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Search: Author = C.E.Moss

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2003MO10      Nucl.Instrum.Methods Phys.Res. A505, 374 (2003)

C.E.Moss, C.M.Frankle, V.N.Litvinenko, H.R.Weller

Recent results using the high intensity γ-ray source facility

NUCLEAR REACTIONS Cu(γ, X), E=3.45-11.96 MeV; measured attenuation σ. Free-electron laser.

doi: 10.1016/S0168-9002(03)01100-8
Citations: PlumX Metrics

1993AM06      Nucl.Sci.Eng. 115, 1 (1993)

W.B.Amian, R.C.Byrd, D.A.Clark, C.A.Goulding, M.M.Meier, G.L.Morgan, C.E.Moss

Differential Neutron Production Cross Sections for 597-MeV Protons

NUCLEAR REACTIONS C, ²⁷Al, Fe, Pb, Ni, B, O, ²³⁸U(p, xn), E=597 MeV; measured σ(θn, En). Intranuclear cascade evaporation model.

doi: 10.13182/NSE93-A35517
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0169.

1992AM03      Nucl.Instrum.Methods Phys.Res. A313, 452 (1992)

W.B.Amian, M.M.Meier, R.C.Byrd, C.A.Goulding, G.L.Morgan, C.E.Moss

Efficiency Calibration of a Cylindrical BC418 Neutron Detector at Neutron Energies between 135 and 800 MeV

NUCLEAR REACTIONS Pb, ⁷Li(p, n), E ≤ 800 MeV; measured neutron detection efficiency for E=135-800 MeV; Fe(n, n), E=110-725 MeV; measured total σ. Cylindrical BC418 neutron detector, efficiency calibration.

doi: 10.1016/0168-9002(92)90823-M
Citations: PlumX Metrics

1992AM07      Nucl.Sci.Eng. 112, 78 (1992)

W.B.Amian, R.C.Byrd, C.A.Goulding, M.M.Meier, G.L.Morgan, C.E.Moss, D.A.Clark

Differential Neutron Production Cross Sections for 800-MeV Protons

NUCLEAR REACTIONS U, B, C, N, O, ²⁷Al, Fe, Cd, W, Pb, ⁹Be(p, xn), E=800 MeV; measured σ(θ, En). Model comparison, tof.

doi: 10.13182/NSE92-A23953
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0170.

1992ME04      Nucl.Sci.Eng. 110, 289 (1992)

M.M.Meier, W.B.Amian, C.A.Goulding, G.L.Morgan, C.E.Moss

Differential Neutron Production Cross Sections for 256-MeV Protons

NUCLEAR REACTIONS ⁹Be, C, O, ²⁷Al, Fe, Pb, ²³⁸U(p, xn), E=256 MeV; measured σ(θ, En). Tof technique, intranuclear cascade evaporation. Model comparison.

doi: 10.13182/NSE92-A23901
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0168.

1992ME05      Nucl.Sci.Eng. 110, 299 (1992)

M.M.Meier, W.B.Amian, C.A.Goulding, G.L.Morgan, C.E.Moss

Neutron Yields from Stopping-Length Targets for 256-MeV Protons

NUCLEAR REACTIONS ⁹Be, C, ²⁷Al, Fe(p, xn), E=256 MeV; measured absolute neutron yields; deduced neutron production mechanism. Tof techniques, intranuclear cascade evaporation-model calculations.

doi: 10.13182/NSE92-A23902
Citations: PlumX Metrics

1990MO35      Nucl.Instrum.Methods Phys.Res. A299, 98 (1990)

C.E.Moss, J.R.Streetman

Comparison of Calculated and Measured Response Functions for Germanium Detectors

RADIOACTIVITY ⁶⁵Zn, ¹³⁷Cs, ¹¹³Sn; measured γ-spectra; deduced detector response functions. Closed-end hyperpure Ge detectors. Monte Carlo simulations.

