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1994HO08      Phys.Rev. C49, 2555 (1994)

P.Hofmann, A.S.Iljinov, Y.S.Kim, M.V.Mebel, H.Daniel, P.David, T.von Egidy, T.Haninger, F.J.Hartmann, J.Jastrzebski, W.Kurcewicz, J.Lieb, H.Machner, H.S.Plendl, G.Riepe, B.Wright, K.Ziock

Fission of Heavy Nuclei Induced by Stopped Antiprotons. I. Inclusive Characteristics of Fission Fragments

NUCLEAR REACTIONS 238U, 232Th, 209Bi(p-bar, F), E at rest; measured fission fragment energy, mass, θ; deduced fission fragment total mass, total momentum. Intranuclear cascade, evaporation, fission models.

doi: 10.1103/PhysRevC.49.2555
Citations: PlumX Metrics


1993RO07      Z.Phys. A345, 89 (1993)

Ch.Rosel, H.Hanscheid, J.Hartfiel, R.von Mutius, J.F.M.d'Achard van Enschut, P.David, H.Janszen, T.Johansson, J.Konijn, T.Krogulski, C.T.A.M.de Laat, H.Paganetti, C.Petitjean, S.M.Polikanov, H.W.Reist, F.Risse, L.A.Schaller, L.Schellenberg, W.Schrieder, A.K.Sinha, A.Taal, J.P.Theobald, G.Tibell, N.Trautmann

The Study of Prompt and Delayed Muon Induced Fission III. The Ratios of Prompt to Delayed Fission Yields

NUCLEAR REACTIONS 233,234,235,236,238U, 237Np, 242,244Pu(μ-, F), E not given; measured prompt to delayed fission yields ratios, absolute probabilities; deduced fission probabilities per muon capture.


1993RO14      Z.Phys. A345, 425 (1993)

C.Rosel, F.F.Karpeshin, P.David, H.Hanscheid, J.Konijn, C.T.A.M.de Laat, H.Paganetti, F.Risse, B.Sabirov, L.A.Schaller, L.Schellenberg, W.Schrieder, A.Taal

Experimental Evidence for Muonic X-Rays from Fission Fragments

NUCLEAR REACTIONS 238U(μ-, F), E at rest; analyzed fission fragment decay γ(X-ray)-coin data; deduced structure associated with transitions of muon attached to fragment.

ATOMIC PHYSICS, Mesic-Atoms 238U(μ-, F), E at rest; analyzed fission fragment decay γ(X-ray)-coin data; deduced structure associated with transitions of muon attached to fragment.


1993VO06      Nucl.Phys. A558, 383c (1993)

T.von Egidy, H.Daniel, F.J.Hartmann, P.Hofmann, Y.S.Kim, W.Schmid, H.H.Schmidt, G.Riepe, H.Machner, P.David, H.S.Plendl, A.S.Iljinov, A.S.Botvina, Ye.S.Golubeva, M.V.Mebel, J.Jastrzebski, W.Kurcewicz

Antiproton Induced Fission

NUCLEAR REACTIONS 209Bi, 232Th, 238U(p-bar, F), E at 105 MeV/c; measured fission fragment mass yield distributions; deduced absolute fission probabilities.

doi: 10.1016/0375-9474(93)90407-O
Citations: PlumX Metrics


1992HA14      Z.Phys. A342, 111 (1992)

H.Hanscheid, P.David, H.Folger, J.Konijn, C.T.A.M.de Laat, C.Petitjean, H.W.Reist, F.Risse, Ch.Rosel, L.A.Schaller, L.Schellenberg, W.Schrieder, L.M.Simons, A.Taal

Nuclear Excitation and Prompt Fission in Muonic 238U

NUCLEAR REACTIONS 238U(μ-, F), E at 43 MeV/c; measured fission (fragment)γ-, γγ-, muonic (X-ray)(fragment)-coin, (X-ray)(fragment)(t); deduced fission barrier augmentation, nonradiative transitions role, fission probabilities.

ATOMIC PHYSICS, Mesic-Atoms 238U(μ-, F), E at 42 MeV/c; measured fission (fragment)γ-, γγ-, muonic (X-ray)(fragment)-coin, (X-ray)(fragment)(t); deduced fission barrier augmentation, nonradiative transitions role, fission probabilities.


