NSR Query Results
Output year order : Descending NSR database version of May 6, 2024. Search: Author = D.M.Drake Found 72 matches. 2021LI47 Nucl.Sci.Eng. 195, 1131 (2021) P.W.Lisowski, M.Drosg, D.M.Drake, B.Hoop Cross Sections for Neutron Production from 6- and 10-MeV Neutrons Incident on 10B and 11B NUCLEAR REACTIONS 10,11B(n, X)1NN, E=6, 10 MeV; measured reaction products, TOF, En, In; deduced neutron yields, σ(θ, E). Comparison with ENDF/B-VIII evaluations.
doi: 10.1080/00295639.2021.1906588
2016DR01 Nucl.Sci.Eng. 182, 256 (2016) Neutron Emission Spectra of Triton Beams of 20.22-MeV Fully Stopped in Targets of H20, D2O, LiF, Si, Ni, Mo, Ta, W, Pt, and Au NUCLEAR REACTIONS 1,2H, O, 6,7Li, 19F, Si, Ni, Mo, Ta, W, Pt, 197Au(t, X), E=15.2, 17.2 MeV; measured reaction products, En, In; deduced neutron yields, σ(θ, E).
doi: 10.13182/NSE15-17
2016DR07 Nucl.Sci.Eng. 183, 298 (2016) Double-Differential Angle--Dependent Three-Body Neutron Production Cross Sections of the Reaction 2H(t, n)X+Y at Triton Energies Between 5.97 and 16.41 MeV NUCLEAR REACTIONS 2H(t, n), E=5.97-16.41 MeV; measured reaction products, En, In; deduced σ(θ, E) and uncertainties. Comparison with available data.
doi: 10.13182/NSE15-118
2016DR09 Nucl.Sci.Eng. 184, 114 (2016) M.Drosg, M.M.Steurer, E.Jericha, D.M.Drake Angle-Dependent Double-Differential Neutron Emission Cross Sections of 3H(t, n) Between 5.98 and 19.14 MeV and Evidence of 4H as Intermediate Reaction Product NUCLEAR REACTIONS 3H(t, n)5He, 3H(t, 2n)4He, E=5.98-19.14 MeV; measured reaction products, En, In; deduced σ(θ, E) and their uncertainties.
doi: 10.13182/NSE16-56
2007CA24 Nucl.Instrum.Methods Phys.Res. B260, 508 (2007) C.M.Castaneda, D.G.Gearhart, R.M.Gearhart, B.Sanii, P.A.J.Englert, J.F.Dempsey, J.C.Young, D.M.Drake, R.C.Reedy Gamma ray production cross sections from the bombardment of Mg, Al, Si, Ca and Fe with medium energy neutrons NUCLEAR REACTIONS Mg, Al, Si, Ca, Fe(n, γX), E=6.5, 17.4, 22.2, 32.5, 42.1, 64.5 MeV; measured Eγ, Iγ, production cross sections. Compared results to model calculations.
doi: 10.1016/j.nimb.2007.04.019
2002BE08 Phys.Rev. C65, 021601 (2002) L.A.Bernstein, J.A.Becker, P.E.Garrett, W.Younes, D.P.McNabb, D.E.Archer, C.A.McGrath, H.Chen, W.E.Ormand, M.A.Stoyer, R.O.Nelson, M.B.Chadwick, G.D.Johns, W.S.Wilburn, M.Devlin, D.M.Drake, P.G.Young 239Pu(n, 2n)238Pu Cross Section Deduced using a Combination of Experiment and Theory NUCLEAR REACTIONS 239Pu(n, 2n), E < 20 MeV; measured Eγ, Iγ, partial γ-ray σ; deduced σ, possible nuclear structure effects. Comparisons with model predictions. Geanie array.
doi: 10.1103/PhysRevC.65.021601
2002TA15 Nucl.Phys. A701, 303c (2002) W.L.Talbert, D.M.Drake, M.T.Wilson, J.W.Lenz, H.-H.Hsu Conductive Cooling of High-Power RIB Targets
doi: 10.1016/S0375-9474(01)01603-7
2001BE11 Nucl.Phys. A682, 404c (2001) L.A.Bernstein, D.E.Archer, J.A.Becker, P.E.Garrett, K.Hauschild, C.A.McGrath, D.P.McNabb, W.Younes, M.Devlin, D.M.Drake, G.D.Johns, R.O.Nelson Studying the Role of Nuclear Structure Effects in Neutron-Induced Reactions using GEANIE at LANSCE NUCLEAR REACTIONS 92Mo(n, xnypzα)91Nb/88Zr/89Zr/91Mo/92Mo/84Sr, E ≈ 1-600 MeV; measured Eγ, Iγ, γ-ray excitation functions. 91Mo deduced isomer T1/2. 239Pu(n, 2n), E=5-20 MeV; measured σ. 235U(n, F), E=0-250 MeV; measured fission yields. Geanie array.
doi: 10.1016/S0375-9474(00)00667-9
2001YO10 Phys.Rev. C64, 054613 (2001) W.Younes, J.A.Becker, L.A.Bernstein, P.E.Garrett, C.A.McGrath, D.P.McNabb, R.O.Nelson, G.D.Johns, W.S.Wilburn, D.M.Drake Transition from Asymmetric to Symmetric Fission in the 235U(n, f) Reaction NUCLEAR REACTIONS 235U(n, F), E=1-250 MeV; measured prompt Eγ, Iγ, γγ-coin; deduced γ-ray yields, fission fragment charge and mass distributions vs excitation energy. Disappearance of shell structure at high excitation energy discussed.
