lattices Compared with the Gas-Model Approximation

NUCLEAR REACTIONS 238U(n, X), E=6.67 eV; 240Pu(n, X), E=1.056 eV; measured transmission. 239U, 241Pu deduced resonance parameter uncertainities. Gas model approximation.

doi: 10.1080/00337578608207442
Citations: PlumX Metrics

1986MO21      Few-Body Systems 1, 83 (1986)

J.Mosner, K.Moller, W.Pilz, G.Schmidt, T.Stiehler

A Measurement of the Total Cross Section of the Capture Reaction 2H(n, t)γ at E(n) = 25 MeV

NUCLEAR REACTIONS 2H(n, t), E=25 MeV; measured σ. Gas target, scintillation counter telescope, two-dimensional measurements.

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30973.

1986ST14      Ann.Phys.(Leipzig) 43, 602 (1986)

T.Stiehler, J.Mosner, G.Schmidt, K.Moller, W.Neubert, W.Pilz, B.Kuhn, J.Hutsch

The Total n-p Capture Cross Section Measured at E(n) = 25 MeV

NUCLEAR REACTIONS 1H(n, γ), E=25 MeV; measured total capture σ. Gas target, multi-wire proportional counters.

doi: 10.1002/andp.19864980620
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30705.

1985MI03      Nucl.Phys. A435, 97 (1985)

S.Mittag, D.Pabst, L.B.Pikelner, W.Pilz, R.Tschammer, A.Meister, D.Seeliger, K.Seidel

Chemically Induced Shifts of 235U and 234U Neutron Resonances

NUCLEAR REACTIONS 235U(n, X), E=1.1, 2, 3.1, 3.6, 4.8, 5.2, 8.8, 11.7, 12.4 eV; measured transmission spectra. 235,236U deduced chemically induced resonance shifts, rms charge radii. Tof, U, UO2, U3O8, UO3 metallic sampler, 235U enrichment.

doi: 10.1016/0375-9474(85)90306-9
Citations: PlumX Metrics

1985SE22      Yad.Fiz. 42, 1041 (1985)

K.Seidel, D.Seeliger, V.K.Ignatovich, A.Meister, S.Mittag, V.Pilz

Temperature Shift of Neutron Resonances

NUCLEAR REACTIONS 161,163Dy, 109Ag, 103Rh(n, n), E=reactor; measured σ(En). 162,164Dy, 110Ag, 104Rh deduced resonances, temperature shifts.

1985ST04      Phys.Lett. 151B, 185 (1985)

T.Stiehler, B.Kuhn, K.Moller, J.Mosner, W.Neubert, W.Pilz, G.Schmidt

A Measurement of the Total Cross Section of the Reaction n + p → d + γ at E(n) = 25 MeV

NUCLEAR REACTIONS 1H(n, γ), E=25 MeV; measured capture σ. Gas target, scintillation telescope.

doi: 10.1016/0370-2693(85)90831-7
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30705.

1981HO13      J.Phys.(London) G7, 803 (1981)

J.Hohn, J.Kayser, W.Pilz, D.Schmidt, D.Seeliger

Experimental Investigation of the 11B + p Reaction and Analysis in the Frame of the Continuum Shell Model

NUCLEAR REACTIONS 11B(p, n), E=5.4-7.5 MeV; measured σ(E, θ); deduced direct, resonance effects. 12C deduced resonances, Γ, J, π. Continuum shell model.

doi: 10.1088/0305-4616/7/6/013
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0288.

1981PI08      Yad.Fiz. 33, 885 (1981)

W.Pilz, D.Schmidt, D.Seeliger, A.I.Vdovin

Study of the 109Ag(p, n)109Cd Reaction in the Energy Range Ep = 4.5-9 MeV

NUCLEAR REACTIONS 109Ag(p, n), E=4.5-9 MeV; measured σ(θ); deduced reaction mechanism. Semi-microscopic model.

