NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = F.D.McDaniel Found 38 matches. 1997AZ03 J.Phys.(London) B30, 353 (1997) A.R.Azordegan, H.L.Sun, Y.C.Yu, J.L.Duggan, F.D.McDaniel, E.K.Lin, C.W.Wang, G.Lapicki Charge State Dependence of Copper L-Shell X-Ray Production by 4-14 MeV Oxygen Ions ATOMIC PHYSICS Cu(16O, X), E=4-14 MeV; measured L-shell X-ray production σ; deduced projectile charge state dependence, electron capture contribution.
doi: 10.1088/0953-4075/30/2/026
1996SU16 Phys.Rev. A53, 4190 (1996) H.L.Sun, Y.C.Yu, E.K.Lin, C.W.Wang, J.L.Duggan, A.R.Azordegan, F.D.McDaniel, G.Lapicki Charge-State Dependence of K-Shell X-Ray Production in Aluminum by 2-12 MeV Carbon Ions NUCLEAR REACTIONS 27Al(C, X), E=2-12 MeV; measured K-shell X-ray production σ; deduced charge state dependence. ECPSSR theory. ATOMIC PHYSICS 27Al(C, X), E=2-12 MeV; measured K-shell X-ray production σ; deduced charge state dependence. ECPSSR theory.
doi: 10.1103/PhysRevA.53.4190
1995ME21 J.Phys.(London) B28, 1187 (1995) R.Mehta, H.L.Sun, D.K.Marble, J.L.Duggan, F.D.McDaniel, G.Lapicki L-Shell X-Ray Production by 2-12 MeV Carbon Ions in Fifteen Selected Elements from Copper to Lead NUCLEAR REACTIONS Cu, Ga, Ge, Br, 89Y, Mo, Ag, Sn, La, Nd, Gd, Ho, Yb, 197Au, Pb(C, X), E=2-12 MeV; measured L-shell X-ray production σ. Model comparison. ATOMIC PHYSICS Cu, Ga, Ge, Br, Y, Mo, Ag, Sn, La, Nd, Gd, Ho, Yb, 197Au, Pb(C, X), E=2-12 MeV; measured L-shell X-ray production σ. Model comparison.
doi: 10.1088/0953-4075/28/7/013
1995SU33 Nucl.Instrum.Methods Phys.Res. B99, 192 (1995) H.L.Sun, J.L.Duggan, F.D.McDaniel, G.Lapicki An Overview of Projectile-Charge-State Dependence of K-, L-, and M-Shell Ionization in Thin Solid Targets for a Variety of Incident Heavy Ions from 0.1 to 5.7 MeV/u NUCLEAR REACTIONS Ho, 45Sc, Ti, Cu, Ge(28Si, X), E=1.86 MeV/nucleon; Ho(12C, X), E=2-12 MeV; Nd, Gd, Ho, Yb, 197Au, Pb(12C, X), E=25 MeV; Nd, Gd, Ho, Yb, 197Au, Pb(16O, X), E=32 MeV; Nd, Ho, 197Au(28Si, X), E=1.8 MeV/nucleon; Nd, Ho, 197Au(19F, X), E=1.86 MeV/nucleon; 27Al(12C, X), E=2-8 MeV; compiled, reviewed K-, L-, M-shell X-ray production σ data, analyses, charge state dependence related features. Thin solid targets. ATOMIC PHYSICS Ho, 45Sc, Ti, Cu, Ge(28Si, X), E=1.86 MeV/nucleon; Ho(12C, X), E=2-12 MeV; Nd, Gd, Ho, Yb, 197Au, Pb(12C, X), E=25 MeV; Nd, Gd, Ho, Yb, 197Au, Pb(16O, X), E=32 MeV; Nd, Ho, 197Au(28Si, X), E=1.8 MeV/nucleon; Nd, Ho, 197Au(19F, X), E=1.86 MeV/nucleon; 27Al(12C, X), E=2-8 MeV; compiled, reviewed K-, L-, M-shell X-ray production σ data, analyses, charge state dependence related features. Thin solid targets.
doi: 10.1016/0168-583X(95)00208-1
1995YU11 Phys.Rev. A52, 3836 (1995) Y.C.Yu, H.L.Sun, J.L.Duggan, F.D.McDaniel, J.Y.Yin, G.Lapicki Charge-State Dependence of M-Shell X-Ray Production in 67Ho by 2-12-MeV Carbon Ions NUCLEAR REACTIONS Ho(12C, X), E=2-12 MeV; measured X-ray production σ; deduced charge state dependence. ATOMIC PHYSICS Ho(12C, X), E=2-12 MeV; measured X-ray production σ; deduced charge state dependence.
