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NSR database version of April 11, 2024.

Search: Author = R.A.Blue

Found 33 matches.

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1988TA18      Phys.Rev. C38, 1247 (1988)

H.Takai, C.N.Knott, D.F.Winchell, J.X.Saladin, M.S.Kaplan, L.de Faro, R.Aryaeinejad, R.A.Blue, R.M.Ronningen, D.J.Morrissey, I.Y.Lee, O.Dietzsch

Population of High Spin States by Quasi-Elastic and Deep Inelastic Collisions

NUCLEAR REACTIONS 170Er(22Ne, X), E=10 MeV/nucleon; measured fragment kinetic energy for X=Mg-B, relative yield, γ(fragment)-, γγ-coin. 166,168,170,172Yb, 170,172Hf deduced transition relative Iγ vs J.

doi: 10.1103/PhysRevC.38.1247
Citations: PlumX Metrics


1986BL12      Phys.Rev. C34, 850 (1986)

C.Bloch, W.Benenson, E.Kashy, D.J.Morrissey, R.A.Blue, R.M.Ronningen, H.Utsunomiya

Effect of 8Be Decay on Nuclear Temperature Measurements

NUCLEAR REACTIONS Ag(14N, X)6Li/7Li/7Be/9Be/10Be/10B/11B, E=280, 350, 490 MeV; measured inclusive residual fragment spectra, 7Li, 8Be yields relative to 6Li, γ-multiplicity; deduced nuclear temperatures.

doi: 10.1103/PhysRevC.34.850
Citations: PlumX Metrics


1986MO13      Phys.Rev. C34, 761 (1986)

D.J.Morrissey, C.Bloch, W.Benenson, E.Kashy, R.A.Blue, R.M.Ronningen, R.Aryaeinejad

Thermal Population of Nuclear Excited States

NUCLEAR REACTIONS 12C(14N, X)7Be/10B, E=6.25-25 MeV/nucelon; measured σ(fragment θ), (fragment)γ-coin, Eγ, Iγ, γ-multiplicity. 7Be, 10B deduced bound state population. 26Al deduced equilibrium characteristics.

doi: 10.1103/PhysRevC.34.761
Citations: PlumX Metrics


1986UT01      Phys.Rev. C33, 185 (1986)

H.Utsunomiya, E.C.Deci, R.A.Blue, L.H.Harwood, R.M.Ronningen, K.Siwek-Wilczynska, J.Wilczynski, D.J.Morrissey

Few-Nucleon Transfer in Quasi-Elastic Collisions at 20 MeV/Nucleon

NUCLEAR REACTIONS 164Dy(14N, 15N), (14N, 13N), (14N, 12B), (14N, 11B), (14N, 10B), (14N, xn), (14N, xnα), 165Ho(14N, 11C), (14N, 12C), (14N, 13C), E=20 MeV/nucleon; measured inclusive fragment spectra, (particle)γ-coin; deduced reaction mechanism.

doi: 10.1103/PhysRevC.33.185
Citations: PlumX Metrics


1985MO17      Phys.Rev. C32, 877 (1985)

D.J.Morrissey, W.Benenson, E.Kashy, C.Bloch, M.Lowe, R.A.Blue, R.M.Ronningen, B.Sherrill, H.Utsunomiya, I.Kelson

Nuclear Temperatures in the Reactions of 14N with Ag at 35 MeV/nucleon

NUCLEAR REACTIONS Ag(14N, X), E=490 MeV; measured particle spectra for X=6,7,8Li, 7,9,10Be, yield vs Q, γ-multiplicity, (particle)γ-coin. 6,7,8Li, 7Be levels deduced effective nuclear temperatures.

doi: 10.1103/PhysRevC.32.877
Citations: PlumX Metrics


1985MO24      Nucl.Phys. A447, 603c (1985)

D.J.Morrissey, W.Benenson, E.Kashy, C.Bloch, M.Lowe, B.Sherrill, R.A.Blue, R.M.Ronningen, H.Utsunomiya

Results from a New Temperature Measurement in Nuclear Reactions

NUCLEAR REACTIONS 12C(14N, X), E=8 MeV/nucleon; measured inclusive fragment spectra for X=Li, Be, B. 7Li, 7Be deduced excited state population fraction. Ag(14N, X), E=490 MeV; measured inclusive fragment spectra for X=Li, Be; deduced temperature for 6,8Li, 7Be fragments.

