NSR Query Results
Output year order : Descending NSR database version of April 24, 2024. Search: Author = D.K.McDaniels Found 71 matches. 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
1989HO11 Z.Phys. A333, 39 (1989) D.J.Horen, J.Lisantti, R.L.Auble, F.E.Bertrand, B.L.Burks, E.E.Gross, R.O.Sayer, D.K.McDaniels, K.W.Jones, J.B.McClelland, S.J.Seestrom-Morris, L.W.Swenson T = 1, Spin-Dipole Strength in 40Ca NUCLEAR REACTIONS 40Ca(p, p'), E=500 MeV; measured σ(θ), σ(Ep). 40Ca deduced T=1 spin-dipole transition strength distribution.
1989LI03 Phys.Rev. C39, 568 (1989) J.Lisantti, D.J.Horen, F.E.Bertrand, R.L.Auble, B.L.Burks, E.E.Gross, R.O.Sayer, D.K.McDaniels, K.W.Jones, J.B.McClelland, S.J.Seestrom-Morris, L.W.Swenson Collective Model Distored-Wave Born Approximation Analysis of 500-MeV Proton Scattering form 40Ca NUCLEAR REACTIONS 40Ca(polarized p, p'), E=500 MeV; analyzed σ(θ), analyzing power vs θ; deduced optical model parameters. 40Ca levels deduced deformation lengths, multipole matrix elements. Relativistic, non-relativistic DWBA analysis.
doi: 10.1103/PhysRevC.39.568
1989LI15 Phys.Rev. C40, 211 (1989) J.Lisantti, D.J.Horen, F.E.Bertrand, R.L.Auble, B.L.Burks, E.E.Gross, R.O.Sayer, D.K.McDaniels, K.W.Jones, J.B.McClelland, S.J.Seestrom-Morris, L.W.Swenson Giant Resonance Strength Distribution in 40Ca from Inelastic Scattering of 500 MeV Protons NUCLEAR REACTIONS 40Ca(polarized p, p'), E=500 MeV; measured σ(θp, Ep), σ(θ). 40Ca deduced giant resonance strength distribution.
doi: 10.1103/PhysRevC.40.211
1989SW01 Phys.Rev. C40, 246 (1989) L.W.Swenson, X.Y.Chen, J.Lisantti, D.K.McDaniels, I.Bergqvist, F.E.Bertrand, D.J.Horen, E.E.Gross, C.Glover, R.O.Sayer, B.L.Burks, O.Hausser, K.Hicks, M.J.Iqbal Different Continuum Approaches to Giant Resonances in 208Pb with 400-MeV Protons NUCLEAR REACTIONS 208Pb(p, p'), E=400 MeV; 208Pb(polarized p, p'), E=200 MeV; measured σ(θ). 208Pb deduced giant resonance L, Γ, EWSR. DWBA analysis, continuum models comparison.
doi: 10.1103/PhysRevC.40.246
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
1988HU10 Nucl.Phys. A483, 429 (1988) D.A.Hutcheon, W.C.Olsen, H.S.Sherif, R.Dymarz, J.M.Cameron, J.Johansson, P.Kitching, P.R.Liljestrand, W.J.McDonald, C.A.Miller, G.C.Neilson, D.M.Sheppard, D.K.McDaniels, J.R.Tinsley, P.Schwandt, L.W.Swenson, C.E.Stronach The Elastic Scattering of Intermediate Energy Protons from 40Ca and 208Pb NUCLEAR REACTIONS 40Ca, 208Pb(polarized p, p), E=200, 300, 400, 500 MeV; measured σ(E, θ), A(E, θ). Natural Ca, enriched 208Pb targets. Relativistic, non-relativistic phenomenological, microscopic model analysis.
doi: 10.1016/0375-9474(88)90078-4
1988LI18 Phys.Rev. C37, 2408 (1988) J.Lisantti, F.E.Bertrand, D.J.Horen, B.L.Burks, C.W.Glover, D.K.McDaniels, L.W.Swenson, X.Y.Chen, O.Hausser, K.Hicks Excitation of Giant Resonances in 28Si with 250 MeV Protons NUCLEAR REACTIONS 28Si(p, p), (p, p'), E=250 MeV; measured σ(θ). 28Si deduced level deformation lengths, giant resonance EWSR.