doi: 10.1103/PhysRevC.64.054613
1998BE21 Phys.Rev. C57, R2799 (1998) L.A.Bernstein, J.A.Becker, W.Younes, D.E.Archer, K.Hauschild, G.D.Johns, R.O.Nelson, W.S.Wilburn, D.M.Drake Probing Reaction Dynamics with the 196Pt(n, xnγ) Reactions for x ≤ 15 NUCLEAR REACTIONS 196Pt(n, xn), E=3-250 MeV; measured Eγ, Iγ; deduced fractional yields. Model comparison.
doi: 10.1103/PhysRevC.57.R2799
1997VO03 Phys.Rev. C55, 2458 (1997) H.Vonach, A.Pavlik, A.Wallner, M.Drosg, R.C.Haight, D.M.Drake, S.Chiba Spallation Reactions in 27Al and 56Fe Induced by 800 MeV Protons NUCLEAR REACTIONS, ICPND 27Al(p, X)28Si/25Na/24Na/22Na/23Ne/18Ne/23F/22F/21F/20F/20O/19O/14O, E=800 MeV; 56Fe(p, X)56Co/53Fe/54Mn/52Mn/52mMn/50mMn/51Cr/49Cr/48Cr/53V/48V/51Ti/48Sc/47Sc/46Sc/44gSc/44mSc/43Sc/42mSc/42K/38mK/41Ar/39Cl/38Cl/34Cl/32Cl/38S/37S/35P/33Si/26Si/30Al/29Al/28Al/28Mg/27Mg/25Na/24Na/22Na/23Ne/20F, E=800 MeV; measured γ production σ, discrete γ lines; deduced nuclide production σ.
doi: 10.1103/PhysRevC.55.2458
1994DR10 Nucl.Instrum.Methods Phys.Res. B84, 337 (1994) D.M.Drake, M.Drosg, R.C.Byrd, R.C.Reedy, D.A.Clark, P.A.J.Englert, J.F.Dempsey, S.G.Bobias, L.Harris Experimental and Numerical Simulation of Martian Neutron Distributions
doi: 10.1016/0168-583X(94)95726-6
1994DR11 Nucl.Instrum.Methods Phys.Res. B94, 319 (1994) Calibration of a Li-Glass Detector for Neutron Energies Above 50 keV by the 1H(t, n)3He Reaction NUCLEAR REACTIONS 6Li(n, t), E ≤ 10 MeV; measured σ(E); deduced Li-glass detector calibration for E(n) > 50 keV. Neutrons from 1H(t, n) reaction.
doi: 10.1016/0168-583X(94)95371-6
1993DR03 Nucl.Instrum.Methods Phys.Res. B73, 387 (1993) Fast Neutron Yield from 20-MeV Tritons on Water Part I. Triton Interaction with Light Water NUCLEAR REACTIONS 1H, 16O(t, n), E=20 MeV; measured σ(θn, En); deduced σ(θ) for (t, n0) reaction. Water target.
doi: 10.1016/0168-583X(93)95756-U
1993DR04 Nucl.Instrum.Methods Phys.Res. B73, 392 (1993) M.Drosg, D.M.Drake, R.C.Haight, R.O.Nelson Fast Neutron Yield from 20-MeV Tritons on Water Part II. Triton Interaction with Heavy Water NUCLEAR REACTIONS 2H, 16O(t, n), E=20 MeV; measured σ(θn, En); deduced neutron yield for 16O(t, n), 2H+t breakup reactions. Heavy water target.
doi: 10.1016/0168-583X(93)95757-V
1992RO17 Phys.Rev. C46, 1968 (1992) D.P.Rosenzweig, J.F.Amann, R.L.Boudrie, K.G.R.Doss, D.M.Drake, I.Halpern, M.A.Khandaker, J.Nelson, D.W.Storm, D.R.Tieger, S.A.Wood Comparison of Inclusive Inelastic Scattering of π+ and π- from Nuclei at 100 MeV NUCLEAR REACTIONS 12C, 40Ca, Sn, Pb(π+, π+'X), (π-, π-'X), E=100 MeV; measured σ(E(π), θ); deduced σ(ratios), relations between pion absorption and scattering. Semiclassical transport model.
doi: 10.1103/PhysRevC.46.1968
1990FE02 Nucl.Instrum.Methods Phys.Res. A287, 595 (1990) W.C.Feldman, G.F.Auchampaugh, D.M.Drake A Technique to Measure the Neutron Lifetime from Low-Earth Orbit RADIOACTIVITY 1n(β-); analyzed, discussed mean T1/2 measurement techniques. Low-earth orbit.
doi: 10.1016/0168-9002(90)91584-X
1990HA19 Phys.Rev. C41, 2556 (1990) A.Hakansson, A.Lindholm, L.Nilsson, J.Blomgren, P.-O.Soderman, D.M.Drake, S.A.Wender, N.Olsson 12C(n, γ0)13C Cross Section in the 8-11 MeV Region NUCLEAR REACTIONS 12C(n, γ), E=8-11 MeV; measured σ(θ=90°).