doi: 10.1016/0168-9002(90)90755-U
Citations: PlumX Metrics

1989AM03      Nucl.Instrum.Methods Phys.Res. A281, 353 (1989)

W.B.Amian, M.M.Meier, R.C.Byrd, C.A.Goulding, C.E.Moss

Efficiency Calibration of a Cylindrical BC418 Neutron Detector at Neutron Energies between 30 and 200 MeV

NUCLEAR REACTIONS ⁷Li(p, n), E not given; measured neutron spectra; deduced detector efficiency. Tof, BC418 detector.

doi: 10.1016/0168-9002(89)91333-8
Citations: PlumX Metrics

1989ME08      Nucl.Sci.Eng. 102, 310 (1989)

M.M.Meier, D.A.Clark, C.A.Goulding, J.B.McClelland, G.L.Morgan, C.E.Moss, W.B.Amian

Differential Neutron Production Cross Sections and Neutron Yields from Stopping-Length Targets for 113-MeV Protons

NUCLEAR REACTIONS Be, C, ²⁷Al, Fe, U, O, Pb, W(p, xn), E=113 MeV; measured σ(θn, En). Thin elemental targets.

doi: 10.13182/NSE89-A27480
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0171.

1987HO10      Nucl.Instrum.Methods Phys.Res. B24/25, 503 (1987)

C.L.Hollas, D.A.Close, C.E.Moss

Analysis of Fissionable Material using Delayed Gamma Rays from Photofission

NUCLEAR REACTIONS ²³²Th, ^235,238U, ²³⁹Pu(γ, F)¹³⁸Cs/⁹⁴Sr/¹³⁶I/⁸⁹Rb/⁹⁰Kr/⁹⁷Y, E=10 MeV bremsstrahlung; measured fission product Iγ ratios. Enriched ²³⁵U, ²³⁹Pu targets.

doi: 10.1016/0168-583X(87)90695-1
Citations: PlumX Metrics

1986MO09      Radiat.Eff. 94, 81 (1986)

C.E.Moss

Gamma-Ray Line Intensities for Depleted Uranium

RADIOACTIVITY ²³⁴Pa(β^-); ^234mPa(β^-), (IT) [from depleted ²³⁸U decay chain]; measured Iγ. ²³⁴U levels deduced γ-branching ratio following isomer decay.

doi: 10.1080/00337578608208359
Citations: PlumX Metrics

1978NO05      Phys.Rev. C18, 102 (1978)

E.B.Norman, C.N.Davids, C.E.Moss

Energy Levels of ⁶⁰Fe Populated by the ⁵⁸Fe(t, p)⁶⁰Fe Reaction

NUCLEAR REACTIONS ⁵⁸Fe(t, p), E=17.0 MeV; measured σ(Ep, θ); deduced Q. ⁶⁰Fe deduced mass excess, levels, L, J, π. Q3D spectrograph, enriched targets.

doi: 10.1103/PhysRevC.18.102
Citations: PlumX Metrics

1977AN01      Phys.Rev. C15, 123 (1977)

R.E.Anderson, J.J.Kraushaar, I.C.Oelrich, R.M.DelVecchio, R.A.Naumann, E.R.Flynn, C.E.Moss

Excitation of Particle-Vibration Multiplets in the A = 110 Region by Two-Neutron Stripping Reactions

NUCLEAR REACTIONS ¹⁰³Rh, ^106,108Pd, ^107,109Ag(t, p), E=17.0 MeV; measured σ(Ep, θ). ¹⁰⁵Rh, ^108,110Pd, ^109,111Ag deduced levels, L, J, π, enhancement. Enriched targets, magnetic spectrograph, DWBA analysis, weak coupling model.

doi: 10.1103/PhysRevC.15.123
Citations: PlumX Metrics

1977MA12      Phys.Rev. C15, 1708 (1977)

J.F.Mateja, C.P.Browne, C.E.Moss, J.B.McGrory

Level Structure of ⁵⁷Mn from a ⁵⁵Mn(t, p)⁵⁷Mn Reaction Study and a Mixed-Configuration Shell Model Calculation

