NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = J.L.Duggan Found 46 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
1993SU30 Nucl.Instrum.Methods Phys.Res. B79, 194 (1993) H.L.Sun, J.F.Kirchhoff, A.R.Azordegan, J.L.Duggan, D.McDaniel, R.M.Wheeler, R.P.Chaturvedi, G.Lapicki M-Shell Ionization of Rare Earth Elements by Proton Impact in the Energy Range 0.6-4.6 MeV NUCLEAR REACTIONS La, Nd, Sm, Eu, Gd, Dy, 165Ho, Er, Yb, Lu, Hf(p, X), E=0.6-4.6 MeV; measured M-shell X-ray production σ; deduced detector efficiency. Windowless Si(Li) detector. ATOMIC PHYSICS La, Nd, Sm, Eu, Gd, Dy, 165Ho, Er, Yb, Lu, Hf(p, X), E=0.6-4.6 MeV; measured M-shell X-ray production σ; deduced detector efficiency. Windowless Si(Li) detector.
doi: 10.1016/0168-583X(93)95323-W
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
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
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
1973CO19 Phys.Lett. 45B, 321 (1973) W.R.Coker, J.Lin, J.L.Duggan, P.D.Miller Multistep Contributions to 11B(h, α)10B from 8.0 to 12.0 MeV NUCLEAR REACTIONS 11B(3He, α), E=8.0, 10.0, 12.0 MeV; measured σ(θ). 10B level deduced S.
doi: 10.1016/0370-2693(73)90044-0
1973WU01 Nucl.Phys. A199, 23 (1973) R.R.Wu, R.L.Dangle, M.M.Duncan, J.L.Duggan, P.D.Miller, Jung Lin A Study of the 11B(3He, p)13C Reaction at 12, 10, 8, 6 and 4 MeV NUCLEAR REACTIONS 11B(3He, p), E=4, 6, 8, 10, 12 MeV; measured σ(θ). Enriched target.
doi: 10.1016/0375-9474(73)90331-X
1971CO14 Nucl.Phys. A168, 307 (1971) W.R.Coker, P.D.Miller, J.L.Duggan, M.M.Duncan, R.L.Dangle, J.Lin The 14C(t, α0)13C Reaction at 6.0, 8.0 and 10.0 MeV NUCLEAR REACTIONS 14C(3He, α), 14C(3He, 3He), E=6.0, 8.0, 10.0 MeV; 13C(α, α), E=15, 18, 20 MeV; measured σ(θ); deduced optical model parameters. Enriched targets.
doi: 10.1016/0375-9474(71)90795-0
1970DU07 Nucl.Phys. A151, 107 (1970) J.L.Duggan, J.Y.Park, S.D.Danielopoulos, P.D.Miller, J.Lin, M.M.Duncan, R.L.Dangle 3He Elastic Scattering from 10B and 14C in the Range 4 to 18 MeV NUCLEAR REACTIONS 10B(3He, 3He)10B, 14C(3He, 3He)14C, E = 4-18 MeV; measured σ(E;θ); deduced optical potential parameters.
doi: 10.1016/0375-9474(70)90971-1
1969MI15 Nucl.Phys. A136, 229 (1969) P.D.Miller, J.L.Duggan, M.M.Duncan, R.L.Dangle, W.R.Coker, J.Lin 11B(3He, d)12C Spectroscopic Factors NUCLEAR REACTIONS 11B(3He, d), (3He, 3He); E = 10, 12, 18 MeV; measured σ(Ed, θ). 12C levels deduced S. Enriched target.
doi: 10.1016/0375-9474(69)90050-5
1969PA11 Nucl.Phys. A134, 277 (1969) J.Y.Park, J.L.Duggan, P.D.Miller, M.M.Duncan, R.L.Dangle Elastic Scattering of 3He Particles by 9Be and 11B Between 4.0 and 18.0 MeV NUCLEAR REACTIONS 9Be, 11B(3He, 3He), E=4-18 MeV; measured σ(θ); deduced optical-model parameters. Enriched 11B target.
doi: 10.1016/0375-9474(69)91052-5
1968DU11 J.Nucl.Energy 22, 611 (1968) A Study of the 7Li(p, α)α Reaction as a Student Exercise NUCLEAR REACTIONS 7Li(p, α), E=150 keV; measured σ(Eα, θ); deduced Q.