doi: 10.1103/PhysRevC.41.2556
1990LI15 Nucl.Phys. A511, 643 (1990) J.Lisantti, D.K.McDaniels, Z.Tang, Z.Xu, D.M.Drake, K.H.Hicks, M.C.Vetterli, L.W.Swenson, X.Y.Chen, F.Farzanpay Elastic and Inelastic Scattering of 280 and 489 MeV Protons from 58Ni NUCLEAR REACTIONS 58Ni(p, p), (p, p'), E=280, 489 MeV; measured σ(θ), analyzing power vs θ; deduced model parameters. 58Ni levels deduced neutron to proton multipole matrix elements ratio.
doi: 10.1016/0375-9474(90)90115-3
1989CH39 Nucl.Phys. A505, 670 (1989) X.Y.Chen, L.W.Swenson, F.Farzanpay, D.K.McDaniels, Z.Xu, Z.Tang, D.M.Drake, I.Bergqvist, A.Brockstedt, J.Lisantti, F.Bertrand, D.J.Horen, K.Hicks, M.Vetterli, M.J.Iqbal Analyzing Powers and Cross Sections of Inclusive Polarized Proton Scattering on 208Pb NUCLEAR REACTIONS 208Pb(polarized p, p'), E=290, 500 MeV; measured σ(θ), analyzing power vs θ. DWBA, relativistic impulse approximation analyses.
doi: 10.1016/0375-9474(89)90037-7
1988BR06 Phys.Rev. C37, 1345 (1988) G.Bruge, D.Garreta, P.Birien, H.Catz, A.Chaumeaux, S.Janouin, D.Legrand, M.C.Lemaire, B.Mayer, J.Pain, F.Perrot, E.Aslanides, O.Bing, D.M.Drake, J.C.Peng, M.Berrada, J.P.Bocquet, E.Monnand, J.Mougey, P.Perrin, J.Lichtenstadt, A.I.Yavin Elastic Scattering of 179.3 MeV Antiprotons by Deuterium NUCLEAR REACTIONS 2H(p-bar, p-bar), E=179.3 MeV; measured σ(θ).
doi: 10.1103/PhysRevC.37.1345
1988CH13 Phys.Lett. 205B, 436 (1988) X.Y.Chen, L.W.Swenson, F.Farzanpay, D.K.McDaniels, Z.Tang, Z.Xu, D.M.Drake, I.Bergqvist, A.Brockstedt, F.E.Bertrand, D.J.Horen, J.Lisantti, K.Hicks, M.Vetterli, M.J.Iqbal Relativistic Medium Effects for 208Pb(p(pol), p') at Intermediate Energies NUCLEAR REACTIONS 208Pb(polarized p, p'), E=290 MeV; measured σ(θp', Ep'), analyzing power vs θ; deduced relativistic medium effects.
doi: 10.1016/0370-2693(88)90973-2
1987AS06 Nucl.Phys. A470, 445 (1987) E.Aslanides, D.M.Drake, J.C.Peng, D.Garreta, P.Birien, G.Bruge, H.Catz, A.Chaumeaux, S.Janouin, D.Legrand, M.-C.Lemaire, B.Mayer, J.Pain, F.Perrot, M.Berrada, J.P.Bocquet, E.Monnand, J.Mougey, P.Perrin, O.Bing, J.Lichtenstadt, A.I.Yavin Search for p-bar-Nucleus States using the (p-bar, p) Knock-Out Reaction at 600 MeV/c NUCLEAR REACTIONS 1,2H, 6Li, 12C, 63Cu, 208Pb, 209Bi(p-bar, p), E=180 MeV; measured σ(Ep, θ=0°); deduced temperatures, proton production σ, mass dependence, effective proton number, quasifree σ(θ=0°).
doi: 10.1016/0375-9474(87)90580-X
1986BE17 Nucl.Phys. A456, 426 (1986) I.Bergqvist, D.M.Drake, D.K.McDaniels, S.A.Wender, A.Lindholm, L.Nilsson, N.Olsson, R.Zorro, F.S.Dietrich The 12C(n, γ0)13C Reaction in the Giant Resonance Region NUCLEAR REACTIONS 12C(n, γ), E=7-19.5 MeV; measured σ(E, θ=90°). 13C deduced giant, pygmy resonances. DSD model, 12,13C(n, γ) data input.
doi: 10.1016/0375-9474(86)90403-3
1986BR04 Phys.Lett. 169B, 14 (1986) G.Bruge, A.Chaumeaux, P.Birien, D.M.Drake, D.Garreta, S.Janouin, D.Legrand, M.C.Lemaire, B.Mayer, J.Pain, M.Berrada, J.P.Bocquet, E.Monnand, J.Mougey, P.Perrin, E.Aslanides, O.Bing, J.Lichtenstadt, A.I.Yavin, J.C.Peng Comparative Study of the Elastic Scattering of 178.4 MeV Antiprotons by the 16O and 18O Isotopes NUCLEAR REACTIONS 16,18O(p-bar, p-bar), E=178.4 MeV; measured σ(θ); deduced optical model parameters, neutron excess role.