doi: 10.1103/PhysRevA.52.3836
1994MC10 J.Phys.(London) B27, 5295 (1994) M.R.McNeir, Y.C.Yu, D.L.Weathers, D.K.Marble, Z.Zhao, J.L.Duggan, F.D.McDaniel, G.Lapicki L-Shell X-Ray Production Cross Sections in 26Fe, 28Ni, 29Cu, 30Zn, 31Ga and 32Ge by 0.5 to 8.0 MeV He Ions NUCLEAR REACTIONS Fe, Ni, Cu, Zn, Ga, Ge(α, X), E=0.5-8 MeV; measured L X-ray production σ. Windowless Si(Li) detector. Model comparison. ATOMIC PHYSICS Fe, Ni, Cu, Zn, Ga, Ge(α, X), E=0.5-8 MeV; measured L X-ray production σ. Windowless Si(Li) detector. Model comparison.
doi: 10.1088/0953-4075/27/21/020
1993ME16 Nucl.Instrum.Methods Phys.Res. B79, 175 (1993) R.Mehta, J.L.Duggan, F.D.McDaniel, M.R.McNeir, Y.C.Yu, D.K.Marble, G.Lapicki L-Shell X-Ray Production Cross Sections for 29Cu, 31Ga, 32Ge, 35Br, 39Y, 60Nd, 64Gd, 67Ho, 70Yb, 79Au, and 82Pb for 2-25 MeV Carbon Ions NUCLEAR REACTIONS Cu, Ga, Ge, Br, 89Y, Nd, Gd, 165Ho, Yb, 197Au, Pb(C, X), E=2-25 MeV; measured L X-ray production σ; deduced Si(Li) detector efficiency. Multiple normalization techniques. ATOMIC PHYSICS Cu, Ga, Ge, Br, 89Y, Nd, Gd, 165Ho, Yb, 197Au, Pb(C, X), E=2-25 MeV; measured L X-ray production σ; deduced Si(Li) detector efficiency. Multiple normalization techniques.
doi: 10.1016/0168-583X(93)95318-Y
1993SU29 Nucl.Instrum.Methods Phys.Res. B79, 186 (1993) H.L.Sun, J.F.Kirchhoff, A.R.Azordegan, J.L.Duggan, F.D.McDaniel, R.M.Wheeler, R.P.Chaturvedi, G.Lapicki M-Shell X-Ray Production Cross Sections of Rare-Earth Elements by 4He2+ Impact in the Energy Range 0.7-7.0 MeV NUCLEAR REACTIONS 139La, Nd, Sm, Eu, Gd, Dy, 165Ho, Er, Yb, Lu, Hf(α, X), E=0.7-7 MeV; measured M-shell X-ray production σ; deduced detector efficiency. Windowless Si(Li) detector. ATOMIC PHYSICS 139La, Nd, Sm, Eu, Gd, Dy, 165Ho, Er, Yb, Lu, Hf(α, X), E=0.7-7 MeV; measured M-shell X-ray production σ; deduced detector efficiency. Windowless Si(Li) detector.
doi: 10.1016/0168-583X(93)95321-U
1991MA66 Nucl.Instrum.Methods Phys.Res. B56/57, 33 (1991) D.K.Marble, F.D.McDaniel, M.R.McNeir, Y.C.Yu, Z.Y.Zhao, D.K.Wilson, D.L.Weathers, J.L.Duggan, R.M.Wheeler, R.P.Chaturvedi, G.Lapicki, V.Zoran Direct Ionization in K-Shell X-Ray Production in Fluorine by Highly-Charged Lithium, Boron, and Oxygen Ions NUCLEAR REACTIONS 19F(7Li, X), E=1.5-4 MeV; 19F(10B, X), E=2-10 MeV; 19F(16O, X), E=3-12 MeV; measured K-shell X-ray production σ(E). Solid YF3 target. Model comparison. ATOMIC PHYSICS 19F(7Li, X), E=1.5-4 MeV; 19F(10B, X), E=2-10 MeV; 19F(16O, X), E=3-12 MeV; measured K-shell X-ray production σ(E). Solid YF3 target. Model comparison.