doi: 10.1103/PhysRevC.37.2408
1987HA11 Phys.Lett. 184B, 316 (1987) O.Hausser, K.Hicks, C.W.Glover, R.Abegg, A.Celler, C.Gunther, R.L.Helmer, R.Henderson, D.J.Horen, C.J.Horowitz, K.P.Jackson, J.Lisantti, D.K.McDaniels, C.A.Miller, R.Sawafta, L.W.Swenson Spin Observables for 208Pb(p(pol), p(pol)) Elastic Scattering at 290 MeV NUCLEAR REACTIONS 208Pb(polarized p, p), E=290 MeV; measured polarizations, transfer coefficients vs momentum transfer; deduced elastic scattering amplitudes, spin rotation parameters. Focal-plane polarimeter. Dirac calculations.
doi: 10.1016/0370-2693(87)90172-9
1987MC03 Nucl.Phys. A467, 557 (1987) D.K.McDaniels, J.Lisantti, I.Bergqvist, L.W.Sewnson, X.Y.Chen, D.J.Horen, F.E.Bertrand, E.E.Gross, C.Glover, R.Sayer, B.L.Burks, O.Hausser, K.Hicks Validity of Collective Model DWBA Analysis for Intermediate Energy Proton Scattering to Low-Lying States of 208Pb NUCLEAR REACTIONS 208Pb(p, p'), E=200, 400 MeV; measured σ(θ). 208Pb levels deduced deformation lengths, multipole moments, neutron, proton matrix element ratio. DWBA analysis.
doi: 10.1016/0375-9474(87)90386-1
1986BE14 Phys.Rev. C34, 45 (1986) F.E.Bertrand, E.E.Gross, D.J.Horen, R.O.Sayer, T.P.Sjoreen, D.K.McDaniels, J.Lisantti, J.R.Tinsley, L.W.Swenson, J.B.McClelland, T.A.Carey, K.Jones, S.J.Seestrom-Morris Giant Resonance Structure in 208Pb Measured using the (p, p') Reaction at 334 MeV NUCLEAR REACTIONS 208Pb(polarized p, p'), E=334 MeV; measured σ(Ep), σ(θ); deduced model parameters. 208Pb deduced giant resonances, Γ, L, EWSR, B(λ). DWBA analysis.
doi: 10.1103/PhysRevC.34.45
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
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
1985HO14 Phys.Rev. C31, 2049 (1985) D.J.Horen, F.E.Bertrand, E.E.Gross, T.P.Sjoreen, D.K.McDaniels, J.R.Tinsley, J.Lisantti, L.W.Swenson, J.B.McClelland, T.A.Carey, S.J.Seestrom-Morris, K.Jones Cross Sections and Analyzing Powers for Quenched Spin Excitations in 40,48Ca at E(p) = 334 MeV NUCLEAR REACTIONS 40,48Ca(polarized p, p'), E=334 MeV; measured σ(Ep'), σ(θ), analyzing power vs θ. 40Ca level deduced B(M2). Microscopic DWIA.
doi: 10.1103/PhysRevC.31.2049
1985MC06 Phys.Lett. 162B, 277 (1985) D.K.McDaniels, J.Lisantti, J.Tinsley, I.Bergqvist, L.W.Swenson, F.E.Bertrand, E.E.Gross, D.J.Horen On the Validity of Microscopic Calculations for Inelastic Proton Scattering NUCLEAR REACTIONS 208Pb(polarized p, p'), E=200, 334 MeV; analyzed σ(θ). 208Pb level deduced B(E2).