doi: 10.1016/0375-9474(86)90636-6
Citations: PlumX Metrics


1985SI19      Phys.Rev. C32, 1450 (1985)

K.Siwek-Wilczynska, R.A.Blue, L.H.Harwood, R.M.Ronningen, H.Utsunomiya, J.Wilczynski, D.J.Morrissey

Detection of Heavy-Ion Reaction Products in Bound Excited States

NUCLEAR REACTIONS 164Dy(14N, X), E=280 MeV; measured (fragment)γ-coin, X=11B, 12,14C, 15N, 15,16O; deduced population of excited states in transfer reactions. Bismuth germanate detectors.

doi: 10.1103/PhysRevC.32.1450
Citations: PlumX Metrics


1984MO29      Phys.Lett. 148B, 423 (1984)

D.J.Morrissey, W.Benenson, E.Kashy, B.Sherrill, A.D.Panagiotou, R.A.Blue, R.M.Ronningen, J.van der Plicht, H.Utsunomiya

Excited State Production and Temperature Measurement in a Heavy Ion Reaction

NUCLEAR REACTIONS Ag(14N, X), E=490 MeV; measured fragment spectra for X=6,7Li, 7Be; deduced fragment excited state population, effective temperature inconsistency.

doi: 10.1016/0370-2693(84)90730-5
Citations: PlumX Metrics


1979SK04      Phys.Rev. C20, 409 (1979)

D.M.Skopik, J.J.Murphy II, H.R.Weller, R.A.Blue, N.R.Roberson, S.A.Wender, D.R.Tilley

Reactions 15N(γ, d0)13C and 13C(d, γ0)15N in the Giant Resonance Region

NUCLEAR REACTIONS 15N(e, e'd), E not given; measured σ(θ); deduced σ(γ, d). 13C(polarized d, γ), E=6.74 MeV; measured σ(θ), A(θ). 15N deduced E1 matrix elements, T-character, phases around 22-MeV excitation.

doi: 10.1103/PhysRevC.20.409
Citations: PlumX Metrics


1978WE02      Phys.Rev. C17, 1260 (1978)

H.R.Weller, R.A.Blue, P.L.Von Behren, N.R.Roberson, C.R.Gould, D.R.Tilley, S.A.Wender

Angular Distribution Measurements for Radiative Capture of Fast Neutrons by 40Ca

NUCLEAR REACTIONS 40Ca(n, γ), E=8.0, 12.0 MeV; measured σ(θ). DSD calculations.

doi: 10.1103/PhysRevC.17.1260
Citations: PlumX Metrics


1976CA22      Phys.Rev. C14, 553 (1976)

C.P.Cameron, N.R.Roberson, D.G.Rickel, R.D.Ledford, H.R.Weller, R.A.Blue, D.R.Tilley

Giant Dipole Resonances in 55,57,59Co Using Polarized Proton Capture

NUCLEAR REACTIONS 54,56,58Fe(polarized p, γ), E=8-15 MeV; measured σ(E, θ), A(E, θ). 58Fe(p, γ), E=5-16 MeV; measured σ. 55,57,59Co GDR deduced isospin splitting.

doi: 10.1103/PhysRevC.14.553
Citations: PlumX Metrics


1976WE01      Phys.Rev. C13, 38 (1976)

H.R.Weller, R.A.Blue, S.E.Darden, W.A.Yoh

14C(d, t)13C Reaction-Cross-Section and Analyzing-Power Measurements at 14 MeV

NUCLEAR REACTIONS 14C(polarized d, t), E=14 MeV; measured σ(E, θ), polarization parameters A(Et, θ). 13C levels deduced S. Enriched targets.

doi: 10.1103/PhysRevC.13.38
Citations: PlumX Metrics


1976WE07      Phys.Rev. C13, 922 (1976)

H.R.Weller, R.A.Blue, N.R.Roberson, D.G.Rickel, S.Maripuu, C.P.Cameron, R.D.Ledford, D.R.Tilley

Giant Resonance Region of 15N Studied by Polarized and Unpolarized Proton Capture Measurements

NUCLEAR REACTIONS 14C(polarized p, γ), E=4.0-16.2 MeV; measured σ(E, Eγ, θ), A(E, θ). 15N deduced E1, E2 strength, T-matrix amplitudes, phases.