doi: 10.1016/0370-2693(86)90676-3
1986CI06 Nucl.Phys. A459, 438 (1986) N.Cindro, D.Pocanic, D.M.Drake, J.D.Moses, J.C.Peng, N.Stein, J.W.Sunier Elastic Scattering of 28Si on 24Mg and 26Mg NUCLEAR REACTIONS 26,24Mg(28Si, 28Si), E=74.5-83 MeV; 24Mg(28Si, 24Mg), (28Si, 26Mg), E=83 MeV; measured σ(θ), σ(E); deduced intermediate structure.
doi: 10.1016/0375-9474(86)90144-2
1986DR10 Radiat.Eff. 92, 145 (1986) M.Drosg, P.W.Lisowski, R.A.Hardekopf, D.M.Drake, K.Treitl Double Differential Neutron Emission Cross Sections of 10B and 11B at 6, 10 and 14 MeV and of 6Li, 7Li and 12C at 14 MeV NUCLEAR REACTIONS 10,11B(n, xn), E=6, 10, 14.1 MeV; 6,7Li, C(n, xn), E=14.1 MeV; measured σ(θ, En); deduced elastic, total emission, reaction σ.
doi: 10.1080/00337578608208308
1986JA04 Nucl.Phys. A451, 541 (1986) S.Janouin, M.-C.Lemaire, D.Garreta, P.Birien, G.Bruge, D.M.Drake, D.Legrand, B.Mayer, J.Pain, J.C.Peng, M.Berrada, J.P.Bocquet, E.Monnand, J.Mougey, P.Perrin, E.Aslanides, O.Bing, J.Lichtenstadt, A.I.Yavin Optical-Model Analysis of Antiproton-Nucleus Elastic Scattering at 50 and 180 MeV NUCLEAR REACTIONS 12C, 40Ca, 208Pb(p-bar, p-bar), E ≈ 50, 180 MeV; 16,18O(p-bar, p-bar), E=178.4 MeV; analyzed σ(θ); deduced reaction σ, potential parameters.
doi: 10.1016/0375-9474(86)90291-5
1986LE13 Nucl.Phys. A456, 557 (1986) M.-C.Lemaire, P.Birien, G.Bruge, D.M.Drake, D.Garreta, S.Janouin, D.Legrand, B.Mayer, J.Pain, J.C.Peng, M.Berrada, J.P.Bocquet, E.Monnand, J.Mougey, P.Perrin, E.L.Aslanides, O.Bing, J.Lichtenstadt, A.I.Yavin Inelastic Scattering of Antiprotons from 12C and 18O at 50 and 180 MeV NUCLEAR REACTIONS 18O, 12C(p-bar, p-bar), (p-bar, p-bar'), E=46.7, 179.7, 178.4 MeV; measured σ(θ); deduced potential parameters. 12C deduced quadrupole deformation parameters, deformation lengths, B(λ), δ. 18O deduced quadrupole, hexadecapole deformation lengths.
doi: 10.1016/0375-9474(86)90075-8
1986MC06 Phys.Rev. C33, 1943 (1986) D.K.McDaniels, J.R.Tinsley, J.Lisantti, D.M.Drake, I.Bergqvist, L.W.Swenson, F.E.Bertrand, E.E.Gross, D.J.Horen, T.P.Sjoreen, R.Liljestrand, H.Wilson Cross Section and Analyzing Power Measurements for the Giant Resonance Region in 208Pb with 200-MeV Protons NUCLEAR REACTIONS 208Pb(polarized p, p'), (p, p'), E=200 MeV; measured σ(Ep'), σ(θ), analyzing power vs θ. 208Pb deduced isoscalar GQR, monopole resonance, isovector GDR, J, π, B(λ), hexadecapole transition EWSR, Γ.
doi: 10.1103/PhysRevC.33.1943
1986MO05 Phys.Rev. C33, 1224 (1986) G.L.Morgan, P.W.Lisowski, S.A.Wender, R.E.Brown, N.Jarmie, J.F.Wilkerson, D.M.Drake Measurement of the Branching Ratio 3H(d, γ)/3H(d, n) using Thick Tritium Gas Targets NUCLEAR REACTIONS, ICPND 3H(d, γ), (d, n), E=0.0-0.72 MeV; measured Eγ, Iγ, En, relative γ yield. 5He resonance deduced branching ratio.
doi: 10.1103/PhysRevC.33.1224
1985CO22 Z.Phys. A322, 491 (1985) M.D.Cohler, R.Wadsworth, S.M.Lane, D.L.Watson, M.J.Smithson, R.E.Brown, D.M.Drake, N.Stein, J.-C.Peng, J.W.Sunier Investigation of a Possible Abrupt Change in Structure at N = 58-60 using Two-Proton Transfer NUCLEAR REACTIONS 106,110,112,116Cd(14C, 14C), (14C, 16O), E=60 MeV; measured σ(θ); deduced optical model parameters. 104,108,110,114Pd levels deduced relative S.
doi: 10.1007/BF01412085
1985DO10 Phys.Rev. C32, 92 (1985) J.C.Dousse, E.D.Arthur, D.M.Drake, J.Gursky, J.D.Moses, N.Stein, J.W.Sunier Coincident Neutron-Proton Emission from Proton Bombardment of 87Sr and 91Zr NUCLEAR REACTIONS, ICPND 87Sr, 91Zr(p, pn), E=14-17.6 MeV; measured σ(θ1, θ2), σ(E); deduced optical model parameters. Two Tof systems. Hauser-Feshbach multi-step statistical model calculations.