doi: 10.1016/0168-583X(91)95964-F
1991MC02 Nucl.Instrum.Methods Phys.Res. B54, 531 (1991) F.D.McDaniel, D.K.Marble, J.L.Duggan, M.R.McNeir, Y.C.Yu, Z.Y.Zhao, D.L.Weathers, P.S.Elliott, R.M.Wheeler, R.P.Chaturvedi, G.Lapicki X-Ray Production in Fluorine by Highly Charged Boron, Carbon, and Oxygen Ions NUCLEAR REACTIONS 19F(B, X), (C, X), E=10 MeV; 19F(O, X), E=8, 10, 12 MeV; measured K X-ray production σ; deduced direct ionization, electron capture contributions. ATOMIC PHYSICS 19F(B, X), (C, X), E=10 MeV; 19F(O, X), E=8, 10, 12 MeV; measured K X-ray production σ; deduced direct ionization, electron capture contributions.
doi: 10.1016/0168-583X(91)95433-E
1991MC09 Phys.Rev. A44, 4372 (1991) M.R.McNeir, Y.C.Yu, D.L.Weathers, J.L.Duggan, F.D.McDaniel, G.Lapicki L-Shell X-Ray Production Cross Sections in 26Fe, 28Ni, 29Cu, 30Zn, 31Ga, and 32Ge by 0.5- to 5.0-MeV Protons NUCLEAR REACTIONS Fe, Ni, Cu, Zn, Ga, Ge(p, X), E=0.5-5 MeV; measured L-shell X-ray production σ. Model comparison. ATOMIC PHYSICS Fe, Ni, Cu, Zn, Ga, Ge(p, X), E=0.5-5 MeV; measured L-shell X-ray production σ. Model comparison.
doi: 10.1103/PhysRevA.44.4372
1991MC11 Nucl.Instrum.Methods Phys.Res. B56/57, 26 (1991) M.R.McNeir, Y.C.Yu, D.L.Weathers, D.K.Marble, J.L.Duggan, F.D.McDaniel, G.Lapicki L-Shell X-Ray Production Cross Sections in 20Ca, 26Fe, 28Ni, 29 and 32Ge by 0.75 to 4.5 MeV 7Li+ Ions NUCLEAR REACTIONS Ge, Cu, Ni, Fe, Ca(7Li, X), E=0.75-4.5 MeV; measured L-subshell X-ray production σ(E); deduced detector efficiency. Windowless Si(Li), high purity Ge detectors. Model comparison. ATOMIC PHYSICS Ge, Cu, Ni, Fe, Ca(7Li, X), E=0.75-4.5 MeV; measured L-subshell X-ray production σ(E); deduced detector efficiency. Windowless Si(Li), high purity Ge detectors. Model comparison.
doi: 10.1016/0168-583X(91)95962-D
1991WE20 Nucl.Instrum.Methods Phys.Res. B56/57, 964 (1991) D.L.Weathers, J.L.Duggan, M.R.McNeir, Y.C.Yu, F.D.McDaniel, C.A.Quarles, H.Lehtihet, D.Kahler Efficiency Determination for a Windowless Si(Li) X-Ray Detector for Photon Energies Below 5 keV Using Atomic-Field Bremsstrahlung NUCLEAR REACTIONS 197Au, Ag, 27Al(γ, X), E=0.6 keV; measured X-ray spectra; deduced detector efficiency. Windowless Si(Li) X-ray detector. ATOMIC PHYSICS 197Au, Ag, 27Al(γ, X), E=0.6 keV; measured X-ray spectra; deduced detector efficiency. Windowless Si(Li) X-ray detector.
doi: 10.1016/0168-583X(91)95072-L
1991YU03 Phys.Rev. A44, 5702 (1991) Y.C.Yu, M.R.McNeir, D.L.Weathers, J.L.Duggan, F.D.McDaniel, G.Lapicki K-Shell X-Ray-Production Cross Sections in 6C, 8O, 9F, 11Na, 12Mg, and 13Al by 0.75- to 4.5-MeV Protons NUCLEAR REACTIONS C, O, 19F, 23Na, Mg, 27Al(p, X), E=0.75-4.5 MeV; measured K-Shell X-ray production σ. Model comparison. ATOMIC PHYSICS C, O, 19F, 23Na, Mg, 27Al(p, X), E=0.75-4.5 MeV; measured K-shell X-ray production σ. Model comparison.