NUCLEAR REACTIONS ⁵⁵Mn(t, p), E=17.0 MeV; measured σ(Ep, θ); deduced Q. ⁵⁷Mn deduced levels, J, π, L, enhancement factors.

doi: 10.1103/PhysRevC.15.1708
Citations: PlumX Metrics

1976MO09      Nucl.Phys. A259, 413 (1976)

C.E.Moss, J.D.Sherman

Excitation Energies of Levels in ²⁷Al and ²⁸Si

NUCLEAR REACTIONS ²⁷Al(p, p'), ²⁸Si(p, p'), E=16.000, 20.000 MeV; measured σ(Ep'). ²⁷Al, ²⁸Si deduced levels. Enriched targets.

doi: 10.1016/0375-9474(76)90076-2
Citations: PlumX Metrics

1976MO27      Nucl.Phys. A269, 429 (1976)

C.E.Moss

Excitation Energies of Levels in ²³Na, ²⁴Mg and ²⁶Mg

NUCLEAR REACTIONS ²³Na, ^24,26Mg(p, p'), E=20 MeV; measured σ(Ep'). ²³Na, ^24,26Mg deduced levels. Enriched targets.

doi: 10.1016/0375-9474(76)90691-6
Citations: PlumX Metrics

1974MO23      Nucl.Phys. A235, 11 (1974)

C.E.Moss, C.S.Zaidins

(³He, 2n) Excitation Functions for Some Light Nuclei

NUCLEAR REACTIONS ⁹Be(³He, 2n), E=10-41 MeV; ²⁴Mg(³He, 2n), E=21-43 MeV; ²⁷Al(³He, 2n), E=14-41 MeV; measured σ(E). Natural, enriched targets.

doi: 10.1016/0375-9474(74)90175-4
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetB0005.

1973BA13      Ann.Phys.(New York) 76, 437 (1973)

H.W.Baer, J.J.Kraushaar, C.E.Moss, N.S.P.King, R.E.L.Green, P.D.Kunz, E.Rost

Study of the (p, t) Reaction on the Even-A Titanium Isotopes

NUCLEAR REACTIONS ^46,48,50Ti(p, t), E=19, 23, 27 MeV; measured σ(Et, θ). Deduced L. ^44,46,48Ti deduced levels, J, π.

doi: 10.1016/0003-4916(73)90043-2
Citations: PlumX Metrics

1973MO06      Aust.J.Phys. 26, 17 (1973)

C.E.Moss, R.H.Spear, F.Ahmad, A.M.Baxter, L.E.Carlson, P.R.Gardner

Gamma Ray Decay Schemes of Levels at Intermediate Energies in ³²S

NUCLEAR REACTIONS ³²S(p, p'γ), E=8.03-9.17 MeV; measured pγ-coin. ³²S levels deduced branching ratios.

doi: 10.1071/PH730017
Citations: PlumX Metrics

1972GA43      Aust.J.Phys. 25, 659 (1972)

P.R.Gardner, C.E.Moss, R.H.Spear, L.E.Carlson

The 5.80 MeV State of ³²S

NUCLEAR REACTIONS ²⁹Si(α, nγ), E=8.7, 8.8, 9.8 MeV; measured σ(E, Eγ, θ), Doppler shift; ³²S(p, p'γ), E=8.63 MeV; measured Eγ, Iγ. ³²S level deduced J, π, T_1/2, γ-branching.

doi: 10.1071/PH720659
Citations: PlumX Metrics

1972MO02      Nucl.Phys. A179, 89 (1972)

C.E.Moss, N.S.P.King, A.B.Comiter, R.A.Ristinen

The (p, nγ) Reaction on ²⁷Al and ²⁸Si

NUCLEAR REACTIONS ²⁷Al, ²⁸Si(p, nγ), E=16, 23 MeV; measured Eγ, Iγ, nγ-coin. ²⁷Al, ²⁸Si(p, n), E=16, 23 MeV; measured En. ²⁷Si, ²⁸P deduced levels, γ-branching ratios. Ge(Li) detector.