1992PA16      Z.Phys. A342, 245 (1992)

H.Paganetti, P.David, H.Hanscheid, J.Konijn, C.T.A.M.de Laat, W.Lourens, F.Risse, Ch.Rosel, L.A.Schaller, A.Taal

Radiationless Transition Probabilities in Muonic 209Bi

NUCLEAR REACTIONS 209Bi(μ-, X), E not given; measured E X-ray, I X-ray, (X-ray)(X-ray)-coin; deduced nonradiative excitation probability. Large volume Ge detectors, BGO Compton suppression system, large CsF crystal.

ATOMIC PHYSICS, Mesic-Atoms 209Bi(μ-, X), E not given; measured E X-ray, I X-ray, (X-ray)(X-ray)-coin; deduced nonradiative excitation probability. Large volume Ge detectors, BGO Compton suppression system, large CsF crystal.

doi: 10.1007/BF01288477
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1992PA17      Z.Phys. A343, 113 (1992)

H.Paganetti, P.David, H.Hanscheid, J.Konijn, C.T.A.M.de Laat, W.Lourens, F.Risse, Ch.Rosel, L.A.Schaller, A.Taal

Delayed Muon Induced Fission of 209Bi and the Role of Meson-Exchange Currents

NUCLEAR REACTIONS 209Bi(μ-, F), E not given; measured fission (fragment)(fragment)(t), E X-ray, I X-ray, γγ-coin; deduced delayed fission probability, relevance to two-body meson-exchange currents investigation.

doi: 10.1007/BF01291603
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1992SI06      J.Phys.(London) G18, L105 (1992)

A.K.Sinha, P.David, H.Hanscheid, F.Risse, Ch.Rosel, W.Schrieder

Fission Probabilities of 237U and 236Pa using the (d, tf) and the (d, αf) Reactions

NUCLEAR REACTIONS 238U(d, tF), (d, αF), E=24.85 MeV; measured fission fragment σ(θ). 237U, 236Pa deduced fission probabilities.

doi: 10.1088/0954-3899/18/5/004
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1106.


1991DE01      Nucl.Phys. A523, 453 (1991)

C.T.A.M.De Laat, A.Taal, J.Konijn, P.David, H.Hanscheid, F.Risse, Ch.F.G.Rosel, W.Schrieder, C.Petitjean

A Study of the Strong Interaction Effects on Pionic 3D and 4F Levels in 181Ta, (nat)Re, (nat)Pt, 197Au, 208Pb, 209Bi and 237Np

NUCLEAR REACTIONS 181Ta, Re, Pt, 197Au, 208Pb, 209Bi, 237Np(π-, xnyp), E at rest; measured prompt, delayed neutron, X-ray, γ-spectra; deduced pionic E(X-ray), I(X-ray), strong interaction shifts, widths.

ATOMIC PHYSICS, Mesic-Atoms 181Ta, Re, Pt, 197Au, 208Pb, 209Bi, 237Np(π-, xnyp), E at rest; measured prompt, delayed neutron, X-ray, γ-spectra; deduced E(X-ray), I(X-ray), strong interaction shifts, widths.

doi: 10.1016/0375-9474(91)90031-Z
Citations: PlumX Metrics


1991RI07      Z.Phys. A339, 427 (1991)

F.Risse, W.Bertl, P.David, H.Hanscheid, E.Hermes, J.Konijn, C.T.A.M.de Laat, H.Pruys, Ch.F.G.Rosel, W.Schrieder, A.Taal, D.Vermeulen

Muon Attachment in Prompt Fission of 237Np

NUCLEAR REACTIONS 237Np(μ-, F), E at rest; measured fission fragment mass, total kinetic energy release, (fragment)(electron)-coin; deduced fission fragment muon attachment probability.

doi: 10.1007/BF01288426
Citations: PlumX Metrics


1991RO10      Z.Phys. A340, 199 (1991)

Ch.Rosel, P.David, H.Folger, H.Hanscheid, J.Konijn, C.T.A.M.de Laat, C.Petitjean, H.W.Reist, F.Risse, L.A.Schaller, L.Schellenberg, W.Schrieder, L.M.Simons, A.K.Sinha, A.Taal

Radiationless Transition Probabilities in Muonic 208Pb, 232Th, and 238U

NUCLEAR REACTIONS 208Pb, 232Th, 238U(μ-, γ), (μ-, X), E at 42-54 MeV/c; measured γγ-coin, X-ray spectra, Eγ, Iγ. 208Pb, 232Th, 238U deduced nonradiative transition probabilities.