doi: 10.1103/PhysRevC.32.92
1985GA02 Phys.Lett. 150B, 95 (1985) D.Garreta, P.Birien, G.Bruge, A.Chaumeaux, D.M.Drake, S.Janouin, D.Legrand, M.C.Lemaire, B.Mayer, J.Pain, J.C.Peng, M.Berrada, J.P.Bocquet, E.Monnand, J.Mougey, P.Perrin, E.Aslanides, O.Bing, J.Lichtenstadt, A.I.Yavin Search for Antiproton-Nucleus States with (p-bar, p) Reactions NUCLEAR REACTIONS 12C, 63Cu, 209Bi(p-bar, pX), E=180 MeV; measured inclusive σ(θ, Ep); deduced no (p-bar)-nucleus states. Intranuclear cascade model.
doi: 10.1016/0370-2693(85)90146-7
1984CO19 Z.Phys. A319, 107 (1984) M.D.Cohler, D.L.Watson, R.Wadsworth, S.M.Lane, M.J.Smithson, R.E.Brown, J.-C.Peng, N.Stein, J.W.Sunier, D.M.Drake Measurement of the Mass of 110Pd and 114Pd using the (14C, 16O) Reaction NUCLEAR REACTIONS 112,114Cd(14C, 16O), E=60 MeV; measured σ(E(16O)). 110,114Pd deduced mass. Enriched target. Mass model comparison.
doi: 10.1007/BF01429774
1984GA04 Phys.Lett. 135B, 266 (1984) D.Garreta, P.Birien, G.Bruge, A.Chaumeaux, D.M.Drake, S.Janouin, D.Legrand, M.C.Mallet-Lemaire, B.Mayer, J.Pain, J.C.Peng, M.Berrada, J.P.Bocquet, E.Monnand, J.Mougey, P.Perrin, E.Aslanides, O.Bing, A.Erell, J.Lichtenstadt, A.I.Yavin Scattering of Antiprotons from Carbon at 46.8 MeV NUCLEAR REACTIONS 12C(p-bar, p-bar), (p-bar, p-bar'), E=46.8 MeV; calculated σ(E(p-bar)), σ(θ); deduced (p-bar)-carbon optical potential parameter limits.
doi: 10.1016/0370-2693(84)90388-5
1984GA32 Phys.Lett. 149B, 64 (1984) D.Garreta, P.Birien, G.Bruge, A.Chaumeaux, D.M.Drake, S.Janouin, D.Legrand, M.C.Lemaire, B.Mayer, J.Pain, J.C.Peng, M.Berrada, J.P.Bocquet, E.Monnand, J.Mougey, P.Perrin, E.Aslanides, O.Bing, J.Lichtenstadt, A.I.Yavin Elastic Scattering of Antiprotons from Carbon, Calcium, and Lead at 180 MeV NUCLEAR REACTIONS 12C, 40Ca, 208Pb(p-bar, p-bar), E=180 MeV; measured σ(θ); deduced potential parameters. Optical model analysis.
doi: 10.1016/0370-2693(84)91552-1
1984LI19 Phys.Lett. 147B, 23 (1984) J.Lisantti, J.R.Tinsley, D.M.Drake, I.Bergqvist, L.W.Swenson, D.K.McDaniels, F.E.Bertrand, E.E.Gross, D.J.Horen, T.P.Sjoreen Analyzing Power for the Inelastic Continuum with 200 MeV Protons NUCLEAR REACTIONS 60Ni, 90Zr, 208Pb(p, p'X), (polarized p, p'X), E=200 MeV; measured inclusive σ(Ep'), σ(θ), analyzing power vs θ; deduced reaction mechanism excitation energy dependence.
doi: 10.1016/0370-2693(84)90584-7
1984WA05 J.Phys.(London) G10, L79 (1984) R.Wadsworth, M.D.Cohler, S.M.Lane, M.J.Smithson, D.L.Watson, R.E.Brown, D.M.Drake, J.-C.Peng, N.Stein, J.W.Sunier A Study of the (14C, 16O) Reaction in the Mass-100 Region NUCLEAR REACTIONS 96,100,102,104Ru, 106,108,110Pd(14C, 16O), E=60 MeV; measured σ(θ). 94,98,100,102Mo, 104,106,108Ru levels deduced relative spectroscopic factors. 96,102,104Ru, 106,108,110Pd(14C, 14C), E=60 MeV; 100Mo(16O, 16O), E=65 MeV; measured σ(θ); deduced optical model parameters. Exact finite-range DWBA analysis.
doi: 10.1088/0305-4616/10/4/003
1983DR13 Nucl.Phys. A410, 429 (1983) D.M.Drake, N.R.Roberson, S.A.Wender, H.R.Weller Polarized Triton Capture on 12C NUCLEAR REACTIONS 12C(t, γ), (polarized t, γ), E=2.3-6.5 MeV; measured σ(E, θ), A(θ). Direct capture model calculation.
