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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, T1/2, 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 T1/2.

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, T1/2; 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, T1/2; 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
Citations: PlumX Metrics


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 T1/2.

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
Citations: PlumX Metrics


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, T1/2, branching ratios, γ-mixing.

doi: 10.1103/PhysRev.188.1806
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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.


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