ATOMIC PHYSICS, Mesic-Atoms 208Pb, 232Th, 238U(μ-, γ), (μ-, X), E at 42-54 MeV/c; measured γγ-coin, X-ray spectra, Eγ, Iγ. 208Pb, 232Th, 238U deduced nonradiative transition probabilities.


1991SC21      Z.Phys. A339, 445 (1991)

W.Schrieder, P.David, H.Hanscheid, J.Konijn, C.T.A.M.de Laat, H.Paganetti, C.Petitjean, H.W.Reist, F.Risse, Ch.F.G.Rosel, L.A.Schaller, L.Schellenberg, A.K.Sinha, A.Taal, N.Trautmann

The Probability of Prompt and Delayed Fission of Muonic 237Np

NUCLEAR REACTIONS 237Np(μ, F), E at rest; measured (fragment)(X-ray)-coin; deduced prompt, delayed, total fission probabilities.

doi: 10.1007/BF01288428
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1990HA03      Z.Phys. A335, 1 (1990)

H.Hanscheid, P.David, J.Konijn, T.Krogulski, C.T.A.M.de Laat, T.Mayer-Kuckuk, C.Petitjean, S.M.Polikanov, H.W.Reist, F.Risse, Ch.F.G.Rosel, L.A.Schaller, L.Schellenberg, W.Schrieder, A.K.Sinha, A.Taal

Muon Capture Rates in 233U, 234U, 235U, 236U, 238U, and 237Np

NUCLEAR REACTIONS 233,234,235,236,238U, 237Np(μ-, F), E at 39 MeV/c; measured (fragment)(fragment)-coin following fission; deduced capture rates, bound muon T1/2.

ATOMIC PHYSICS, Mesic-Atoms 233,234,235,236,238U, 237Np(μ-, F), E at 39 MeV/c; measured (fragment)(fragment)-coin following fission; deduced capture rates, bound muon T1/2.


1990TA10      Nucl.Phys. A511, 573 (1990)

A.Taal, P.David, H.Hanscheid, J.H.Koch, C.T.A.M.de Laat, W.Lourens, F.Risse, Ch.F.G.Rosel, A.van der Schaaf, W.Schrieder, J.Konijn

Deeply Bound 1s and 2p States in Pionic Atoms

NUCLEAR REACTIONS 24Mg, 27Al, 28Si(π-, xnyp), E at rest; measured prompt, delayed neutron, X-ray, γ-spectra. 93Nb, Ru, Ag, Cd(π-, X), E at rest; measured X-ray spectra; deduced strong interaction shifts, widths.

ATOMIC PHYSICS, Mesic-Atoms 24Mg, 27Al, 28Si(π-, xnyp), E at rest; measured prompt, delayed neutron, X-ray, γ-spectra. 93Nb, Ru, Ag, Cd(π-, X), E at rest; measured X-ray spectra; deduced strong interaction shifts, widths.

doi: 10.1016/0375-9474(90)90111-X
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1988DA17      Z.Phys. A330, 397 (1988)

P.David, H.Hanscheid, J.Hartfiel, H.Janszen, T.Mayer-Kuckuk, R.von Mutius, F.Risse, Ch.F.G.Rosel, W.Schrieder, C.Petitjean, H.W.Reist, S.M.Polikanov, J.Konijn, C.T.A.M.de Laat, A.Taal, T.Krogulski, T.Johansson, G.Tibell, J.F.M.d'Achard van Enschut, J.P.Theobald, N.Trautmann, C.Gugler, L.A.Schaller, L.Schellenberg

The Study of Prompt and Delayed Muon Induced Fission II. Mean Life Times of Negative Muons Bound to 237Np, 242Pu and 244Pu

NUCLEAR REACTIONS 237Np, 242,244Pu(μ-, F), E at rest; measured fission (fragment)(fragment)μ-, (fragment)(fragment)-coin; deduced muon capture rates.


