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NSR database version of April 27, 2024.

Search: Author = J.N.Dyer

Found 9 matches.

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1980PI02      Phys.Rev. C21, 147 (1980)

R.Pitthan, G.M.Bates, J.S.Beachy, E.B.Dally, D.H.Dubois, J.N.Dyer, S.J.Kowalick, F.R.Buskirk

Comparison of Giant Multipole Resonances of Multipolarity E1 to E4 in 58Ni (T0 = 1) and 60Ni (T0 = 2) with Inelastic Electron Scattering

NUCLEAR REACTIONS 58,60Ni(e, e'), E=102 MeV; measured σ(E, θ). 58,60Ni deduced levels, giant resonance, Γ, B(λ), multipolarity.

doi: 10.1103/PhysRevC.21.147
Citations: PlumX Metrics


1979PI02      Phys.Rev. C19, 299 (1979)

R.Pitthan, F.R.Buskirk, J.N.Dyer, E.E.Hunter, G.Pozinsky

Distribution of E2 Strength in 28Si below 50 MeV Excitation Energy

NUCLEAR REACTIONS 28Si(e, e'), E=92 MeV; measured σ(Ee', θ). 28Si levels deduced multipolarity, B(λ), discussed sum rules.

doi: 10.1103/PhysRevC.19.299
Citations: PlumX Metrics


1979PI04      Phys.Rev. C19, 1251 (1979)

R.Pitthan, H.Hass, D.H.Meyer, F.R.Buskirk, J.N.Dyer

E0, E1, E2, E3, and E4 Giant Resonances in the N = 82 Nucleus 140Ce between 4 and 48 MeV Excitation Energy with Inelastic Electron Scattering

NUCLEAR REACTIONS 140Ce(e, e'), E=80, 92 MeV; measured σ(E, Ee', θ). 140Ce giant resonances deduced multipolarity, B(λ), Γγ, sum rules of giant resonances.

doi: 10.1103/PhysRevC.19.1251
Citations: PlumX Metrics


1978PI12      Phys.Rev.Lett. 41, 1276 (1978)

R.Pitthan, H.Hass, D.H.Meyer, J.N.Dyer, F.R.Buskirk

E1 Form Factor and the Existence of Breathing Mode at 80A-1/3 MeV In Heavy Nuclei

NUCLEAR REACTIONS 140Ce(e, e'), E=92.1 MeV; measured σ(θ).

doi: 10.1103/PhysRevLett.41.1276
Citations: PlumX Metrics


1976MO20      Z.Naturforsch. 31a, 668 (1976)

G.L.Moore, F.R.Buskirk, E.B.Dally, J.N.Dyer, X.K.Maruyama, R.Pitthan

The Widths of the E2 (ΔT = 0 and ΔT = 1) Giant Resonances in 165Ho

NUCLEAR REACTIONS 165Ho(e, e'), E=60-105 MeV; measured σ(E). 165Ho deduced giant resonances, Γ.


1974BU23      Z.Phys. 271, 69 (1974)

F.R.Buskirk, J.N.Dyer, X.K.Maruyama, K.E.Woehler

The Measured Energy Loss of High Energy Electrons in Various Metals

NUCLEAR REACTIONS Be, Sn, Gd(e, e), E=53, 75, 93 MeV; measured electron energy loss, half widths.

doi: 10.1007/BF01676374
Citations: PlumX Metrics


1974PI07      Phys.Rev.Lett. 33, 849 (1974); Erratum Phys.Rev.Lett. 34, 848 (1975)

R.Pitthan, F.R.Buskirk, E.B.Dally, J.N.Dyer, X.K.Maruyama

Electroexcitation of Giant Multipole Resonances in 197Au and 208Pb between 5 and 40 MeV Excitation Energy with 90-MeV Electrons

NUCLEAR REACTIONS 197Au, 208Pb(e, e'), E=90 MeV; measured σ(Ee', θ). 197Au, 208Pb deduced giant resonances, λ, B(λ), level-width.

doi: 10.1103/PhysRevLett.33.849
Citations: PlumX Metrics


1973BE60      Phys.Lett. 47B, 355 (1973)

R.W.Berard, F.R.Buskirk, E.B.Dally, J.N.Dyer, X.K.Maruyama, R.L.Topping, T.J.Traverso

Elastic Electron Deuteron Scattering

NUCLEAR REACTIONS 2H(e, e), E=105 MeV; measured σ(θ). 2H deduced rms radii.

doi: 10.1016/0370-2693(73)90622-9
Citations: PlumX Metrics


1972BU01      Phys.Rev. C5, 391 (1972)

F.A.Bumiller, F.R.Buskirk, J.N.Dyer, W.A.Monson

Elastic Electron Scattering from 6Li and 7Li at Low Momentum Transfer

NUCLEAR REACTIONS 6,7Li(e, e), E=23-97 MeV; measured σ(E). 6,7Li deduced rms nuclear radii.

doi: 10.1103/PhysRevC.5.391
Citations: PlumX Metrics


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