doi: 10.1016/0370-2693(85)90922-0
1984FA11 Phys.Rev. C30, 1622 (1984) J.A.Faucett, B.E.Wood, D.K.McDaniels, P.A.M.Gram, M.E.Hamm, M.A.Oothoudt, C.A.Goulding, L.W.Swenson, K.S.Krane, A.W.Stetz, H.S.Plendl, J.Norton, H.Funsten, D.Joyce Kinematically Complete Measurement of the (π±, π±p) Reaction on 12C at 220 MeV NUCLEAR REACTIONS 12C(π+, π+p), (π-, π-p), (π-, π-'), (π+, π+'), E=220 MeV; measured σ(θ(π), E(π)), σ(θ(π), θ(p), E(p)), σ(θ(π), θ(p), E(π)), σ(θ(π), θ(p)), σ(θ(π), θ(p)) vs missing mass; deduced reaction mechanism. Kinematically complete experiment.
doi: 10.1103/PhysRevC.30.1622
1984HO16 Phys.Rev. C30, 709 (1984) D.J.Horen, F.E.Bertrand, E.E.Gross, T.P.Sjoreen, D.K.McDaniels, J.R.Tinsley, J.Lisantti, L.W.Swenson, J.B.McClelland, T.A.Carey, S.J.Seestrom-Morris, K.Jones Excitation of E2 Transitions in 40Ca by 334-MeV Protons NUCLEAR REACTIONS 40Ca(polarized p, p'), E=334 MeV; measured σ(θ), analyzing power vs θ; deduced optical model parameters. 40Ca deduced levels, J, π, L admixture, deformation lengths, B(E2). Macroscopic DWBA analysis.
doi: 10.1103/PhysRevC.30.709
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
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
1982AR01 Phys.Rev. C25, 936 (1982) L.G.Arnold, B.C.Clark, E.D.Cooper, H.S.Sherif, D.A.Hutcheon, P.Kitching, J.M.Cameron, R.P.Liljestrand, R.N.MacDonald, W.J.McDonald, C.A.Miller, G.C.Neilson, W.C.Olsen, D.M.Sheppard, G.M.Stinson, D.K.McDaniels, J.R.Tinsley, R.L.Mercer, L.W.Swenson, P.Schwandt, C.E.Stronach Energy Dependence of the p - 40Ca Optical Potential: A Dirac equation perspective NUCLEAR REACTIONS 40Ca(polarized p, p), E=26-1040 MeV; analyzed data; deduced optical potential energy dependence. Dirac equation.
doi: 10.1103/PhysRevC.25.936
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
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
1981BE33 Phys.Lett. 103B, 326 (1981) F.E.Bertrand, E.E.Gross, D.J.Horen, J.R.Wu, J.Tinsley, D.K.McDaniels, L.W.Swenson, R.Liljestrand Excitation of Giant Resonance Modes in 90Zr and 120Sn by 200 MeV Protons NUCLEAR REACTIONS 90Zr, 120Sn(p, p'), E=200 MeV; measured σ(Ep, θ). 90Zr deduced M1 transition strength. 90Zr, 120Sn deduced GDR, isoscalar GQR, giant octupole resonance, hexadecapole strength upper limit. Broad-range magnetic spectrograph.
doi: 10.1016/0370-2693(81)90235-5
1981HU04 Phys.Rev.Lett. 47, 315 (1981) D.A.Hutcheon, J.M.Cameron, R.P.Liljestrand, P.Kitching, C.A.Miller, W.J.McDonald, D.M.Sheppard, W.C.Olsen, G.C.Neilson, H.S.Sherif, D.K.McDaniels, J.R.Tinsley, L.W.Swenson, P.Schwandt, C.E.Stronach, L.Ray Elastic Scattering of 400-MeV Protons by 208Pb NUCLEAR REACTIONS 208Pb(polarized p, p), E=400 MeV; measured σ(θ), A(θ). Second-order Kerman-McManus-Thaler optical model analysis.
doi: 10.1103/PhysRevLett.47.315
1980KY01 Phys.Lett. 91B, 353 (1980) G.S.Kyle, N.M.Hintz, M.S.Oothoudt, M.Kaletka, P.M.Lang, H.Nann, K.K.Seth, D.K.McDaniels, P.M.Varghese, T.Kozlowski, D.G.Madland, C.L.Morris, J.C.Pratt, J.E.Spencer, N.Tanaka, H.A.Thiessen, G.S.Blanpied, G.W.Hoffmann, R.P.Liljestrand, J.C.Fong, G.Igo, R.J.Ridge, C.A.Whitten, Jr. Elastic and Inelastic Scattering of 800 MeV Protons by 58Ni NUCLEAR REACTIONS 58Ni(p, p), (p, p'), E=800 MeV; measured σ(θ). 58Ni levels deduced deformation lengths. DWBA analysis.