1987DA09      Z.Phys. A326, 367 (1987)

P.David, J.Hartfiel, H.Janszen, R.von Mutius, J.Arvieux, L.Farvacque, B.Berthier, B.Bonin, J.C.Lugol

Study of the Reaction 238U(α, α'f) at E(α) = 480 MeV

NUCLEAR REACTIONS 238U(α, α'F), E=480 MeV; measured fission probability vs excitation; deduced reaction mechanism.


1987DA22      Z.Phys. A328, 37 (1987)

P.David, J.Hartfiel, H.Janszen, T.Mayer-Kuckuk, R.von Mutius, C.Petitjean, H.W.Reist, S.M.Polikanov, J.Konijn, C.T.A.M.de Laat, A.Taal, T.Krogulski, T.Johansson, G.Tibell, J.F.M.d'Achard van Enschut

The Study of Prompt and Delayed Muon Induced Fission. I. Total Kinetic Energies and Mass Distributions

ATOMIC PHYSICS, Mesic-Atoms 235,238U, 237Np, 242Pu(μ-, F), E at 48, 53 MeV/c; 238U, 237Np(π-, F), E at 110 MeV/c; measured muon induced fission fragment total kinetic energy, mass distributions; deduced muon induced fission characteristics.

NUCLEAR REACTIONS 235,238U, 237Np, 242Pu(μ-, F), E at 48, 53 MeV/c; 238U, 237Np(π-, F), E at 110 MeV/c; measured fission fragment total kinetic energy, mass distributions; deduced muon induced fission characteristics.


1987DE10      Phys.Lett. 189B, 7 (1987)

C.T.A.M.De Laat, A.Taal, W.Duinker, J.Konijn, J.F.M.D'Achard van Enschut, P.David, J.Hartfiel, H.Janszen, T.Mayer-Kuckuk, R.von Mutius, G.Piller, L.A.Schaller, L.Schellenberg, T.Krogulski, C.Petitjean, H.W.Reist, W.Muller

The Quadrupole Moment and Strong Interaction Parameters from Muonic and Pionic X-Ray Studies of 237Np

ATOMIC PHYSICS, Mesic-Atoms 237Np(π-, X), E at 100 MeV/c; 237Np(μ-, X), E at 50 MeV/c; measured X-ray spectra; deduced strong interaction shifts, widths. 237Np deduced spectroscopic quadrupole moment, B(E2). Compton suppression spectrometer. Optical model.

NUCLEAR REACTIONS 237Np(π-, X), E at 100 MeV/c; 237Np(μ-, X), E at 50 MeV/c; measured X-ray spectra. 237Np deduced spectroscopic quadrupole moment, B(E2). Compton suppression spectrometer. Optical model.

doi: 10.1016/0370-2693(87)91260-3
Citations: PlumX Metrics


1986DA21      Phys.Lett. 180B, 324 (1986)

P.David, J.Hartfiel, H.Janszen, T.Mayer-Kuckuk, R.von Mutius, C.T.A.M.de Laat, A.Taal, W.Duinker, J.Konijn, J.F.M.D'Achard van Enschut, C.Gugler, L.A.Schaller, L.Schellenberg, T.Krogulski, C.Petitjean, H.W.Reist, W.Muller

The Probability of Non-Radiative Decay of the 3d Level in Muonic 237Np

ATOMIC PHYSICS, Mesic-Atoms 237Np; measured muonic X-ray spectra. 237Np deduced radiationless muonic transition probability.

