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NSR database version of May 24, 2024.

Search: Author = D.Cohen

Found 28 matches.

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2024LI02      Eur.Phys.J. A 60, 8 (2024)

L.Li, S.Strauch, J.C.Bernauer, W.J.Briscoe, A.Ch.Ndukwe, E.Cline, D.Cohen, K.Deiters, E.J.Downie, I.P.Fernando, A.Flannery, R.Gilman, Y.Ilieva, M.Kohl, I.Lavrukhin, W.Lin, W.Lorenzon, S.Lunkenheimer, P.Mohanmurthy, J.Nazeer, M.Nicol, T.Patel, A.Prosnyakov, H.Reid, P.E.Reimer, G.Ron, T.Rostomyan, O.M.Ruimi, N.Sparveris, D.Yaari

Instrumental uncertainties in radiative corrections for the MUSE experiment

doi: 10.1140/epja/s10050-023-01215-0
Citations: PlumX Metrics


2022CL01      Phys.Rev. C 105, 055201 (2022)

E.Cline, W.Lin, P.Roy, P.E.Reimer, K.E.Mesick, A.Akmal, A.Alie, H.Atac, A.Atencio, C.Ayerbe Gayoso, N.Benmouna, F.Benmokhtar, J.C.Bernauer, W.J.Briscoe, J.Campbell, D.Cohen, E.O.Cohen, C.Collicott, K.Deiters, S.Dogra, E.Downie, I.P.Fernando, A.Flannery, T.Gautam, D.Ghosal, R.Gilman, A.Golossanov, B.F.Halter, J.Hirschman, Y.Ilieva, M.Kim, M.Kohl, B.Krusche, I.Lavrukhin, L.Li, B.Liang-Gilman, A.Liyanage, W.Lorenzon, P.Mohanmurthy, R.Mokal, P.Moran, S.J.Nazeer, P.Or, T.Patel, E.Piasetzky, T.Rauber, R.S.Raymond, D.Reggiani, H.Reid, G.Ron, E.Rooney, T.Rostomyan, M.Schwarz, A.Sneath, P.G.Solazzo, N.Sparveris, N.Steinberg, S.Strauch, V.Sulkosky, N.Wuerfel

Characterization of muon and electron beams in the Paul Scherrer Institute PiM1 channel for the MUSE experiment

doi: 10.1103/PhysRevC.105.055201
Citations: PlumX Metrics


2021BA42      Nucl.Instrum.Methods Phys.Res. B598, 11 (2021)

S.Bakr, D.D.Cohen, R.Siegele, J.W.Archer, S.Incerti, V.Ivanchenko, A.Mantero, A.Rosenfeld, S.Guatelli

Geant4 X-ray fluorescence with updated libraries

doi: 10.1016/j.nimb.2021.09.009
Citations: PlumX Metrics


2019SI21      Nucl.Instrum.Methods Phys.Res. B450, 19 (2019)

R.Siegele, D.D.Cohen, Z.Pastuovic

Heavy ion PIXE cross sections in Ti, Zn, Nb, Ru and Ta for 4.8-30.0 Mev oxygen and 3.0-12.0 MeV lithium beams

NUCLEAR REACTIONS Ti, Zn, Nb, Ru, Ta(Li, X), E=4.8-30 MeV; Ti, Zn, Nb, Ru, Ta(O, X), E=3-12 MeV; measured reaction products, X-rays; deduced σ for K, L lines. Comparison with theoretical calculations.

doi: 10.1016/j.nimb.2018.09.017
Citations: PlumX Metrics


2013FR01      Nucl.Instrum.Methods Phys.Res. A698, 117 (2013)

M.Friedman, D.Cohen, M.Paul, D.Berkovits, Y.Eisen, G.Feinberg, G.Giorginis, S.Halfon, A.Krasa, A.J.M.Plompen, A.Shor

Simulation of the neutron spectrum from the 7Li(p, n) reaction with a liquid-lithium target at Soreq Applied Research Accelerator Facility

NUCLEAR REACTIONS 7Li(p, n), E<3.5 MeV; analyzed available data; deduced neutron source parameters for Maxwellian-averaged σ measurements. Comparison with available data.