doi: 10.1016/0370-2693(80)90994-6
1980SH02 Nucl.Phys. A333, 461 (1980) T.C.Sharma, L.W.Swenson, K.S.Krane, P.Varghese, D.K.McDaniels, H.A.Thiessen, N.Tanaka, R.R.Silbar, M.Greenfield, C.F.Moore Proton Yields from Quasielastic Pion Scattering on 27Al and 208Pb NUCLEAR REACTIONS 27Al, 208Pb(π+, π+p), (π-, π-p), E=255 MeV; measured σ(Ep, θp); deduced σ ratio. Semi-classical nucleon charge exchange model.
doi: 10.1016/0375-9474(80)90110-4
1979IG01 Phys.Lett. 81B, 151 (1979) G.Igo, G.S.Adams, T.S.Bauer, G.Pauletta, C.A.Whitten, Jr., A.Wriekat, G.W.Hoffmann, G.S.Blanpied, W.R.Coker, C.Harvey, R.P.Liljestrand, L.Ray, J.E.Spencer, H.A.Thiessen, C.Glashausser, N.M.Hintz, M.A.Oothoudt, H.Nann, K.K.Seth, B.E.Wood, D.K.McDaniels, M.Gazzaly Elastic Differential Cross Sections and Analyzing Powers for Polarized p + 40,42,44,48Ca at 0.8 GeV NUCLEAR REACTIONS 40,42,44,48Ca(polarized p, p), E=0.8 GeV; measured σ(θ), A(θ); deduced rms radii of neutrons. Kerman-McManus-Thaler optical potential analysis.
doi: 10.1016/0370-2693(79)90510-0
1979KR14 Phys.Rev. C20, 1873 (1979) K.S.Krane, T.C.Sharma, L.W.Swenson, D.K.McDaniels, P.Varghese, B.E.Wood, R.R.Silbar, H.D.Wohlfahrt, C.A.Goulding Energetic Charged-Particle Spectrum Following μ- Capture by Nuclei NUCLEAR REACTIONS Al, Cu, Pb(μ-, X), E=0; measured charged-particle spectrum, σ(E).
doi: 10.1103/PhysRevC.20.1873
1979RA15 Phys.Lett. 83B, 275 (1979) L.Ray, T.Kozlowski, D.G.Madland, C.L.Morris, J.C.Pratt, J.E.Spencer, N.Tanaka, H.A.Thiessen, G.S.Kyle, N.M.Hintz, M.A.Oothoudt, P.M.Lang, H.Nann, K.K.Seth, D.K.McDaniels, P.M.Varghese, G.S.Blanpied, G.W.Hoffmann, R.P.Liljestrand, J.C.Fong, G.Igo, R.J.Ridge, R.M.Rolfe, C.A.Whitten, Jr. Coupled-Channels Effects in 0.8 GeV Proton Inelastic Scattering from 58Ni NUCLEAR REACTIONS 58Ni(p, p'), E=0.8 GeV; calculated σ(θ). Coupled channel, DWBA calculations with multistep, multiphonon mixing.
doi: 10.1016/0370-2693(79)91106-7
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
1978HO05 Phys.Rev.Lett. 40, 1256 (1978) G.W.Hoffman, G.S.Blanpied, W.R.Coker, R.P.Liljestrand, N.M.Hintz, M.A.Oothoudt, T.S.Bauer, G.Igo, G.Pauletta, J.Soukup, C.A.Whitten, Jr., D.Madland, J.C.Pratt, L.Ray, J.E.Spencer, H.A.Thiessen, H.Nann, K.K.Seth, C.Glashausser, D.K.McDaniels, J.Tinsley, P.Varghese Analyzing Power in Proton-Nucleus Elastic Scattering at 0.8 GeV NUCLEAR REACTIONS 12C, 58Ni, 90Zr, 208Pb(polarized p, p), E=0.8 GeV; measured A(θ), σ(θ).