doi: 10.1016/0375-9474(83)90635-8
1983MA20 Nucl.Sci.Eng. 84, 98 (1983) R.L.Macklin, D.M.Drake, E.D.Arthur Neutron Capture Cross Sections of 182W, 183W, 184W, and 186W from 2.6 to 2000 keV NUCLEAR REACTIONS 182,183,184,186W(n, γ), E=2.6-2000 keV; measured σ(capture) vs E. 184W deduced resonances, J, π, (gΓγΓn/Γ). 183,185,187W deduced resonances, J, π, (gΓγΓn/Γ), < Γγ >/D, s-, p-, d-wave strength functions, average level spacing.
doi: 10.13182/NSE83-A17717
1983TI03 Phys.Rev. C28, 1417 (1983) J.R.Tinsley, D.K.McDaniels, J.Lisantti, L.W.Swenson, R.Liljestrand, D.M.Drake, F.E.Bertrand, E.E.Gross, D.J.Horen, T.P.Sjoreen Observation of 2(h-bar x omega) Hexadecapole Strength in Lead Nuclei from 200 MeV Inelastic Proton Scattering NUCLEAR REACTIONS 206,208Pb(p, p'), E=200 MeV; measured σ(Ep'), σ(θ). 208Pb deduced isosclar giant resonance L, Γ, B(E4).
doi: 10.1103/PhysRevC.28.1417
1982JO01 Nucl.Phys. A382, 71 (1982) S.Joly, G.Grenier, D.M.Drake, I.Bergqvist, D.K.McDaniels, A.Lindholm, L.Nilsson, N.Olsson, A.Waheed, R.Zorro, F.Rigaud Study of the 208Pb(n, γ0)209Pb Reaction between 0.8 and 7.7 MeV NUCLEAR REACTIONS 208Pb(n, γ), E=0.8-7.7 MeV; measured σ(E, θ). Compound nucleus, direct-semidirect model analyses.
doi: 10.1016/0375-9474(82)90441-9
1982MA33 Nucl.Sci.Eng. 82, 143 (1982) R.L.Macklin, D.M.Drake, J.J.Malanify, E.D.Arthur, P.G.Young Cross Section of the 169Tm(n, γ) Reaction from 2.6 keV to 2 MeV NUCLEAR REACTIONS 169Tm(n, γ), E=3-2000 keV; measured σ(capture). 170Tm deduced resonances, parameters, s-, p-, d-wave strength functions.
doi: 10.13182/NSE82-A28697
1982MC08 Nucl.Phys. A384, 88 (1982) D.K.McDaniels, P.Varghese, D.M.Drake, E.Arthur, A.Lindholm, I.Bergqvist, J.Krumlinde Radiative Capture of Fast Neutrons by 165Ho and 238U NUCLEAR REACTIONS 165Ho, 238U(n, γ), E=7-15 MeV; measured σ(θ), σ(total) vs E. Direct-semidirect model.
doi: 10.1016/0375-9474(82)90306-2
1981DR01 Phys.Lett. B98, 36 (1981) D.M.Drake, M.Cates, N.Cindro, D.Pocanic, E.Holub Gross Structure and Resonant Behaviour of 14C + 14C Elastic Scattering NUCLEAR REACTIONS 14C(14C, 14C), E=23.4-58.4 MeV; measured σ(θ, E); deduced gross structure, resonant behavior. Optial model analysis.
doi: 10.1016/0370-2693(81)90362-2
1981DR02 Phys.Lett. 100B, 236 (1981) D.M.Drake, J.D.Moses, J.C.Peng, N.Stein, J.W.Sunier Large Angle Scattering of 16O by 24,25,26Mg by Detecting the Heavy Mass Recoil NUCLEAR REACTIONS 24Mg(16O, 24Mg), E=45-58.5 MeV; 25Mg(16O, 25Mg), E=47-59 MeV; 26Mg(16O, 26Mg), E=43.5-58 MeV; measured σ(E); deduced gross resonance structure. Q3D spectrometer.
doi: 10.1016/0370-2693(81)90324-5
1981DR08 Phys.Rev.Lett. 47, 1581 (1981) D.M.Drake, S.Joly, L.Nilsson, S.A.Wender, K.Anoil, I.Halpern, D.Storm E2 Isovector Giant Resonance as Seen through the Capture of Fast Neutrons NUCLEAR REACTIONS 208Pb(n, γ), E=7-20 MeV; measured σ(Eγ), asymmetry. 209Pb deduced E2 giant isovector resonance.
doi: 10.1103/PhysRevLett.47.1581
1980DR09 Phys.Rev.Lett. 45, 1765 (1980) D.M.Drake, J.D.Moses, J.C.Peng, N.Stein, J.W.Sunier Exotic Heavy-Ion Reactions on 40Ca: (14C, 14O) Double Charge Exchange and (14C, 15O) Rearrangement Transfer NUCLEAR REACTIONS 40Ca(14C, 14O), (14C, 15O), (14C, 16O), (14C, 15N), E=51 MeV; measured σ(θ). 38,39,40Ar, 39K levels deduced excitation probability. DWBA analysis, double charge exchange, rearrangement transfer processes.
doi: 10.1103/PhysRevLett.45.1765
1980NI02 Phys.Rev. C21, 902 (1980) L.Nilsson, M.Drosg, D.M.Drake, A.Lindholm Isospin Structure of the Giant Dipole Resonance in 41Ca NUCLEAR REACTIONS 40K(p, γ), E=8.5-16.6 MeV; measured σ(E); deduced isospin effects on GDR. direct-semidirect model.