doi: 10.1016/0022-3107(68)90033-6
1967CO03 Nucl.Phys. A91, 97 (1967) W.R.Coker, M.M.Duncan, J.L.Duggan, P.D.Miller An Investigation of the 9Be(3He, p)11B Reaction at Low Energies NUCLEAR REACTIONS 9Be(3He, p), E = 1-3 MeV; measured σ(Ep, θ). 11B deduced levels J, π, L.
doi: 10.1016/0375-9474(67)90453-8
1964DU04 Bull.Am.Phys.Soc. 9, No.5, 553, N1 (1964) J.L.Duggan, M.M.Duncan, V.H.Webb 11B(d, α)9Be Reaction NUCLEAR STRUCTURE 11B; measured not abstracted; deduced nuclear properties.
1964MI01 Bull.Am.Phys.Soc. 9, No.1, 45, DC12 (1964) P.D.Miller, J.L.Duggan, M.M.Duncan Absence of States in Be8 at 7.56, 13.91, and 18.00 MeV NUCLEAR STRUCTURE 7Li; measured not abstracted; deduced nuclear properties.
1964MI10 Nucl.Phys. 54, 155(1964) P.D.Miller, J.L.Duggan, M.M.Duncan Absence of States in Be8 at 7.56, 13.91 and 18.00 MeV NUCLEAR REACTIONS 7Li(p, α), (p, γ), Ep=0.50-2.0 MeV; measured α-, γ-spectra. 8Be deduced levels. Enriched target.
doi: 10.1016/0029-5582(64)90401-8
1963CO24 Bull.Am.Phys.Soc. Southeastern Section, p. 18, S8, (November 1963); Bull.Am.Phys.Soc. 9, No.3, 351, S8 (1964) W.R.Coker, M.M.Duncan, J.L.Duggan, V.H.Webb, P.D.Miller The Be9(He3, p)B11 Reaction NUCLEAR STRUCTURE 9Be; measured not abstracted; deduced nuclear properties.
1963DU02 Bull.Am.Phys.Soc. 8, No.2, 114, I1 (1963) M.M.Duncan, J.L.Duggan, R.D.Purrington Analysis of the Continuum Neutron Spectra from the Bombardment of Li7 by He3 NUCLEAR STRUCTURE 7Li; measured not abstracted; deduced nuclear properties.
1963DU03 Bull.Am.Phys.Soc. 8, No.2, 124, U7 (1963) Energy Levels in C11 NUCLEAR STRUCTURE 9Be; measured not abstracted; deduced nuclear properties.
1963DU12 Nucl.Phys. 46, 336 (1963) J.L.Duggan, P.D.Miller, R.F.Gabbard A Study of the Reactions Be9(He3, n)C11, Li7(He3, n)B9 and C13(He3, n)O15 NUCLEAR STRUCTURE 13C, 9Be, 7Li; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(63)90604-7
1963WE15 Bull.Am.Phys.Soc.Southeastern Section, p.18, S7, (November 1963); Bull.Am.Phys.Soc. 9 No.3, 351, S7 (1963) V.N.Webb, M.M.Duncan, J.Lin, J.L.Duggan, L.E.Akers, H.E.Banta The C14(He3, p)N16, C14(He3, d)N15 and C14(He3, α)C13 Reactions NUCLEAR STRUCTURE 14C; measured not abstracted; deduced nuclear properties.
1962DU01 Bull.Am.Phys.Soc. 7, No.1, 59, R3 (1962) Reactions Li7(He3, n)B9 and Be9(He3, n)C11 NUCLEAR STRUCTURE 7Li; measured not abstracted; deduced nuclear properties.
1962DU03 ORNL-3268, p.12 (1962) J.L.Duggan, P.D.Miller, R.F.Gabbard A Study of the Reactions Be9(He3, n)C11, Li7(He3, n)B9, and C13(He3, n)O15 NUCLEAR STRUCTURE 13C, 7Li, 9Be; measured not abstracted; deduced nuclear properties.
1961GA08 Bull.Am.Phys.Soc. 6, No.5, 416, B6 (1961) R.F.Gabbard, P.D.Miller, J.L.Duggan C13(He3, n)O15 Reaction
1961MI01 Bull.Am.Phys.Soc. 6, No.1, 60, TA2 (1961) P.D.Miller, J.L.Duggan, R.F.Gabbard Angular Yield of Neutrons from the T(p, n)He3 Reaction NUCLEAR STRUCTURE 9B, 11C, 15O; measured not abstracted; deduced nuclear properties.
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