doi: 10.1016/j.nima.2012.09.027
Citations: PlumX Metrics


2012FE06      Phys.Rev. C 85, 055810 (2012)

G.Feinberg, M.Friedman, A.Krasa, A.Shor, Y.Eisen, D.Berkovits, D.Cohen, G.Giorginis, T.Hirsh, M.Paul, A.J.M.Plompen, E.Tsuk

Quasi-stellar neutrons from the 7Li(p, n)7Be reaction with an energy-broadened proton beam

NUCLEAR REACTIONS 7Li(p, n)7Be, E=1.85-1.95 MeV; measured time of flight, spectrum, E(n), I(n), σ(θ), narrow and broad-energy proton beam; deduced angle-integrated spectrum and Maxwellian-flux distribution. 27Al(p, γ), E=0.985-1.0 MeV; measured thick-target σ(E). 197Au(n, γ), E<160 keV; measured Eγ, Iγ, average activation σ for neutrons from 7Li(p, n) reaction. Relevance to s-process cross sections.

doi: 10.1103/PhysRevC.85.055810
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset23284.


1995HU23      Nucl.Instrum.Methods Phys.Res. B101, 263 (1995)

M.Hult, M.El Bouanani, L.Persson, H.J.Whitlow, M.Andersson, C.Zaring, M.Ostling, D.D.Cohen, N.Dytlewski, I.F.Bubb, P.N.Johnston, S.R.Walker

Empirical Characterisation of Mass Distribution Broadening in ToF-E Recoil Spectrometry

doi: 10.1016/0168-583X(95)00270-7
Citations: PlumX Metrics


1994HU16      Nucl.Instrum.Methods Phys.Res. B85, 916 (1994)

M.Hult, H.J.Whitlow, M.Ostling, N.Lundberg, C.Zaring, D.D.Cohen, N.Dytlewski, P.N.Johnston, S.R.Walker

RBS and Recoil Spectrometry Analysis of CoSi2 Formation on GaAs

NUCLEAR REACTIONS Ga, As(α, α), E=2.4 MeV; measured Rutherford backscattering spectra, reference, annealed samples. Rutherford back scattering, recoil spectrometry, CoSi2 formation on GaAs.

doi: 10.1016/0168-583X(94)95950-1
Citations: PlumX Metrics


1994JO11      Nucl.Instrum.Methods Phys.Res. B85, 907 (1994)

P.N.Johnston, S.R.Walker, I.F.Bubb, D.D.Cohen, N.Dytlewski, M.Hult, H.J.Whitlow, C.Zaring, M.Ostling, M.Andersson

Mass and Energy Dispersive Recoil Spectrometry of Si(x)Ge(1-x) Grown by Electron Beam Evaporation

NUCLEAR REACTIONS O, Si, Ge, C(127I, X), E=77 MeV; measured recoil energy spectra, X=O, Si, Ge, C respectively; deduced O contaminant, levels quantification. Mass, energy dispersive recoil spectrometry.

doi: 10.1016/0168-583X(94)95948-X
Citations: PlumX Metrics


1994SP03      Phys.Rev. C49, 2398 (1994)

B.M.Spicer, N.Dytlewski, S.Koutsoliotas, D.D.Cohen, M.Geso

Excitation Function for the Population of the 4.51 MeV State of 27Al in Inelastic Proton Scattering: Evidence for 6- strength ( Question )

NUCLEAR REACTIONS, ICPND 27Al(p, p'γ), E=5.6-7.3 MeV; measured Eγ, Iγ, σ(E). 28Si deduced resonance, 6- strength fragmentation features.

doi: 10.1103/PhysRevC.49.2398
Citations: PlumX Metrics


1994TE04      Nucl.Instrum.Methods Phys.Res. B84, 415 (1994)

G.Terwagne, D.D.Cohen, G.A.Collins

Cross-Section Measurements of the 14N(3He, p)16O and 14N(3He, α)13N Reactions between 1.6 and 2.8 MeV

NUCLEAR REACTIONS 14N(3He, p), (3He, α), E=1.6-2.8 MeV; measured σ(θ) vs E; deduced applicability to nitrogen depth profiling.

doi: 10.1016/0168-583X(94)95335-X
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0625.