doi: 10.1103/PhysRevC.13.922
Citations: PlumX Metrics


1975GO31      Phys.Rev. C12, 1730 (1975)

J.D.Goss, P.L.Jolivette, C.P.Browne, S.E.Darden, H.R.Weller, R.A.Blue

Angular Distribution Measurements for 14C(d, p)15C and the Level Structure of 15C

NUCLEAR REACTIONS 14C(d, p), E=14 MeV; measured σ(Ep, θ). 14C(polarized d, d), (polarized d, p), E=14 MeV; measured iT11(θ). 15C levels deduced J, π, S.

doi: 10.1103/PhysRevC.12.1730
Citations: PlumX Metrics


1975WE09      Phys.Rev. C11, 1464 (1975)

H.R.Weller, R.A.Blue, J.J.Ramirez, E.M.Bernstein

14C(p, α)11B Reaction for 4 MeV < E < 7.5 MeV

NUCLEAR REACTIONS 14C(p, α), E=4-7.5 MeV; measured σ(E, Eα, θ). 15N levels deduced J, π.

doi: 10.1103/PhysRevC.11.1464
Citations: PlumX Metrics


1974WE06      Phys.Rev. C10, 575 (1974)

H.R.Weller, R.A.Blue, J.J.Ramirez, E.M.Bernstein, H.R.Hiddleston, R.M.Prior, S.E.Darden, M.Divadeenam

2p-1h Structure of 15N from 14C(p, p)14C Cross Section and Polarization Measurements

NUCLEAR REACTIONS 14C(p, p), E=4-11.5 MeV; measured σ(θ), P(θ). 15N levels deduced J, π, p-width, level-width.

doi: 10.1103/PhysRevC.10.575
Citations: PlumX Metrics


1973GO28      Phys.Rev.C8, 514 (1973)

J.D.Goss, A.A.Rollefson, C.P.Browne, R.A.Blue, H.R.Weller

15C States via the 14C(d, p)15C Reactions

NUCLEAR REACTIONS 14C(d, p), E=12.0, 13.0, 14.012 MeV; measured σ(Ep). 15C deduced levels, level-width.

doi: 10.1103/PhysRevC.8.514
Citations: PlumX Metrics


1973WE04      Nucl.Phys. A207, 177 (1973)

H.R.Weller, R.A.Blue, J.J.Ramirez, E.M.Bernstein

The 14C(p, γ0)15N Cross Section below E = 12 MeV

NUCLEAR REACTIONS 14C(p, γ0), E=7.7-12.0 MeV; measured σ(E;θ). 15N deduced levels, J, π. Enriched target.

doi: 10.1016/0375-9474(73)90029-8
Citations: PlumX Metrics


1973WE12      Nucl.Phys. A211, 221 (1973)

H.R.Weller, R.A.Blue

The 13C(d, γ0)15N and the 11B(d, γ0)13C Cross Sections in the Region Of the Giant Dipole Resonance

NUCLEAR REACTIONS 13C(d, γ0), 11B(d, γ0), E=1-4 MeV; measured σ(E, θ). 15N, 13C deduced resonances. Enriched targets.

doi: 10.1016/0375-9474(73)90715-X
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0384.


1972BL04      Nucl.Phys. A184, 377 (1972)

R.A.Blue, K.J.Stout, G.Marr

Polarization of Protons from the 12C(d, p)13C Reaction

NUCLEAR REACTIONS 12C(d, p)13C, E=4-6 MeV; measured proton polarization P(E;θ).

doi: 10.1016/0375-9474(72)90415-0
Citations: PlumX Metrics


1972KE08      Nucl.Phys. A186, 528 (1972)

R.M.Keyser, R.A.Blue, H.R.Weller

A Study of 17O via 3He Bombardment of 14C

NUCLEAR REACTIONS 14C(3He, α), (3He, d), (3He, p), (3He, 3He), E=2.2-7.0 MeV; measured σ(E;Eα, θ). 17O deduced levels, J, π. Enriched target.

doi: 10.1016/0375-9474(72)90982-7
Citations: PlumX Metrics


1972MO39      Nucl.Phys. A197, 290 (1972)

T.Mo, R.A.Blue, H.R.Weller

A Study of 17F Above 19 MeV from 3He Bombardment of 14N

NUCLEAR REACTIONS 14N(3He, α), 14N(3He, 3He), 14N(3He, γ), E=3.5-7.0 MeV; measured σ(θ, E). 17F deduced levels, J, π, level-width. Natural targets.