doi: 10.1103/PhysRevA.44.5702
1991YU04 Nucl.Instrum.Methods Phys.Res. B56/57, 1188 (1991); see 1991Yu06 Y.C.Yu, M.R.McNeir, D.L.Weathers, D.K.Marble, J.L.Duggan, F.D.McDaniel, G.Lapicki K-Shell X-Ray Production Cross Sections in 6C, 8O, 11Na, 12Mg and 13Al by 0.75 to 5.0 MeV 7Li+ Ions
doi: 10.1016/0168-583X(91)95128-Z
1991YU05 Phys.Rev. A44, 7252 (1991) Y.C.Yu, M.R.McNeir, D.L.Weathers, J.L.Duggan, F.D.McDaniel, D.K.Marble, Z.Y.Zhao, G.Lapicki K-Shell X-Ray Production in 6C, 8O, 9F, 11Na, 12Mg, and 13Al by 0.5-8.0-MeV Helium Ions NUCLEAR REACTIONS C, O, 19F, 23Na, Mg, 27Al(α, X), E=0.5-8 MeV; measured K-shell X-ray production σ. ATOMIC PHYSICS C, O, 19F, 23Na, Mg, 27Al(α, X), E=0.5-8 MeV; measured K-shell X-ray production σ.
doi: 10.1103/PhysRevA.44.7252
1991YU06 Nucl.Instrum.Methods Phys.Res. B56/57, 1188 (1991) Y.C.Yu, M.R.McNeir, D.L.Weathers, D.K.Marble, J.L.Duggan, F.D.McDaniel, G.Lapicki K-Shell X-Ray Production Cross Section in 6C, 8O, 11Na, 12Mg and 13Al by 0.75 to 5.0 MeV 7Li+ Ions NUCLEAR REACTIONS C, O, 23Na, Mg, 27Al(7Li, X), E=0.75-5 MeV; measured K-shell X-ray production σ(E). Analytical windowless Si(Li) detector. ATOMIC PHYSICS C, O, 23Na, Mg, 27Al(7Li, X), E=0.75-5 MeV; measured K-shell X-ray production σ(E). Analytical windowless Si(Li) detector.
doi: 10.1016/0168-583X(91)95128-Z
1989GR08 Nucl.Instrum.Methods Phys.Res. B40/41, 116 (1989) J.D.Gressett, D.K.Marble, F.D.McDaniel, J.L.Duggan, J.F.Culwell, G.Lapicki M-Shell X-Ray Production in Gold, Lead, Bismuth, Thorium and Uranium by 70-200 keV Protons NUCLEAR REACTIONS 197Au, Pb, 209Bi, Th, U(p, X), E=70-200 keV; measured M X-ray production σ. ATOMIC PHYSICS 197Au, Pb, 209Bi, Th, U(p, X), E=70-200 keV; measured M X-ray production σ.
doi: 10.1016/0168-583X(89)90936-1
1989MA26 Nucl.Instrum.Methods Phys.Res. B40/41, 98 (1989) D.K.Marble, J.D.Gressett, F.D.McDaniel, J.L.Duggan, J.F.Culwell, G.Lapicki L-Shell X-Ray Production in Copper, Germanium, Rubidium, Strontium and Yttrium by 100-225 keV Protons NUCLEAR REACTIONS Cu, Ge, Rb, Sr, 89Y(p, X), E=100-225 keV; measured L X-ray production σ. ATOMIC PHYSICS Cu, Ge, Rb, Sr, 89Y(p, X), E=100-225 keV; measured L X-ray production σ.
doi: 10.1016/0168-583X(89)90932-4
1988PR01 Phys.Rev. A37, 365 (1988) J.L.Price, J.L.Duggan, F.D.McDaniel, G.Lapicki, R.Mehta M-Shell X-Ray Production Cross Sections for 0.5-2.5-MeV Be+ Ions Incident upon Selected Elements from Praseodymium to Bismuth ATOMIC PHYSICS 141Pr, Nd, Eu, Dy, 165Ho, Hf, W, 197Au, Pb, 209Bi(9Be, X), E=0.5-2.5 MeV; measured M-shell X-ray production σ(E).
doi: 10.1103/PhysRevA.37.365
1987AN10 Phys.Rev. A36, 3699 (1987) M.C.Andrews, F.D.McDaniel, J.L.Duggan, P.D.Miller, P.L.Pepmiller, H.F.Krause, T.M.Rosseel, L.A.Rayburn, R.Mehta, G.Lapicki L- and M-Shell X-ray Production Cross Sections of Nd, Gd, Ho, Yb, Au, and Pb by 25-MeV Carbon and 32-MeV Oxygen Ions ATOMIC PHYSICS Nd, Gd, Ho, Yb, Au, Pb(12C, X), E=25 MeV; measured L X-ray, M X-ray production σ.