1992CO08      Nucl.Instrum.Methods Phys.Res. B64, 413 (1992)

D.D.Cohen, G.M.Bailey, N.Dytlewski

3He Induced Charged Particle Reactions for Oxygen Analysis

NUCLEAR REACTIONS 16O(3He, α), (3He, p), E ≈ 2.9-3.8 MeV; measured yields vs E. 16O(3He, pγ), E=2.6 MeV; measured Eγ, Iγ. Thick targets. Thick sample oxygen analysis techniques.

doi: 10.1016/0168-583X(92)95506-M
Citations: PlumX Metrics


1989CO07      At.Data Nucl.Data Tables 41, 287 (1989)

D.D.Cohen

K- and L-Shell Ionization Cross Sections for Deuterons Calculated in the ECPSSR Theory

NUCLEAR STRUCTURE Z=6-95; calculated K-, L-subshell ionization σ for deuteron impact.

ATOMIC PHYSICS Z=6-95; calculated K-, L-subshell ionization σ for deuteron impact.

doi: 10.1016/0092-640X(89)90021-1
Citations: PlumX Metrics


1988CO07      Nucl.Instrum.Methods Phys.Res. A267, 492 (1988)

D.D.Cohen

X-Rays from an 241Am Source and Their Relative Intensities

RADIOACTIVITY 241Am(α); measured E X-ray, I X-ray, Eγ, Iγ. 237Np deduced transitions, branching ratios.

doi: 10.1016/0168-9002(88)90490-1
Citations: PlumX Metrics


1986CO04      At.Data Nucl.Data Tables 34, 393 (1986)

D.D.Cohen, M.Harrigan

Calculated L-Shell X-Ray Line Intensities for Proton and Helium Ion Impact

ATOMIC PHYSICS Z=28-96; calculated α-, proton-induced I(L X-ray).

doi: 10.1016/0092-640X(86)90011-2
Citations: PlumX Metrics


1985CO28      At.Data Nucl.Data Tables 33, 255 (1985)

D.D.Cohen, M.Harrigan

K- and L-Shell Ionization Cross Sections for Protons and Helium Ions Calculated in the ECPSSR Theory

ATOMIC PHYSICS Z=6-95; compiled K-, L-subshell proton-, α-induced ionization σ. PWBA, energy loss, Coulomb deflection, perturbed stationary state, relativistic effects.

doi: 10.1016/0092-640X(85)90004-X
Citations: PlumX Metrics


1984CO24      J.Phys.(London) B17, 3913 (1984)

D.D.Cohen

Comments on Several Analytical Techniques for L-Subshell Ionisation Calculations

ATOMIC PHYSICS Dy, W, Au, Pb, Th, U(α, X), E=1-3 MeV; analyzed X-ray emission rate, production σ data; deduced subshell ionization σ.

doi: 10.1088/0022-3700/17/19/014
Citations: PlumX Metrics


1984HA55      Aust.J.Phys. 37, 475 (1984)

M.F.Harrigan, B.M.Spicer, D.D.Cohen

L-Subshell X-Ray Production by 100-250 keV/a.m.u. Ions

ATOMIC PHYSICS Gd(p, X), E=100-200 keV; Au, W(α, X), E=600-100 keV; measured X-ray yields; deduced L-subshell ionization σ.

doi: 10.1071/PH840475
Citations: PlumX Metrics


1983CO25      Nucl.Instrum.Methods 218, 795 (1983)

D.D.Cohen

L Subshell Ionization Cross Section for Light Ion Bombardment of High Z Targets

NUCLEAR REACTIONS Dy, W, Au, Pb, Th, U(p, X), (α, X), E=1-3 MeV; measured L X-rays; deduced L-subshell ionization σ vs ion velocity.

doi: 10.1016/0167-5087(83)91085-2
Citations: PlumX Metrics


1980AL19      J.Phys.(London) G6, 1173 (1980)

B.J.Allen, D.D.Cohen, F.Z.Company

Radiative Widths of Neutron Scattering Resonances

NUCLEAR REACTIONS 19F, 24Mg, 27Al, 28Si, 56Fe, 207Pb(n, γ), E=20-80 keV; measured σ(Eγ, E). 20F, 25Mg, 28Al, 29Si, 57Fe, 208Pb deduced resonances, Γn, L, J, π, Γγ. Moxon-Rae detectors, Monte-Carlo analysis.

doi: 10.1088/0305-4616/6/9/013
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30663.