NUCLEAR REACTIONS 237Np(μ-, γ), E at rest; measured X-ray spectra. 237Np deduced radiationless muonic 3d → 1s transition probability.

doi: 10.1016/0370-2693(86)91196-2
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1985DE48      Phys.Lett. 162B, 81 (1985)

C.T.A.M.De Laat, A.Taal, W.Duinker, A.H.Wapstra, J.Konijn, J.F.M.d'Achard van Enschut, P.David, J.Hartfiel, H.Janszen, R.von Mutius, C.Gugler, L.A.Schaller, L.Schellenberg, T.Krogulski, C.Petitjean, H.W.Reist

Strong Interaction Effects in Pionic 208Pb

NUCLEAR REACTIONS 208Pb(π, X), E at rest; measured pionic X-rays; deduced strong interaction shifts.

ATOMIC PHYSICS, Mesic-Atoms 208Pb(π, X), E at rest; measured pionic X-rays; deduced strong interaction shifts.

doi: 10.1016/0370-2693(85)91065-2
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1984DA04      Nucl.Phys. A417, 24 (1984)

P.David, J.Debrus, J.Hartfiel, H.Janszen, R.Von Mutius, H.J.Maier

A Study of the 230Th(α, α'f) Reaction at 50 MeV

NUCLEAR REACTIONS, ICPND 230Th(α, α'F), E=50 MeV; measured fission fragment energies, mass yield distribution, total kinetic energy vs excitation.

doi: 10.1016/0375-9474(84)90321-X
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1983DA09      Phys.Lett. 124B, 161 (1983)

P.David, J.Hartfiel, H.Janszen, T.Johansson, J.Konijn, T.Krogulski, T.Mayer-Kuckuk, C.Petitjean, S.Polikanov, H.W.Reist, G.Tibell

Total Kinetic Energy Release and Mass Distributions in Prompt and Delayed Muon Induced Fission of 238U

NUCLEAR REACTIONS 238U(μ-, F), E at rest; measured prompt, delayed fission fragment mass, total kinetic energy release; deduced prompt to delayed fission yields, muonic state T1/2.

doi: 10.1016/0370-2693(83)91426-0
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1982DA14      Nucl.Phys. A380, 27 (1982)

P.David, J.Debrus, H.Janszen, J.Schulze, M.N.Harakeh, J.Van Der Plicht, A. Van Der Woude

The Study of the (α, α'f) Reaction at 120 MeV on 232Th (III). Total Kinetic Energies and Mass Distributions for Excitation Energies below 12 MeV

NUCLEAR REACTIONS, Fission 232Th(α, α'F), E=120 MeV; measured σ(fragment θ), fragment energy, mass distributions, mass-energy correlations, fission probabilities, total kinetic energy release.

doi: 10.1016/0375-9474(82)90580-2
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1982DE07      Nucl.Phys. A373, 509 (1982)

R.De Leo, M.N.Harakeh, S.Micheletti, J.Van Der Plicht, A.Van Der Woude, P.David, H.Janszen

Axial Symmetry around the Recoil Axis for the 238U(α, α'f) Reaction and the Fission Probability in the Giant Resonance Region

NUCLEAR REACTIONS, Fission 238U(α, α'F), E=120 MeV; measured σ(fragment, φ, θ), fission probabilities. 238U deduced fission decay mode in giant resonance region.

doi: 10.1016/0375-9474(82)90548-6
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1982MO28      Phys.Lett. 119B, 315 (1982)

H.P.Morsch, M.Rogge, P.Decowski, H.Machner, C.Sukosd, P.David, J.Debrus, J.Hartfiel, H.Janszen, J.Schulze

Fission Decay of Isoscalar Giant Resonances Excited in 172 MeV α Scattering from 238U

NUCLEAR REACTIONS 238U(α, α'F), E=172 MeV; measured fission(fragment)α-coin, σ(fragment θ, θα), σ(θα'). 238U deduced isoscalar giant resonances.

doi: 10.1016/0370-2693(82)90678-5
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1981VA20      Nucl.Phys. A369, 51 (1981)

J.Van Der Plicht, M.N.Harakeh, A.Van Der Woude, P.David, J.Debrus, H.Janszen, J.Schulze

The Study of the (α, αf) Reaction at 120 MeV on 232Th and 238U (II). Fission Barrier Properties Deduced from Fission Probabilities and Angular Distributions

NUCLEAR REACTIONS, Fission 232Th, 238U(α, α'F), E=120 MeV; measured σ(fragment θ), fission probabilities. Double-humped barrier model calculations.