doi: 10.1103/PhysRevA.36.3699
1987BH04 Nucl.Instrum.Methods Phys.Res. B24/25, 180 (1987) R.P.Bhalla, F.D.McDaniel, G.Lapicki Carbon K-Shell X-Ray and Auger-Electron Cross Sections and Fluorescence in Benzene Bombarded by 0.6 to 2.0 MeV Protons ATOMIC PHYSICS C(p, X), E=0.6-2.0 MeV; measured K X-ray, Auger electron σ, fluorescence yields. Proportional counter, electrostatic analyzer.
doi: 10.1016/0168-583X(87)90617-3
1987MC05 Nucl.Instrum.Methods Phys.Res. B27, 500 (1987) Molecular Effects in Carbon K-Shell Auger-Electron Production by 0.6-2.0 MeV Protons and Extraction of an Atomic Cross Section NUCLEAR REACTIONS C(p, X), E=0.6-2 MeV; measured K-shell Auger electron σ(E); deduced atomic σ.
doi: 10.1016/0168-583X(87)90083-8
1987PR04 Nucl.Instrum.Methods Phys.Res. B24/25, 85 (1987) J.L.Price, J.L.Duggan, F.D.McDaniel, G.Lapicki, R.Mehta L-Shell X-ray Production Cross Sections for 0.5-2.5 MeV Be+ Ions Incident upon Selected Elements From Z = 29 to 47 ATOMIC PHYSICS Cu, Zn, Ge, Br, Zr, Ag(9Be, X), E=0.5-2.5 MeV; measured L X-ray production σ. Si-Li X-ray detector.
doi: 10.1016/0168-583X(87)90595-7
1985DU07 Phys.Rev. A32, 2088 (1985) J.L.Duggan, P.M.Kocur, J.L.Price, F.D.McDaniel, R.Mehta, G.Lapicki L-Shell X-Ray Production Cross Sections of Ni, Cu, Ge, As, Rb, Sr, Y, Zr, and Pd by (0.25-2.5)-MeV Protons NUCLEAR REACTIONS Ni, Cu, Ge, As, Rb, Sr, Y, Zr, Pd(p, X), E=0.25-2.5 MeV; measured L X-ray production σ(E).
doi: 10.1103/PhysRevA.32.2088
1983MC05 Nucl.Instrum.Methods 214, 57 (1983) Direct Ionization and Capture in Inner-Shell Processes ATOMIC PHYSICS Sc, Ti, Cu, Ge(Si, X), E=52 MeV; Nd, Ho, Au(19F, X), (Si, X), E=1.86 MeV/nucleon; Nd, Ho, Au(Cl, X), E=1.8 MeV/nucleon; measured X-ray production σ; deduced direct ionization, electron capture contributions.
doi: 10.1016/0167-5087(83)90540-9
1983ME16 Phys.Rev. A28, 2722 (1983) R.Mehta, J.L.Duggan, F.D.McDaniel, M.C.Andrews, G.Lapicki, P.D.Miller, L.A.Rayburn, A.R.Zander Direct Ionization and Electron Capture in M-Shell X-Ray Production by Fluorine Ions ATOMIC PHYSICS Au, Pb, Bi, U(19F, X), E=25, 27, 35 MeV; measured M-shell X-ray production σ.
doi: 10.1103/PhysRevA.28.2722
1982ME11 Phys.Rev. A26, 1883 (1982) R.Mehta, J.L.Duggan, J.L.Price, F.D.McDaniel, G.Lapicki M-Shell X-Ray-Production Cross Sections in Thin Targets of 79Au, 82Pb, 83Bi, and 92U by 0.3-2.6 MeV 11H+ and 42He+ Ions ATOMIC PHYSICS Au, Pb, Bi, U(p, X), (α, X), E=0.3-2.6 MeV; measured E(X-ray), I(X-ray), X-ray production σ; deduced electron capture contribution. First Born approximation calculations.
doi: 10.1103/PhysRevA.26.1883
1978GL04 Phys.Rev. C18, 2520 (1978) G.P.Glasgow, F.D.McDaniel, J.L.Weil, J.D.Brandenberger, M.T.McEllistrem Level and Decay Scheme Studies in 92Zr and 94Zr via (n, n'γ) Reactions NUCLEAR REACTIONS 92,94Zr(n, n'γ), E=2.2-3.7 MeV; measured Eγ, σ(E, Eγ, 90°), σ(Eγ, θγ). 92,94Zr deduced levels, δ, J, π, branching ratio. Enriched targets, Ge(Li) detectors, tof background suppression. Statistical model calculation.
