NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = P.David Found 48 matches. 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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
1974RI08 Nucl.Phys. A228, 461 (1974) 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
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
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
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
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
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
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