1980CO22      Nucl.Instrum.Methods 178, 481 (1980)

D.D.Cohen

A Radially Dependent Photopeak Efficiency Model for Si(Li) Detectors

RADIOACTIVITY 54Mn(EC); 241Am(α); measured X-ray spectra; deduced Si(Li) detector efficiency, calibration related features.

doi: 10.1016/0029-554X(80)90828-9
Citations: PlumX Metrics


1979AL20      Aust.J.Phys. 32, 447 (1979)

B.J.Allen, D.D.Cohen

keV Neutron Capture Cross Section of 170Yb

NUCLEAR REACTIONS 170Yb(n, γ), E=10-70 keV; measured σ; deduced S-process parameter.

doi: 10.1071/PH790447
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30543.


1974ME18      Nucl.Phys. A224, 429 (1974)

R.D.Meeker, G.M.Kalvius, B.D.Dunlap, S.L.Ruby, D.Cohen

Hyperfine Interactions and Nuclear Moments in Even Uranium Isotopes from Mossbauer Spectroscopy

NUCLEAR REACTIONS 234,236,238U(γ, γ'); measured hyperfine splitting, Mossbauer effect. 234,236,238U levels deduced μ, quadrupole moment ratios.

doi: 10.1016/0375-9474(74)90547-8
Citations: PlumX Metrics


1972UN01      Nucl.Phys. A191, 233 (1972)

J.P.Unik, E.P.Horwitz, K.L.Wolf, I.Ahmad, S.Fried, D.Cohen, P.R.Fields, C.A.A.Bloomquist, D.J.Henderson

Production of Actinides and the Search for Super-Heavy Elements Using Secondary Reactions Induced by GeV Protons

NUCLEAR REACTIONS W(p, X), E=28 GeV; 238U(p, X), E=12, 28 GeV; measured yields, cross sections, actinides, upper limits for transactinides.

doi: 10.1016/0375-9474(72)90513-1
Citations: PlumX Metrics


1969KA17      Phys.Letters 29B, 489 (1969)

G.M.Kalvius, S.L.Ruby, B.D.Dunlap, G.K.Shenoy, D.Cohen, M.B.Brodsky

Mossbauer Isomer Shift in 243Am

NUCLEAR REACTIONS 243Am(γ, γ), E=84 keV; measured Mossbauer effect. 243Am deduced isomer shift.

doi: 10.1016/0370-2693(69)90030-6
Citations: PlumX Metrics


1969RU05      Phys.Rev. 184, 374 (1969)

S.L.Ruby, G.M.Kalvius, B.D.Dunlap, G.K.Shenoy, D.Cohen, M.B.Brodsky, D.J.Lam

Nuclear Gamma-Ray Resonance Study of Hyperfine Interactions in 238U

NUCLEAR REACTIONS 238U(γ, γ), E = 44.7 keV; measured Mossbauer effect; deduced hyperfine parameters. 238U level deduced μ.

doi: 10.1103/PhysRev.184.374
Citations: PlumX Metrics


1968DU02      Phys.Rev. 171, 316(1968)

B.D.Dunlap, G.M.Kalvius, S.L.Ruby, M.B.Brodsky, D.Cohen

Isomer Shift and Hyperfine Splittings of the 59.6-keV Mossbauer Resonance in 237Np

NUCLEAR REACTIONS 237Np(γ, γ), E=59.6 keV; measured Mossbauer effect. 237Np deduced μ, quadrupole moment, isomer shift. 241Am source in Am, Th, Cu. NpO2, NpAl2 absorbers.

doi: 10.1103/PhysRev.171.316
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1959CO93      J.Inorg.Nucl.Chem. 11, 159 (1959)

D.Cohen, J.C.Sullivan, A.J.Zielen

Half-Life of 239Np

doi: 10.1016/0022-1902(59)80060-9
Citations: PlumX Metrics


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Note: The following list of authors and aliases matches the search parameter D.Cohen: , D.D.COHEN