doi: 10.1016/0375-9474(81)90006-3
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1980VA14      Nucl.Phys. A346, 349 (1980)

J.Van Der Plicht, M.N.Harakeh, A. Van der Woude, P.David, J.Debrus, H.Janszen, J.Schulze

The Study of the (α, α'F) Reaction at 120 MeV on 232Th and 238U (I). Fission probabilities and angular distributions in the region of the giant quadrupole resonances

NUCLEAR REACTIONS, Fission 232Th, 238U(α, α'F), E=120 MeV; measured σ(fragment θ), fission probabilities. 232Th, 238U deduced fission decay modes in the GQR region.

doi: 10.1016/0375-9474(80)90474-1
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1979DA08      Nucl.Phys. A319, 205 (1979)

P.David, J.Debrus, H.Fahlbusch, J.Schulze

4He Induced Reactions on 45Sc at T(4He) = 150 MeV and on 238U, 197Au, 120Sn and 67Zn at T(4He) = 140 MeV

NUCLEAR REACTIONS 45Sc(α, xnyp), E=150 MeV; 238U, 197Au, 120Sn, 64Zn(α, F), E=140 MeV; measured yields, σ(44mSc)/σ(44gSc) isomeric yield ratio, fission σ; calculated fission probabiliy; discussed 24Na yield. Liquid drop model. Ge(Li) detectors, mica solid state detectors, activation analysis.

doi: 10.1016/0375-9474(79)90181-7
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1979HA14      Phys.Lett. 82B, 297 (1979)

S.Hartwig, F.H.Heimlich, G.Huber, E.Rossle, J.Bleckwenn, M.Kobberling, J.Moritz, K.H.Schmidt, D.Wegener, D.Zeller, P.David, H.Mommsen

Comparison of Inelastic Electron and Positron Scattering Cross Sections on 12C and 27Al

NUCLEAR REACTIONS 12C, 27Al(e-, e-), (e-, e-'), (e+, e+), (e+, e+'), E=very high; measured σ.

doi: 10.1016/0370-2693(79)90760-3
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1979VA05      Phys.Rev.Lett. 42, 1121 (1979)

J.van der Plicht, M.N.Harakeh, A.van der Woude, P.David, J.Debrus

Inhibition of the Fission Decay Channel of the Isoscalar Giant Quadrupole Resonance in the Actinide Region

NUCLEAR REACTIONS 232Th(α, α'F), E=120 MeV; measured σ(Eα'), α'F(θ)-coin. 232Th deduced upper limit for fission probability of T=0, GQR.

doi: 10.1103/PhysRevLett.42.1121
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1978BI01      Phys.Rev. C17, 177 (1978)

J.Bisplinghoff, P.David, M.Blann, W.Scobel, T.Mayer-Kuckuk, J.Ernst, A.Mignerey

35Cl-Induced Fission and Fissionlike Reactions on 58,62Ni, 112,116,120,124Sn, and 141Pr

NUCLEAR REACTIONS 58,62Ni, 112,116,120,124Sn, 141Pr(35Cl, F), E=155-170 MeV; measured σ(E, Z, θ); deduced total fission σ. Gas proportional/solid state counter telescopes.

doi: 10.1103/PhysRevC.17.177
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1978DA10      Phys.Lett. 77B, 178 (1978)

P.David, J.Debrus, F.Lubke, R.Schoenmackers, J.Schulze

The Fission Processes 236U(α, α'f) at E = 50 MeV and 235U(d, pf) at E = 23 MeV and the Total Kinetic Energy Release in Fission of Excited Nuclei

NUCLEAR REACTIONS 236U(α, α'), E=50 MeV; 235U(d, p), E=23 MeV; measured fission total kinetic energy.

doi: 10.1016/0370-2693(78)90615-9
Citations: PlumX Metrics


1978DA27      S.Afr.J.Phys. 1, 241 (1978)

P.David, J.Debrus, J.Schulze, M.N.Harakeh, J.v.d.Plicht, A.v.d.Woude, H.P.Morsch

Total Kinetic Energy Release in the Fission of Excited Nuclei

NUCLEAR REACTIONS 235U(d, pF), E=23 MeV; 236U(α, α'F), E=50 MeV; 232Th(α, α'F), E=120 MeV; measured total fragment kinetic energy vs excitation; deduced reaction mechanism. Norenberg, Swiatecki models.