doi: 10.1016/0375-9474(72)90107-8
Citations: PlumX Metrics

1972MO08      Phys.Rev. C5, 1122 (1972)

C.E.Moss, C.Detraz, C.S.Zaidins, D.J.Frantsvog

Half-Lives of ²⁰Na and ³⁶K

RADIOACTIVITY ²⁰Na, ³⁶K; measured T_1/2.

doi: 10.1103/PhysRevC.5.1122
Citations: PlumX Metrics

1971DE04      Phys.Rev.Lett. 26, 448 (1971)

C.Detraz, C.E.Moss, C.D.Zafiratos, C.S.Zaidins

Isospin Purity at High Excitation Energies as Evidenced by Cross Correlations of Mirror-Channel Fluctuations

NUCLEAR REACTIONS ¹⁹F(³He, ⁷Li), (³He, ⁷Be), E=39-42 MeV; measured σ(E). ²²Na compound-nucleus excitations deduced isospin purity. Cross-correlation fluctuation analysis.

doi: 10.1103/PhysRevLett.26.448
Citations: PlumX Metrics

1971DE05      Phys.Lett. 34B, 128 (1971)

C.Detraz, C.E.Moss, C.S.Zaidins

Beta Decay of ²³Mg, ²⁷Si, ³¹S, ³⁵Ar and ³⁹Ca

RADIOACTIVITY ²³Mg, ²⁷Si, ³¹S, ³⁵Ar, ³⁹Ca; measured β-delayed γ-spectra; deduced log ft, branching ratios.

doi: 10.1016/0370-2693(71)90686-1
Citations: PlumX Metrics

1971DE14      Nucl.Phys. A167, 337 (1971)

C.Detraz, C.E.Moss, C.D.Zafiratos, C.S.Zaidins

The ¹⁹F(³He, ⁶Li)¹⁶O Reaction at 40 MeV. A Study of the Multi-Particle-Multi-Hole Structure of ¹⁶O States

NUCLEAR REACTIONS ¹⁹F(³He, ⁶Li), E=37.7 to 41.2 MeV; measured σ(E(⁶Li), θ); deduced reaction mechanism. ¹⁶O levels deduced S, configurations.

doi: 10.1016/0375-9474(71)90080-7
Citations: PlumX Metrics

1971DE37      Nucl.Phys. A177, 258 (1971)

C.Detraz, C.D.Zafiratos, C.E.Moss, C.S.Zaidins

Investigation of the Mechanism of tau-Induced Four-Nucleon Pick-up Reactions

NUCLEAR REACTIONS ¹²C, ¹⁹F(³He, ⁷Li), E=37.7 - 41.2mev; measured σ(E(³He), E(⁷Li), θ). ¹⁹F(³He, ⁷Be), E=41 MeV; measured σ(E(⁷Be), θ). ¹⁴N, ¹⁶O, ²⁰Ne, ²²Ne, ²⁷Al, ²⁸Si, ⁴⁰Ar, ⁴⁰Ca(³He, ⁷Be), E=41 MeV; measured σ(10° cm). ¹⁴N, ¹⁶O, ²⁰Ne, ²⁷Al, ⁴⁰Ar(³He, ⁷Li), E=41 MeV; measured σ(10° cm). Reaction mechanisms deduced.

doi: 10.1016/0375-9474(71)90173-4
Citations: PlumX Metrics

1971KI17      Nucl.Phys. A177, 625 (1971)

