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NSR database version of March 21, 2024.

Search: Author = J.L.Duggan

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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
Citations: PlumX Metrics


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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
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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
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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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0447.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0468.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2331.


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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0189.


1968DU11      J.Nucl.Energy 22, 611 (1968)

J.L.Duggan

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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0413.


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
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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)

J.L.Duggan, M.M.Duncan

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA1485.


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)

J.L.Duggan, M.M.Duncan

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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