doi: 10.1103/PhysRevLett.40.1256
1978HO12 Phys.Lett. 76B, 383 (1978) G.W.Hoffmann, G.S.Blanpied, W.R.Coker, R.P.Liljestrand, L.Ray, J.E.Spencer, H.A.Thiessen, N.M.Hintz, M.A.Oothoudt, T.S.Bauer, G.Igo, G.Pauletta, J.Soukup, C.A.Whitten, Jr., H.Nann, K.K.Seth, C.Glashausser, D.K.McDaniels, J.Tinsley, P.Varghese Analysis of Elastic Scattering of 0.8 GeV Polarized Protons from 116Sn and 124Sn NUCLEAR REACTIONS 116,124Sn(polarized p, p), E=800 MeV; analyzed A(θ), σ(θ). Spin-dependent Kerman-McManus-Thaler formalism.
doi: 10.1016/0370-2693(78)90888-2
1978HO18 Phys.Lett. 79B, 376 (1978) G.W.Hoffmann, G.S.Blanpied, W.R.Coker, C.Harvey, R.P.Liljestrand, G.S.Adams, T.S.Bauer, G.Igo, G.Pauletta, C.A.Whitten, Jr., A.Wriekat, L.Ray, J.E.Spencer, H.A.Thiessen, H.Nann, K.K.Seth, N.M.Hintz, G.Kyle, M.A.Oothoudt, B.E.Wood, D.K.McDaniels, C.Glashausser, M.Gazzaly Elastic Differential Cross Sections and Analyzing Powers for p + 54Fe, 58,64Ni at 800 MeV NUCLEAR REACTIONS 54Fe, 58,64Ni(polarized p, p), E=800 MeV; measured σ(θ); deduced neutron density distribution. Approximately model-independent analysis.
doi: 10.1016/0370-2693(78)90386-6
1978SW01 Phys.Rev.Lett. 40, 10 (1978) L.W.Swenson, T.Sharma, K.Krane, P.Varghese, D.K.McDaniels, H.A.Thiessen, N.Tanaka, M.Greenfield, C.F.Moore Coincidence Measurements of Quasielastic Pion Scattering by 27Al and 208Pb NUCLEAR REACTIONS 27Al, 208Pb(π+, π+p), (π-, π-p), E=255 MeV; measured σ, ratios.
doi: 10.1103/PhysRevLett.40.10
1977BL09 Phys.Rev.Lett. 39, 1447 (1977); Erratum Phys.Rev.Lett. 40, 420 (1978) G.S.Blanpied, W.R.Coker, R.P.Liljestrand, L.Ray, G.W.Hoffman, D.Madland, C.L.Morris, J.C.Pratt, J.E.Spencer, H.A.Thiessen, N.M.Hintz, G.S.Kyle, M.A.Oothoudt, T.S.Bauer, J.C.Fong, G.Igo, R.J.Ridge, C.A.Whitten, Jr., Y.Kozlowski, D.K.McDaniels, P.Varghese, P.M.Lang, H.Nann, K.K.Seth, C.Glashausser Elastic Scattering of 0.8-GeV Protons from 12C, 58Ni, and 208Pb NUCLEAR REACTIONS 12C, 58Ni, 208Pb(p, p), E=0.8 GeV; measured σ(θ).
doi: 10.1103/PhysRevLett.39.1447
1977TH05 Nucl.Phys. A283, 475 (1977) M.J.Throop, Y.T.Cheng, A.Goswami, O.Nalcioglu, D.K.McDaniels, L.W.Swenson, N.Jarmie, J.H.Jett, P.A.Lovoi, D.Stupin, G.G.Ohlsen, G.C.Salzman A Surface-Delta Description of Analyzing Power Measurements for Collective States of Ni and Zn Isotopes NUCLEAR REACTIONS 58,60Ni, 64Zn(polarized p, p'), E=15 MeV; measured σ(θ), A(θ). Enriched target, 98.0%.