N.S.P.King, C.E.Moss, H.W.Baer, R.A.Ristinen

A Study of Excited States in ⁵⁸Cu, ⁵⁴Co, ⁵⁰Mn and ⁴⁶V

NUCLEAR REACTIONS ⁴⁶Ti, ⁵⁰Cr, ⁵⁴Fe, ⁵⁸Ni(p, nγ), E=7-16 MeV; measured σ(E;En, Eγ). ⁴⁶Ti, ⁵⁰Cr, ⁵⁴Fe, ⁵⁸Ni(p, n), E=14.5 MeV; measured En. ⁴⁶Ti(³He, t), E=30 MeV; measured σ(Et). ⁴⁶V, ⁵⁰Mn, ⁵⁴Co, ⁵⁸Cu deduced levels, J. Enriched targets, Ge(Li) detector.

doi: 10.1016/0375-9474(71)90311-3
Citations: PlumX Metrics

1971MO23      Nucl.Phys. A170, 111 (1971)

C.E.Moss, C.Detraz, C.S.Zaidins

Beta Decay of ²⁵Al and ³⁷K

RADIOACTIVITY ²⁵Al[from ²⁸Si(p, α)], ³⁷K[from ⁴⁰Ca(p, α)]; measured Iγ, Eγ, T_1/2; deduced log ft.

doi: 10.1016/0375-9474(71)90685-3
Citations: PlumX Metrics

1971MO27      Nucl.Phys. A174, 408 (1971)

C.E.Moss, C.Detraz, C.S.Zaidins

Beta Decay of ²⁶Si, ³⁰S and ³⁴Ar

RADIOACTIVITY ²⁶Si[from ²⁴Mg(³He, n)], ³⁰S[from ²⁸Si(³He, n)], ³⁴Ar[from ³²S(³He, n)]; measured Iγ, Eγ, T_1/2; deduced log ft.

doi: 10.1016/0375-9474(71)90673-7
Citations: PlumX Metrics

1971MO34      Nucl.Phys. A178, 241 (1971)

C.E.Moss, A.B.Comiter

Excitation Energies of Levels in ¹⁶F, ²⁰Na and ²⁴Al

NUCLEAR REACTIONS ¹⁶O, ²⁰Ne, ²⁴Mg(p, n), E=23 MeV; measured En. ¹⁶F, ²⁰Na, ²⁴Al deduced levels. Natural, enriched targets.

doi: 10.1016/0375-9474(71)90201-6
Citations: PlumX Metrics

1971ZA06      Phys.Rev.Lett. 27, 437 (1971)

C.D.Zafiratos, C.Detraz, C.E.Moss, C.S.Zaidins

Comparison between the (³He, ⁷Be) α-Pickup Reactions on ⁴⁰Ca and ⁴⁰Ar

NUCLEAR REACTIONS ⁴⁰Ca, ⁴⁰Ar(³He, ⁷Be), E=41 MeV; measured σ(E(⁷Be), θ).

doi: 10.1103/PhysRevLett.27.437
Citations: PlumX Metrics

1970BA40      Phys.Rev.Lett. 25, 1035 (1970)

H.W.Baer, J.J.Kraushaar, C.E.Moss, N.S.P.King, R.E.L.Green

Inadequacies in a Conventional Distorted-Wave Born-Approximation Analysis of (p, t) Transitions in Titanium Isotopes at E = 27 MeV

NUCLEAR REACTIONS ^46,48,50Ti(p, t), E=27 MeV; measured σ(Et, θ). ^44,46,48Ti transitions deduced L. DWBA.

doi: 10.1103/PhysRevLett.25.1035
Citations: PlumX Metrics

1970LA17      Nucl.Phys. A158, 43 (1970)

G.P.Lamaze, C.R.Gould, C.E.Moss, N.R.Roberson, D.R.Tilley

An Angular Correlation Study of the Low-Lying Levels of ²⁹P

NUCLEAR REACTIONS ³²S(p, αγ), E=12.12, 12.89 MeV; measured σ(Eα, Eγ, θ(αγ)). ²⁹P deduced levels, J, π, γ-branching ratios, γ-mixing ratios. Natural targets.

doi: 10.1016/0375-9474(70)90048-5
Citations: PlumX Metrics

1970MO08      Nucl.Phys. A145, 423 (1970)