1978SC03      Z.Phys. A284, 343 (1978)

W.Scobel, J.Bisplinghoff, M.Blann, A.Mignerey, P.David, J.Ernst, T.Mayer-Kuckuk

Elastic Scattering of 35Cl from 27Al, 58,62Ni, 116,120,124Sn and 141Pr

NUCLEAR REACTIONS 27Al, 58,62Ni, 116,120,124Sn, 141Pr(35Cl, 35Cl), E=100-170 MeV; measured σ(E, θ); deduced optical model parameters, interaction radii.

doi: 10.1007/BF01406807
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1977BI06      Phys.Rev. C16, 1058 (1977)

J.Bisplinghoff, A.Mignerey, M.Blann, P.David, W.Scobel

Statistical Analysis of Heavy-Ion-Induced Fission Excitation Functions

NUCLEAR REACTIONS 62Ni, 116Sn, 141Pr(35Cl, F), E=155-170 MeV; calculated σ(E). Statistical model.

doi: 10.1103/PhysRevC.16.1058
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1977DA14      Nucl.Phys. A287, 179 (1977)

P.David, J.Bisplinghoff, M.Blann, T.Mayer-Kuckuk, A.Mignerey

Evaporation Residue Excitation Functions for 35Cl Induced Reactions of 112,120Sn and 141Pr

NUCLEAR REACTIONS 112,120Sn, 141Pr(35Cl, X), E=135-170 MeV; measured evaporation residue cross sections, fission cross sections; deduced complete fusion cross sections σcf(E), fusion radii, fusion barriers. Enriched targets. Gas-proportional-solid-state detector telescopes.

doi: 10.1016/0375-9474(77)90570-X
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1976BA28      Nucl.Phys. A264, 493 (1976)

N.M.Bachschi, P.David, J.Debrus, F.Lubke, H.Mommsen, R.Schoenmackers, G.G.Jonsson, K.Lindgren

Photonuclear Reactions in 45Sc and (nat)Cu Induced by 2 GeV Bremsstrahlung

NUCLEAR REACTIONS 45Sc, Cu(γ, xnpγ), E(max)=2 GeV bremsstrahlung; measured yields, isomeric yield ratios. Ge(Li) detectors.

doi: 10.1016/0375-9474(76)90418-8
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1976DA03      Phys.Lett. 60B, 445 (1976)

P.David, J.Debrus, F.Lubke, H.Mommsen, R.Schoenmackers

Total Kinetic Energies and Mass Yield Distributions of 252Cf Fission Fragments

RADIOACTIVITY, Fission 252Cf(SF); measured yields.

doi: 10.1016/0370-2693(76)90703-6
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset21914.


1976DA04      Phys.Lett. 61B, 158 (1976)

P.David, J.Debrus, F.Lubke, H.Mommsen, E.Schmitt, R.Schoenmackers, H.Simons

Fission of 238U Following Inelastic α-Particle Scattering at Bombarding Energy Eα = 50 MeV

NUCLEAR REACTIONS 238U(α, α'F), E=50 MeV; measured σ(E(A)).

doi: 10.1016/0370-2693(76)90614-6
Citations: PlumX Metrics


1976DA17      Z.Phys. A278, 281 (1976)

P.David, J.Debrus, H.Essen, F.Lubke, H.Mommsen, R.Schoenmackers, W.Soyez, H.V.v.Geramb, E.F.Hefter

Elastic and Inelastic 4He-Scattering on 208Pb, 232Th and 234,236,238U

NUCLEAR REACTIONS 208Pb, 232Th, 234,236,238U(α, α), (α, α'), measured E=50 MeV; measured σ(θ). 232Th, 234,236,238U deduced β.

doi: 10.1007/BF01409180
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6114.