doi: 10.1016/0375-9474(77)90553-X
1975TH01 Nucl.Phys. A239, 333 (1975) M.J.Throop, Y.T.Cheng, D.K.McDaniels Coulomb Excitation of 67Zn and Core-Quasiparticle Coupling in f5/2 Nuclei NUCLEAR REACTIONS 67Zn(α, α'γ), E=3.2-4.86 MeV; measured σ(E, Eγ, θ). 64,66Zn(α, α'γ), 14N(α, pγ); measured σ(Eγ). 73Ge(α, α'γ); analyzed previous data. 67Zn levels deduced B(E2), J, π, γ-mixing. 73Ge deduced transition. 64,66Zn level deduced B(E2).
doi: 10.1016/0375-9474(75)90455-8
1975TH05 Phys.Rev.Lett. 35, 16 (1975) M.J.Throop, Y.T.Cheng, D.K.McDaniels, D.M.Stupin, L.W.Swenson, N.Jarmie, J.H.Jett, P.A.Lovoi, G.G.Ohlsen, G.C.Salzman Inelastic Proton Scattering as a Test of Surface-Delta Wave Functions NUCLEAR REACTIONS 58,60Ni, 64Zn(polarized p, p'), E=15 MeV; measured σ(Ep', θ), A(θ).
doi: 10.1103/PhysRevLett.35.16
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
1974CH09 Phys.Rev. C9, 1192 (1974) Y.T.Cheng, A.Goswami, M.J.Throop, D.K.McDaniels Status of Nuclear Coexistence for 32S NUCLEAR REACTIONS 31P(p, γ), E=0.811, 1.117, 1.583 MeV; measured DSAM. 32S level deduced T1/2.
doi: 10.1103/PhysRevC.9.1192
1974DR01 Phys.Rev. C9, 179 (1974) M.Drosg, D.K.McDaniels, J.C.Hopkins, J.D.Seagrave, R.H.Sherman, E.C.Kerr Elastic Scattering of Neutrons from 3He between 7.9 and 23.7 MeV NUCLEAR REACTIONS 3He(n, n), E=7.9-23.7 MeV; measured σ(E;θ).
doi: 10.1103/PhysRevC.9.179
1973GO12 Phys.Rev. C7, 1263 (1973) A.Goswami, D.K.McDaniels, O.Nalcioglu Anomalous Parity States in g9/2-Shell Nuclei and the Thankappan-True Core-Coupling Hamiltonian NUCLEAR STRUCTURE 73Ge, 99Tc, 111Ag calculated levels.
doi: 10.1103/PhysRevC.7.1263
1973MC05 Phys.Rev. C7, 882 (1973) D.K.McDaniels, M.Drosg, J.C.Hopkins, J.D.Seagrave Angular Distributions and Absolute Cross Sections for the T(d, n)4He Neutron-Source Reaction NUCLEAR REACTIONS 3H(d, n), E=5.0-15.7 MeV; measured σ(En, θ); deduced absolute σ(0°).
doi: 10.1103/PhysRevC.7.882
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
1972MC23 Phys.Rev. C6, 1593 (1972) D.K.McDaniels, M.Drosg, J.C.Hopkins, J.D.Seagrave Angular Distributions and Absolute Cross Sections for the T(p, n)3He Neutron Source Reaction NUCLEAR REACTIONS 3H(p, n), E=6, 7, 10, 11, 12, 13, 14, 15, 16 MeV; measured σ(E;θ).
doi: 10.1103/PhysRevC.6.1593
1972SA27 Nucl.Phys. A192, 312 (1972) G.C.Salzman, A.Goswami, D.K.McDaniels Coulomb Excitation of 73Ge and Quasiparticle-Phonon Coupling Theories NUCLEAR REACTIONS 72,73,74,76Ge(α, α'γ), Eα=4.0, 3.8, 3.6, 3.4, 3.0, 2.6 MeV; measured Iγ; Eα=3.9 MeV; measured σ(θ(γ)). 72,73,74,76Ge deduced B(E2), J, π, γ-mixing. Enriched target.
doi: 10.1016/0375-9474(72)90262-X
1971BA72 Phys.Rev. C4, 1601 (1971) Resonance Structure in Reaction 9Be(d, γ)11B NUCLEAR REACTIONS 9Be(d, γ), E=0.56-3.56 MeV; measured σ(E;θ). 11B deduced levels, resonances, level-width.