doi: 10.1103/PhysRevC.18.2520
1976BR42 Nucl.Instrum.Methods 138, 321 (1976) J.D.Brandenberger, F.D.Snyder, J.D.Dawson, T.W.Burrows, F.D.Mcdaniel A new method of absolute neutron flux determination using an associated γ-ray technique
doi: 10.1016/0029-554X(76)90042-2
1975LA18 Phys.Lett. 58B, 293 (1975) C.Lagrange, R.E.Shamu, T.Burrows, G.P.Glasgow, G.Hardie, F.D.McDaniel Effect of Nuclear Deformation on Neutron Elastic Scattering NUCLEAR REACTIONS 148,154Sm(n, n'), E=6.25 MeV; measured σ(En', θ). 148,154Sm(n, n), E=6.25 MeV; measured σ(θ). 148,154Sm deduced β.
doi: 10.1016/0370-2693(75)90656-5
1975MC11 Phys.Rev. A11, 1607 (1975) F.D.McDaniel, T.J.Gray, R.K.Gardner K-Shell X-Ray Production Cross Sections of Selected Elements from Ti to Y for 0.5- to 2.5-MeV Alpha-Particle Bombardment ATOMIC PHYSICS Ti, V, Cr, Fe, Ni, Cu, Zn, Ga, As, Se, Rb, Sr, Y(α, X), E=0.5-2.5 MeV; measured K X-ray yields.
doi: 10.1103/PhysRevA.11.1607
1974MC13 Phys.Rev. C10, 1087 (1974) F.D.McDaniel, J.D.Brandenberger, G.P.Glasgow, H.G.Leighton Elastic and Inelastic Scattering of 1.5-MeV Neutrons by the Even-A Isotopes of Zirconium and Molybdenum NUCLEAR REACTIONS 90,92,94Zr, 92,94,96,100Mo(n, n), (n, n'), En=1.5 MeV; measured σ(θ), σ(En', θ); deduced optical model parameters. Isotopically enriched samples, neutron time of flight, dynamic bias, compound-elastic scattering, level width fluctuations.
doi: 10.1103/PhysRevC.10.1087
1974MC14 Phys.Rev. C10, 1124 (1974) Nuclear Lifetime of States in 94Tc and 96Tc via the Pulsed-Beam, Direct-Timing Techniques NUCLEAR REACTIONS 94Mo(p, nγ), E=5.82 MeV; 96Mo(p, nγ), E=5.46 MeV; measured γ(t). 94,96Tc levels deduced T1/2.
doi: 10.1103/PhysRevC.10.1124
1973GL03 Priv.Comm. (June 1973) G.P.Glasgow, F.D.McDaniel, L.D.Brandenburger, J.L.Weil, M.T.McEllistrem Resolution of Ambiguities in the Level Scheme of 94Zr
1973ST12 Phys.Rev. C7, 2304 (1973) M.F.Steuer, R.M.Wood, M.W.McDonald, F.D.McDaniel, M.P.Etten Spin-Flip Probability for 7.44-MeV Neutrons Scattered Inelastically (Q = -1.78 MeV) by a Silicon Target NUCLEAR REACTIONS Si(n, n'), E=7.44 MeV; measured σ(E(n')). Deduced spin-flip probability.
doi: 10.1103/PhysRevC.7.2304
1972MC03 Nucl.Phys. A180, 497 (1972) Proton Spin-Flip in the Microscopic Distorted-Wave Approximation NUCLEAR REACTIONS 54Fe(p, p), E=19.6 MeV; analyzed σ(θ), P(θ), spin-flip probability. Antisymmetrized DW approximation.
doi: 10.1016/0375-9474(72)90875-5
1972MC20 Phys.Rev. C6, 1181 (1972) F.D.McDaniel, M.W.McDonald, M.F.Steuer, R.M.Wood Spin-Flip Probability in the Inelastic Scattering of 7.48-MeV Neutrons From the 4.43-MeV State of 12C NUCLEAR REACTIONS 12C(n, n'γ), E=7.48 MeV; measured σ(En', Eγ, θ(n')); deduced spin-flip probability(θ).
doi: 10.1103/PhysRevC.6.1181
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