1976ZU01      Z.Phys. A279, 163 (1976)

F.zu Bentheim, P.David, J.Debrus, F.Hinterberger, R.Jahn, F.Lubke, H.Mommsen, R.Schoenmackers, B.Schuller

Elastic Scattering of α-Particles on 10B for Eα = 5-50 MeV

NUCLEAR REACTIONS 10B(α, α), E=30-50.6 MeV; measured σ(E, θ). 10B(α, α'), E=50 MeV; measured σ(Eα', θ). 10B(α, α), E=5-50 MeV; calculated σ(E). Inopin-Ericson model.


1974DA08      Nucl.Phys. A221, 145 (1974)

P.David, J.Debrus, F.Lubke, H.Mommsen, R.Schoenmackers, G.Stein

Bremsstrahlung Induced Nuclear Reactions with E(max γ) = 450 MeV

NUCLEAR REACTIONS 27Al, 40,44Ca, 51V, 59Co, 93Nb, Ag, 181Ta, 197Au(γ, p), (γ, t), (γ, 3He), (γ, α), E=450 MeV; measured σ(E particle) at 90°, yields.

doi: 10.1016/0375-9474(74)90104-3
Citations: PlumX Metrics


1974RI08      Nucl.Phys. A228, 461 (1974)

A.Riccato, P.David

The Reactions 68,70Zn(3He, d)69,71Ga and Level Systematics of the Odd-Mass Ga Isotopes

NUCLEAR REACTIONS 68,70Zn(3He, d), E(3He)=15, 17 MeV; measured σ(Ed, θ). 69,71Ga deduced levels, L, J, π, S. Enriched targets.

doi: 10.1016/0375-9474(74)90615-0
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1793.


1972DA04      Nucl.Phys. A182, 234 (1972)

P.David, J.Debrus, H.Mommsen, A.Riccato

Elastic Scattering of α-Particles on 10B for E = 5-30 MeV

NUCLEAR REACTIONS 10B(α, α), E=5-30 MeV; measured σ(Eα;θ).

doi: 10.1016/0375-9474(72)90274-6
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0220.


1972DA16      Nucl.Phys. A197, 163 (1972)

P.David, J.Debrus, U.Kim, G.Kumbartzki, H.Mommsen, W.Soyez, K.H.Speidel, G.Stein

High-Energy Photofission of Gold and Uranium

NUCLEAR REACTIONS 197Au, 238U(γ, F), Eγ < 0.8, 1.0, 1.2, 1.5, 1.8, 2.0, 2.2 GeV; measured σ(Q) per number of equivalent quanta; deduced mass distributions, forward-backward ratios.

doi: 10.1016/0375-9474(72)90753-1
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetL0095.


1972VO13      Nucl.Phys. A195, 617 (1972)

W.Von Witsch, W.Viefers, H.Mommsen, P.David, F.Hinterberger

Test of the Treiman-Yang Criterion in the 2H(d, pd)n Reaction at 20 MeV Bombarding Energy

NUCLEAR REACTIONS 2H(d, pd), E=20 MeV; measured σ(Ep, Ed, θ(p), θ(d), phi(p), phid). Enriched target.

doi: 10.1016/0375-9474(72)91083-4
Citations: PlumX Metrics


1971BE42      Nucl.Phys. A171, 401 (1971)

M.G.Betigeri, P.David, J.Debrus, H.Mommsen, A.Riccato

Study of the Reactions 66Zn(3He, d)67Ga and 66Zn(3He, α)65Zn

NUCLEAR REACTIONS 66Zn(3He, d), 66Zn(3He, α), E(3He)=18 MeV; measured σ(Ed, θ), σ(Eα, θ). 65Zn, 67Ga deduced levels, J, π, L, isobaric analogs, S. Enriched target 66Zn.

doi: 10.1016/0375-9474(71)90030-3
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1162.


1969DA02      Nucl.Phys. A128, 47 (1969)

P.David, H.H.Duhm, R.Bock, R.Stock

(3He, α) Reactions on the Chromium Isotopes

NUCLEAR REACTIONS 50,52,53,54Cr(3He, α), E=18 MeV; measured σ(Eα, θ). 49,51,52,53Cr deduced levels, L-values, S. Enriched targets.

doi: 10.1016/0375-9474(69)90978-6
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1223.


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