doi: 10.1103/PhysRevC.4.1601
1971BE38 Phys.Rev.Lett. 27, 269 (1971) I.Bergqvist, D.Drake, D.K.McDaniels Spectrum of the Reaction 208Pb(n, γ)209Pb and Semidirect Capture Theory NUCLEAR REACTIONS 208Pb(n, γ), E=9.2, 11.2, 13.2 MeV; measured σ(Eγ); deduced agreement with semidirect capture theory.
doi: 10.1103/PhysRevLett.27.629
1971DR07 Phys.Lett. 36B, 557 (1971) D.Drake, I.Bergqvist, D.K.McDaniels Dependence of 14 MeV Radiative Neutron Capture on Mass Number NUCLEAR REACTIONS 165Ho, 208Pb, 238U, Gd, Ta, Au(n, γ), E=14 MeV; measured σ.
doi: 10.1016/0370-2693(71)90088-8
1971HU04 Phys.Rev. C3, 1222 (1971) F.C.P.Huang, E.F.Gibson, D.K.McDaniels Search for an Excited Prolate Rotational Band in 28Si NUCLEAR REACTIONS 27Al(p, γ), E=655, 679, 774, 1262, 2203 keV; measured Eγ, Iγ, σ(E;Eγ), Doppler shift attenuation. 28Si deduced levels, J, π, T1/2, γ-branching.
doi: 10.1103/PhysRevC.3.1222
1970HU14 Phys.Rev. C2, 1342 (1970) 8543-keV 6+ State in 28Si and the Ground-State Rotational Band NUCLEAR REACTIONS 27Al(p, γ), E=1.317, 2.203 MeV; measured σ(Eγ), Doppler shift attenuation. 28Si resonances deduced γ-branching. 28Si levels deduced T1/2.
doi: 10.1103/PhysRevC.2.1342
1969GI05 Phys.Rev. 188, 1965 (1969) E.F.Gibson, A.Goswami, F.Huang, D.K.McDaniels 7416-keV 2+ Level in 28Si and an Excited Prolate Rotational Band NUCLEAR REACTIONS 27Al(p, γ), E=679, 1262 keV; measured γγ-coin, Doppler shift attenuation. 28Si levels deduced T1/2, branching ratios, E2 transition strengths.
doi: 10.1103/PhysRev.188.1965
1969KU15 Nucl.Instr.Methods 69, 56 (1969) E.Kurtz, K.Battleson, D.K.McDaniels, D.J.Horen Resonance Energy and Yield Measurements with a Ge(Li) Detector NUCLEAR REACTIONS 27Al(p, γ), E=1-4 MeV; measured σ(E;Eγ); deduced resonance energies.
doi: 10.1016/0029-554X(69)90572-2
1969PI10 Phys.Rev. 181, 1555 (1969) C.J.Piluso, G.C.Salzman, D.K.McDaniels Lifetime and Angular Distribution Measurements from the 31P(p, γ)32S Reaction NUCLEAR REACTIONS 31P(p, γ), E = 1.248-1.583 MeV; measured σ(E;Eγ, θ), Doppler shift attenuation. 32S deduced levels, J, T1/2, γ-branching, γ-mixing. Ge(Li) detector.
doi: 10.1103/PhysRev.181.1555
1968DO12 Phys.Rev. 175, 1446 (1968) Lifetime Measurements from the K39(p, γ)Ca40 Reaction NUCLEAR STRUCTURE 40Ca; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.175.1446
1968GI05 Phys.Rev. 172, 1004 (1968) E.F.Gibson, K.Battleson, D.K.McDaniels Lifetimes, Energies, and Branching Ratios of 28Si Excited States NUCLEAR REACTIONS 27Al(p, γ), E=1.2-2.4 MeV; measured Eγ, Iγ, Doppler shift attenuation. 28Si deduced resonances, levels, J, π, T1/2.