doi: 10.1103/PhysRevC.21.902
1979CI02 Phys.Lett. 84B, 55 (1979) N.Cindro, J.D.Moses, N.Stein, M.Cates, D.M.Drake, D.L.Hanson, J.W.Sunier Resonances in 36Ar via the 24Mg(12C, α)32S Reaction NUCLEAR REACTIONS 24Mg(12C, α), E=27.5-35.5 MeV; measured σ(E, θ); deduced reaction mechanism. Legendre polynomial analysis.
doi: 10.1016/0370-2693(79)90647-6
1979DR13 Nucl.Instrum.Methods 160, 143 (1979) 180 Degree n-p Cross Sections For Fast Neutron Measurements With Counter Telescopes NUCLEAR REACTIONS 1H(n, n), E=25.3-31.1 MeV; measured products, Eπ, Iπ; deduced σ(θ). Data were imported from EXFOR entry 10804.
doi: 10.1016/0029-554X(79)90177-0
1979JO03 Nucl.Sci.Eng. 70, 53 (1979) S.Joly, J.Voignier, G.Grenier, D.M.Drake, L.Nilsson Neutron Capture Cross Sections of Rhodium, Thulium, Iridium, and Gold between 0.5 and 3.0 MeV NUCLEAR REACTIONS Rh, Tm, Au, Ir(n, γ), E=0.5-3.0 MeV; measured σ.
doi: 10.13182/NSE79-A18926
1979JO10 Phys.Rev. C20, 2072 (1979) Gamma-Ray Strength Functions for 104Rh, 170Tm, and 198Au NUCLEAR REACTIONS 103Rh, 169Tm, 197Au(n, γ), E=0.5-3.0 MeV; measured σ(E, Eγ). 104Rh, 170Tm, 198Au deduced γ-ray strength functions, Γγ.
doi: 10.1103/PhysRevC.20.2072
1979PE08 Phys.Rev.Lett. 43, 675 (1979) J.C.Peng, N.Stein, J.W.Sunier, D.M.Drake, J.D.Moses, J.A.Cizewski, J.R.Tesmer Study of the Reactions 46,48Ti(14C, 16O)44,46Ca and 50,52Cr(14C, 16O)48,50Ti at 51 MeV NUCLEAR REACTIONS 46,48Ti, 50,52Cr(14C, 16O), E=51 MeV; measured σ(θ). 44,46Ca levels deduced configuration, S, reaction mechanism. Finite range DWBA calculations.
doi: 10.1103/PhysRevLett.43.675
1978BE11 Nucl.Phys. A295, 256 (1978) I.Bergqvist, B.Palsson, L.Nilsson, A.Lindholm, D.M.Drake, E.Arthur, D.K.McDaniels, P.Varghese Radiative Capture of Fast Neutrons by 89Y and 140Ce NUCLEAR REACTIONS 89Y, 140Ce(n, γ), E=6.2-15.6 MeV; measured σ(n, γ) at 90°. Compare with theory.
doi: 10.1016/0375-9474(78)90114-8
1978DR03 Nucl.Sci.Eng. 65, 49 (1978) D.M.Drake, E.D.Arthur, M.G.Silbert Cross Sections for Gamma-Ray Production by 14-MeV Neutrons NUCLEAR REACTIONS Be, C, Mg, Al, Si, Cr, Fe, Ca, Ti, V, Ni, Cu, Nb, Mo, Ta, Pt, Th, 235,238U, 239Pu(n, X), E=14.2 MeV; measured integral σ(Eγ).
doi: 10.13182/NSE78-A27125
1977DR09 Nucl.Sci.Eng. 63, 401 (1977) D.M.Drake, G.F.Auchampaugh, E.D.Arthur, C.E.Ragan, P.G.Young Double-Differential Beryllium Neutron Cross Sections at Incident Neutron Energies of 5.9, 10.1, and 14.2 MeV NUCLEAR REACTIONS Be(n, 2n), E=5.9, 10.1, 14.2 MeV; measured σ(θ).
doi: 10.13182/NSE77-A27057
1976SH01 Phys.Rev.Lett. 36, 82 (1976) Y.Shamai, J.Alster, D.Ashery, S.Cochavi, M.A.Moinester, A.I.Yavin, E.D.Arthur, D.M.Drake Measurements of the (π+, π0) Reaction on Light Elements in the (3, 3)-Resonance Region NUCLEAR REACTIONS 7Li, 10B, 13C(π+, π0), E=70-250 MeV; measured σ(E). Activation technique.
doi: 10.1103/PhysRevLett.36.82
1975AR19 Phys.Rev.Lett. 35, 914 (1975) E.D.Arthur, D.M.Drake, I.Halpern Fore-Aft Anisotropy in the Radiative Capture of 14-MeV Neutrons NUCLEAR REACTIONS 10B, 12C, 29Si, 40Ca(n, γ), E=14 MeV; measured γ-yields, Iγ(θ).
doi: 10.1103/PhysRevLett.35.914
1975JA13 Phys.Rev.Lett. 35, 641 (1975) H.E.Jackson, D.G.Kovar, L.Meyer-Schutzmeister, R.E.Segel, J.P.Schiffer, S.Vigdor, T.P.Wangler, R.L.Burman, D.M.Drake, P.A.M.Gram, R.P.Redwine, V.G.Lind, E.N.Hatch, O.H.Otteson, R.E.McAdams, B.C.Cook, R.B.Clark Systematics of Pion and Proton Interactions with Ni Nuclides NUCLEAR REACTIONS 58,60Ni(π+, X), (π-, X), E=220 MeV; 58,60Ni(p, X), E=200 MeV; 58Ni(π+, X), E=100 MeV; measured σ(fragment) from γ-spectra.