1981SE16      Yad.Fiz. 34, 1173 (1981)

K.Seidel, A.Meister, D.Pabst, L.B.Pikelner, W.Pilz

Resonance Interaction of Neutrons with a Molecular Gas and with Crystals

NUCLEAR REACTIONS 238U(n, n), (n, X), E=6.67 eV; measured σ, transmission; deduced atomic thermal vibration effects. Polycrystalline UO3, gaseous UF6 samples.

1980EC02      Nucl.Instrum.Methods 169, 533 (1980)

P.Eckstein, H.Helfer, D.Katzmer, J.Kayser, R.Krause, D.Lehmann, W.Meiling, W.Pilz, J.Rumpf, D.Schmidt, D.Seeliger, T.Streil

A Multi-Angle Detector System for Fast Neutron Time-of-Flight Spectroscopy

NUCLEAR REACTIONS 59Co(p, n), E=5.5 MeV; 28Si(n, n'), E=9 MeV; 28Si(n, n), E=6.8-12 MeV; measured σ(En, θ). Multi-angle tof spectrometer.

doi: 10.1016/0029-554X(80)90953-2
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30563.

1980GU11      Nucl.Phys. A342, 239 (1980)

H.Guratzsch, B.Kuhn, H.Kumpf, J.Mosner, W.Neubert, W.Pilz, G.Schmidt, S.Tesch

Neutron-Neutron Effective Range from Quasifree Scattering 2H(n, nn)p At 25 MeV

NUCLEAR REACTIONS 2H(n, 2n), E=25 MeV; measured σ(E(n1), E(n2), θ1, θ2), quasifree neutron-neutron kinematic condition; deduced neutron-neutron effective range. D2O target.

doi: 10.1016/0375-9474(80)90252-3
Citations: PlumX Metrics

1980LO05      Yad.Fiz. 31, 3 (1980);Sov.J.Nucl.Phys. 31, 1 (1980)

G.N.Lovchikova, O.A.Salnikov, S.P.Simakov, A.M.Trufanov, G.V.Kotelnikova, V.Pilz, T.Streil

Investigation of Mechanism of the Reactions 94Zr(p, n)94Nb, 119Sn(p, n)120Sb, 122Sn(p, n)122Sb in the Proton Energy Region 6-9 MeV

NUCLEAR REACTIONS 94Zr, 119,122Sn(p, n), E=6-9 MeV; measured σ(En, θ); deduced non-equilibrium process. Fermi gas model, inverse shift.

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0221.

1978LO14      Yad.Fiz. 28, 605 (1978); Sov.J.Nucl.Phys. 28, 310 (1978)

G.N.Lovchikova, O.A.Salnikov, S.P.Simakov, A.M.Trufanov, D.Seeliger, E.Kaiser, W.Pilz, D.Schmidt, T.Streil

Neutron Spectra in Decay of Isobaric Analog Resonances in the Reactions 109Ag(p, n)109Cd and 115In(p, n)115Sn

NUCLEAR REACTIONS 109Ag(p, n), E=6.4-7.0 MeV; measured σ(E, θ). 110Cd deduced analog resonances. 115In(p, n), E=6.6-7.5 MeV; measured σ(E, θ). 116Sn deduced analog resonances.

1977EC05      Kernenergie 20, 161 (1977)

P.Eckstein, H.Helfer, D.Katzmer, J.Kayser, D.Lehmann, W.Pilz, J.Rumpf, D.Schmidt, D.Seeliger, T.Streil

Spektroskopie schneller Neutronen am Tandembeschleuniger, EGP-10-1

1977GU13      Nucl.Phys. A293, 109 (1977)

H.Guratzsch, B.Kuhn, H.Kumpf, J.Mosner, W.Neubert, W.Pilz, G.Schmidt, S.Tesch

The Neutron-Proton Final-State Interaction in Proton-Induced Deuteron Break-up at 8.5 MeV

NUCLEAR REACTIONS 2H(p, 2p), E=8.5 MeV; measured σ(Ep1, Ep2, θ1, θ2, φ); deduced final-state interaction angular distribution; compared with Faddeev theory for exponential, Yamaguchi form factors.

doi: 10.1016/0375-9474(77)90479-1
Citations: PlumX Metrics

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