doi: 10.1016/0375-9474(72)90763-4
Citations: PlumX Metrics


1972RA03      Phys.Rev. C5, 17 (1972)

J.J.Ramirez, R.A.Blue, H.R.Weller

Multilevel Multichannel Study of the Structure of 15N from 12- to 14-MeV Excitation Energy

NUCLEAR REACTIONS 14C(p, p), (p, α), (p, n), (p, γ), 11B(α, α), E=2-4 MeV; measured σ(E;θ). 15N deduced resonances, levels, level-width, J, π, isobaric analog.

doi: 10.1103/PhysRevC.5.17
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0090.


1972WE04      Phys.Rev. C5, 648 (1972)

H.R.Weller, R.A.Blue, S.L.Blatt

Energy of the 14N(d, γ0)16O Resonance in the Giant-Dipole Region of 16O

NUCLEAR REACTIONS 14N(d, γ), E=1.8-3 MeV; measured σ(E). 16O deduced resonance.

doi: 10.1103/PhysRevC.5.648
Citations: PlumX Metrics


1972WE07      Nucl.Phys. A185, 284 (1972)

H.R.Weller, R.A.Blue, E.M.Bernstein, J.J.Ramirez

The 14C(p, γ0)15N Cross Section from E = 3.2 to 7.7 MeV

NUCLEAR REACTIONS 14C(p, γ0), E=3.2 to 7.7 MeV; measured σ(E, θ). 15N deduced levels, J, π. Enriched target.

doi: 10.1016/0375-9474(72)90570-2
Citations: PlumX Metrics


1971KE08      Phys.Lett. 34B, 602 (1971)

R.M.Keyser, R.A.Blue, H.R.Weller

The 21.7 and 22.1 MeV States in 17O

NUCLEAR REACTIONS 14C(3He, α), E=2-6 MeV; measured σ(E;θ). 17O deduced resonances, J, π, level-width.

doi: 10.1016/0370-2693(71)90149-3
Citations: PlumX Metrics


1970RA22      Phys.Lett. 32B, 361 (1970)

J.J.Ramirez, H.R.Weller, R.A.Blue

Observation of the 13.42 MeV T = 3/2 State in 15N

NUCLEAR REACTIONS 14C(p, p), (p, α), (p, n), (p, γ), E=2-4 MeV; measured σ(E). 15N resonance deduced J, π, isobaric analog.

doi: 10.1016/0370-2693(70)90497-1
Citations: PlumX Metrics


1967BL02      Nucl.Phys. A90, 601(1967)

R.A.Blue, K.J.Stout, G.Marr

Polarization of Protons from the 9Be(d, p)10Be Reaction

NUCLEAR REACTIONS 9Be(d, p), E = 1-6 MeV; measured polarization (Ep, θ).

doi: 10.1016/0375-9474(67)90066-8
Citations: PlumX Metrics


1965BL02      Phys.Rev. 137, B284 (1965)

R.A.Blue, W.Haeberli

Polarization of Protons Elastically Scattered by Oxygen

NUCLEAR STRUCTURE 16O; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.137.B284
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0492.


1964SI04      Bull.Am.Phys.Soc. 9, No.1, 68, GC7 (1964)

E.A.Silverstein, L.D.Oppliger, R.A.Blue

Level Parameters of 3.86-MeV State in F17

NUCLEAR STRUCTURE 16O; measured not abstracted; deduced nuclear properties.


1963BL06      Bull.Am.Phys.Soc. 8, No.4, 317, G3 (1963)

R.A.Blue, L.E.Porter, W.Haeberli

Polarization of Protons Scattered by Oxygen

NUCLEAR STRUCTURE O; measured not abstracted; deduced nuclear properties.


1962BL15      Bull.Am.Phys.Soc. 7, No.7, 434, BA6 (1962)

R.A.Blue, R.I.Brown, L.W.Morrow, W.G.Weitkamp, L.C.McIntyre

Polarization of Protons Scattered by Oxygen

NUCLEAR STRUCTURE O; measured not abstracted; deduced nuclear properties.


1962LU01      Bull.Am.Phys.Soc. 7, No.4, 268, CB5 (1962)

R.A.Lux, R.A.Blue, W.Haeberli

NUCLEAR STRUCTURE 7Li; measured not abstracted; deduced nuclear properties.


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