C.E.Moss

Nuclear Energy Levels of ³¹S and ³³Cl

NUCLEAR REACTIONS ³²S(³He, α), (³He, αγ), (³He, d), E=8.0-12.2 MeV; measured σ(Eα, θ), σ(Eα, Eγ, θ(αγ)), σ(Ed, θ); deduced Q. ³⁶Ar(p, α), E=12.0 MeV; measured σ(Eα). ³¹S, ³³Cl deduced levels, L(n), L(p), J, π, γ-branching ratios, γ-mixing ratios. Natural, enriched targets.

doi: 10.1016/0375-9474(70)90434-3
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1970MO09      Nucl.Phys. A144, 577 (1970)

C.E.Moss, R.V.Poore, N.R.Roberson, D.R.Tilley

Spins of Levels in ³²P and ³⁴S

NUCLEAR REACTIONS ²⁹Si, ³¹P(α, pγ), E=7.65, 8.00 MeV; measured Eγ, σ(Ep, Eγ, θ(pγ)). ³²P, ³⁴S deduced levels, J, γ-branching ratios, γ-mixing ratios. Enriched, natural targets.

doi: 10.1016/0375-9474(70)90346-5
Citations: PlumX Metrics

1970RA24      Phys.Rev. C2, 557 (1970)

C.E.Ragan III, C.E.Moss, C.R.Gould, N.R.Roberson, G.E.Mitchell, D.R.Tilley

Mean Lifetime of the 2.94-MeV Level in ³³S

NUCLEAR REACTIONS ³⁰Si(α, nγ), E=7.8-8.4 MeV; measured σ(E, Eγ), recoil distance. ³³S level deduced T_1/2.

doi: 10.1103/PhysRevC.2.557
Citations: PlumX Metrics

1969MO03      Nucl.Phys. A124, 440(1969)

C.E.Moss

Excitation Energies of Levels in ³¹P

NUCLEAR REACTIONS ²⁹Si(³He, p), E=9.009 MeV; measured σ(Ep). ³⁰Si(³He, d), E=10.010 MeV; measured σ(Ed). ³¹P deduced levels. Enriched targets.

doi: 10.1016/0375-9474(69)90367-4
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1969RA29      Phys.Rev. 188, 1806 (1969); Erratum Phys.Rev. C2, 1581 (1970)

C.E.Ragan III, C.E.Moss, R.V.Poore, N.R.Roberson, G.E.Mitchell, D.R.Tilley

Mean Lifetimes and Branching Ratios of Low-Lying Levels in ³³S

NUCLEAR REACTIONS ³⁰Si(α, nγ), E=5.5-9.0 MeV; measured σ(E, Eγ), Doppler shift attenuation. ³³S deduced levels, T_1/2, branching ratios, γ-mixing.

doi: 10.1103/PhysRev.188.1806
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1968MO16      Phys.Rev. 174, 1333 (1968)

C.E.Moss, R.V.Poore, N.R.Roberson, D.R.Tilley

Spins of Levels in ³³P

NUCLEAR STRUCTURE ³³P; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.174.1333
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1968MO22      Nucl.Phys. A121, 285 (1968)

C.E.Moss

Excitation Energies of Levels in ³⁴S

NUCLEAR REACTIONS ³⁴S(p, p'), E=12.011 MeV; measured σ(Ep'). ³⁴S deduced levels. Enriched target.

doi: 10.1016/0375-9474(68)90421-1
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1967MO04      Nucl.Phys. A96, 1(1967)

C.E.Moss

Non-Existence of a Level at 1.35 MeV in ³³S

NUCLEAR REACTIONS ³²S(d, p), E = 2.541 MeV; measured σ(Ep, θ). ³³S deduced levels. Natural target.

doi: 10.1016/0375-9474(67)90689-6
Citations: PlumX Metrics

1967MO24      Priv.Comm. (1967)

C.E.Moss

NUCLEAR STRUCTURE ³¹S; measured not abstracted; deduced nuclear properties.