doi: 10.1103/PhysRevLett.35.641
1975JA15 Phys.Rev.Lett. 35, 1170 (1975) H.E.Jackson, D.G.Kovar, L.Meyer-Schutzmeister, S.E.Vigdor, T.P.Wangler, R.E.Segel, J.P.Schiffer, R.L.Burman, P.A.M.Gram, D.M.Drake, V.G.Lind, E.N.Hatch, O.H.Otteson, R.E.McAdams, B.C.Cook, R.B.Clark Absolute Cross Sections for Production of Prompt Nuclear γ Rays by Fast Pions NUCLEAR REACTIONS 27Al(π+, X), E=100 MeV; 51V, 40Ca(π-, X), E=220 MeV; 60Ni(π-, X), (π+, X), E=380 MeV; measured σ(Eγ).
doi: 10.1103/PhysRevLett.35.1170
1974BE55 Nucl.Phys. A231, 29 (1974) I.Bergqvist, D.M.Drake, D.K.McDaniels Radiative Capture of Fast Neutrons by 40Ca NUCLEAR REACTIONS 40Ca(n, γ), E=6.8-18.2 MeV; measured σ(E, Eγ); deduced reaction mechanism.
doi: 10.1016/0375-9474(74)90291-7
1974DR09 Nucl.Sci.Eng. 55, 427 (1974) Cross Sections of Uranium-235 and Plutonium-239 for Neutrons Producing Gamma Rays NUCLEAR REACTIONS 235U(n, X), E=1, 2, 5, 8 MeV; 239Pu(n, X), E=1, 2 MeV; measured σ(Eγ).
doi: 10.13182/NSE74-A23475
1973DR02 Nucl.Phys. A203, 257 (1973) D.M.Drake, S.L.Whetstone, I.Halpern The Radiative Capture of Fast Protons by Medium-Mass Nuclei NUCLEAR REACTIONS 56Fe, 59Co, 58,60,61Ni, 63Cu, 64Zn(p, γ), E=8-22 MeV; measured σ(E;Eγ). Enriched targets.
doi: 10.1016/0375-9474(73)90134-6
1972BE46 Nucl.Phys. A191, 641 (1972) I.Bergqvist, D.M.Drake, D.K.McDaniels Radiative Capture of Energetic Neutrons by 208Pb NUCLEAR REACTIONS 208Pb(n, γ), E=6.2-14.7 MeV; measured σ(E;Eγ); deduced total σ; tested semi-direct capture theory. 209Pb deduced giant resonance structure. Isotopic target.
doi: 10.1016/0375-9474(72)90637-9
1970BR43 Nucl.Phys. A156, 609 (1970) W.K.Brown, D.R.Dixon, D.M.Drake Fission Cross Sections of 237Np from Pommard NUCLEAR REACTIONS, Fission 237Np(n, F), E=0.032-2.2 keV, 0.1-2.8 MeV; measured σ(E). Pommard nuclear explosion experiment.
doi: 10.1016/0375-9474(70)90256-3
1970DR11 Nucl.Sci.Eng. 40, 294 (1970) D.M.Drake, J.C.Hopkins, C.S.Young Gamma-Ray-Production Cross Sections for Fast Neutron Interactions with Several Elements
doi: 10.13182/nse70-a19690
1969DR04 Nucl.Phys. A133, 108(1969) Inelastic Neutron Scattering and Gamma Production from Fast-Neutron Bombardment of 235U NUCLEAR REACTIONS 235U(n, Xγ), E = 4.0, 6.0, 7.5 MeV; measured σ(E;Eγ, θ); deduced σ(n, n').
doi: 10.1016/0375-9474(69)90453-9
1969DR08 Nucl.Phys. A128, 209 (1969) D.M.Drake, J.C.Hopkins, C.S.Young, H.Conde, A.Sattler Fast Neutron Elastic and Inelastic Scattering from Silicon NUCLEAR REACTIONS Si(n, n'), En=4.0 to 7.67 MeV; measured σ(En;En', θ), σ(En;Eγ, θ). Natural target.
doi: 10.1016/0375-9474(69)90986-5
1968HO03 Nucl.Phys. A107, 139 (1968) J.C.Hopkins, D.M.Drake, H.Conde Elastic and Inelastic Scattering of Fast Neutrons from 6Li and 7Li NUCLEAR REACTIONS 7Li(n, n'), 7Li(n, n), E = 3.35 MeV; 6,7Li(n, n), (n, n'), E = 4.83 MeV, 5.74 MeV, 7.5 MeV; measured σ(En', θ). Enriched targets.
doi: 10.1016/0375-9474(68)90731-8
1967KU08 Phys.Rev. 161, 1236 (1967) F.T.Kuchnir, P.Axel, L.Criegee, D.M.Drake, A.O.Hanson, D.C.Sutton Neutron Spectra from Monoenergetic Photons on Bismuth NUCLEAR STRUCTURE 208Bi; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.161.1236
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