doi: 10.1103/PhysRev.172.1004
1967MC19 Nucl.Instr.Methods 54, 317 (1967) D.K.McDaniels, K.W.Dolan, C.J.Piluso High Energy Gamma Ray Energy Measurements NUCLEAR REACTIONS 27Al(p, γ), E=0.9-5.5 MeV; measured σ(E;Eγ). 19F(p, αγ), E=0.936 MeV; measured Eγ. 16O deduced transition. 28Si deduced resonances, levels.
doi: 10.1016/0029-554X(67)90642-8
1967MO20 Phys.Rev. 162, 1087 (1967) Gamma-Ray Spectrum of Ruthenium-99 NUCLEAR STRUCTURE 99Rh; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.162.1087
1966DO07 Phys.Rev. 148, 1151 (1966) K.W.Dolan, D.K.McDaniels, D.O.Wells Energy Levels of 56Fe NUCLEAR STRUCTURE 58Co, 56Co; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.148.1151
1966MO10 Nucl.Phys. 82, 289(1966) G.A.Moss, D.O.Wells, D.K.McDaniels An Investigation of the Levels of 131Xe RADIOACTIVITY 131I [from fission]; measured Eγ, Iγ, γγ(θ). 131Xe deduced levels, J, π.
doi: 10.1016/0029-5582(66)90003-4
1966MO16 Nucl.Phys. 85, 513 (1966) The Decay of 140Ba RADIOACTIVITY 140Ba [from fission]; measured Eγ, Iγ. 140La deduced levels.
doi: 10.1016/0029-5582(66)90318-X
1966PI01 Nucl.Phys. 77, 193(1966) C.J.Piluso, D.O.Wells, D.K.McDaniels The Decay of 56Ni and 57Ni RADIOACTIVITY 56,57Ni[from 54Fe(α, 2n), 54Fe(α, n)]; measured Eγ, Iγ. 56,57Co deduced levels, J, π. Natural target.
doi: 10.1016/0029-5582(66)90686-9
1966RA09 Nucl.Phys. 81, 296 (1966); Erratum Nucl.Phys. A95, 705 (1967) P.V.Rao, D.K.McDaniels, B.Crasemann Decay of 75Se RADIOACTIVITY 75Se[from 74Se(n, γ)]; measured Eγ, Iγ, I(X-ray), γX-coin; deduced K-capture probability P(K), capture branching. Enriched target.
1965TE02 Phys.Rev. 139, B1125 (1965) J.K.Temperley, D.K.McDaniels, D.O.Wells Level Scheme of Ga69 NUCLEAR STRUCTURE 69Ge; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.139.B1125
1964TE03 Bull.Am.Phys.Soc. 9, No.7, 718, K5 (1964) J.K.Temperley, D.K.McDaniels, D.O.Wells Decay of Ge69 NUCLEAR STRUCTURE 69Ge; measured not abstracted; deduced nuclear properties.
1962HE05 Bull.Am.Phys.Soc. 7, No.4, 270, CB13 (1962) Symmetry-Axis Behavior of α-γ Correlations in C12(α, α'γ) Reactions NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
1962MC11 Phys.Letters 1, 295 (1962) D.K.McDaniels, D.L.Hendrie, R.H.Bassel, G.R.Satchler Alpha-Gamma Angular Correlations and the Distorted - Waves Theory NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(62)91391-4
1960BL07 Nuclear Phys. 17, 641 (1960) J.S.Blair, G.W.Farwell, D.K.McDaniels Diffraction Analysis of Elastic and Inelastic Scattering by Magnesium NUCLEAR STRUCTURE 24Mg; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(60)90150-4
1960MC14 Nucl.Phys. 17, 614 (1960) D.K.McDaniels, J.S.Blair, S.W.Chen, G.W.Farwell Alpha-Particle Excitation of Quadrupole and Octupole Surface Modes in Ti, Fe, Ni, Zn, and Sr NUCLEAR STRUCTURE 48Ti, 66Zn, 64Zn, 60Ni, 58Ni, 56Fe, 88Sr, 68Zn; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(60)90149-8
1959MC67 Bull.Am.Phys.Soc. 4, No.8, 445, C12 (1959) D.K.McDaniels, G.W.Farwell, J.S.Blair Elastic and Inelastic Scattering from Mg
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