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NSR database version of April 26, 2024.

Search: Author = R.R.Spencer

Found 37 matches.

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2002GU17      Phys.Rev. C65, 058801 (2002)

K.H.Guber, R.O.Sayer, T.E.Valentine, L.C.Leal, R.R.Spencer, J.A.Harvey, P.E.Koehler, T.Rauscher

New Maxwellian Averaged Neutron Capture Cross Sections for 35, 37Cl

NUCLEAR REACTIONS 35,37Cl(n, γ), (n, X), E=0.1-600 keV; measured capture and total σ; deduced parameters, Maxwellian averaged σ, astrophysical reaction rates.

doi: 10.1103/PhysRevC.65.058801
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14090.


2001GU26      Nucl.Sci.Eng. 139, 111 (2001)

K.H.Guber, R.R.Spencer, L.C.Leal, P.E.Koehler, J.A.Harvey, R.O.Sayer, H.Derrien, T.E.Valentine, D.E.Pierce, V.M.Cauley, T.A.Lewis

High-Resolution Transmission Measurements of 233U using a Cooled Sample at the Temperature T = 11 K

NUCLEAR REACTIONS 233U(n, X), E < 300 keV; measured total σ. High-resolution transmission spectra, comparisons with previous results.

doi: 10.13182/NSE01-A2226
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13891.


2001KO76      Phys.Rev. C64, 065802 (2001)

P.E.Koehler, J.A.Harvey, R.R.Winters, K.H.Guber, R.R.Spencer

High-Resolution Neutron Capture and Transmission Measurements for 116, 120Sn, and Their Stellar Neutron-Capture Cross Sections at s-Process Temperatures

NUCLEAR REACTIONS 116,120Sn(n, γ), (n, X), E=0.05-500 keV; measured total and capture σ; deduced resonance parameters, astrophysical reaction rates. Comparison with previous results.

doi: 10.1103/PhysRevC.64.065802
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13909.


2000GU18      Nucl.Sci.Eng. 135, 141 (2000)

K.H.Guber, R.R.Spencer, L.C.Leal, J.A.Harvey, N.W.Hill, G.Dos Santos, R.O.Sayer, D.C.Larson

New High-Resolution Fission Cross-Section Measurements of 233U in the 0.4-eV to 700-keV Energy Range

NUCLEAR REACTIONS 233U(n, F), E < 700 keV; measured fission σ. High-resolution measurement, comparisons with previous data.

doi: 10.13182/NSE00-A2130
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13890.


2000KO58      Phys.Rev. C62, 055803 (2000); Erratum Phys.Rev. C63, 049901 (2001)

P.E.Koehler, R.R.Winters, K.H.Guber, T.Rauscher, J.A.Harvey, S.Raman, R.R.Spencer, J.C.Blackmon, D.C.Larson, D.W.Bardayan, T.A.Lewis

High-Resolution Neutron Capture and Transmission Measurements, and the Stellar Neutron-Capture Cross Section of 88Sr

NUCLEAR REACTIONS 88Sr(n, γ), (n, X), E=0.1-950 keV; measured Eγ, Iγ, capture and total σ; deduced resonance parameters, astrophysical reaction rates. R-matrix analysis, comparisons with previous results.

doi: 10.1103/PhysRevC.62.055803
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13742.


1998KO07      Phys.Rev. C57, R1558 (1998)

P.E.Koehler, R.R.Spencer, K.H.Guber, R.R.Winters, S.Raman, J.A.Harvey N.W.Hill, J.C.Blackmon, D.W.Bardayan, D.C.Larson, T.A.Lewis, D.E.Pierce, M.S.Smith

High Resolution Neutron Capture and Transmission Measurements on 137Ba and Their Impact on the Interpretation of Meteoric Barium Anomalies

NUCLEAR REACTIONS 137Ba(n, γ), E=20 eV-500 keV; measured capture σ(E); deduced astrophysical reaction rates. Comparison with meteorite isotopic abundances.

doi: 10.1103/PhysRevC.57.R1558
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13695.


1997GU04      Phys.Rev.Lett. 78, 2704 (1997)

K.H.Guber, R.R.Spencer, P.E.Koehler, R.R.Winters

New 142,144Nd(n, γ) Cross Sections and the s-Process Origin of the Nd Anomalies in Presolar Meteoric Silicon Carbide Grains

NUCLEAR REACTIONS 142,144Nd(n, γ), E=5-50 keV; measured Maxwellian averaged σ; deduced s-process nucleosyntheis related features in the Ce-Nd-Sm region.

doi: 10.1103/PhysRevLett.78.2704
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13647.


1997GU15      Nucl.Phys. A621, 254c (1997)

K.H.Guber, R.R.Spencer, P.E.Koehler, R.R.Winters

A BaF2 Detector System for (n, γ) Cross Section Measurements at ORELA

NUCLEAR REACTIONS 142Nd(n, γ), E=2-3 keV; measured neutron tof vs Eγ, multiplicity. 144Nd, 197Au(n, γ), E=1-2 keV; measured tof spectra; deduced detector characteristics. 4π BaF2 detector array.

doi: 10.1016/S0375-9474(97)00249-2
Citations: PlumX Metrics


1997GU16      Nucl.Phys. A621, 266c (1997)

K.H.Guber, R.R.Spencer, P.E.Koehler, R.R.Winters

Measurements of 142,144Nd(n, γ) Cross Sections at ORELA for Astrophysical s-Process Studies

NUCLEAR REACTIONS 142,144Nd(n, γ), E < 200 keV; measured σ; deduced reaction rates. Astrophysical s-process implications.

doi: 10.1016/S0375-9474(97)00252-2
Citations: PlumX Metrics


1997KO35      Nucl.Phys. A621, 258c (1997)

P.E.Koehler, R.R.Spencer, R.R.Winters, K.H.Guber, J.A.Harvey, N.W.Hill, M.S.Smith

New Neutron Capture and Transmission Measurements for 134,136Ba at ORELA and Their Impact on s-Process Nucleosynthesis Calculations

NUCLEAR REACTIONS 134,136Ba(n, γ), E < 500 keV; measured σ; deduced reaction rates. Other data compared, astrophysical s-process implications.

doi: 10.1016/S0375-9474(97)00250-9
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13729.


1996KO27      Phys.Rev. C54, 1463 (1996)

P.E.Koehler, R.R.Spencer, R.R.Winters, K.H.Guber, J.A.Harvey, N.W.Hill, M.S.Smith

Resonance Neutron Capture and Transmission Measurements and the Stellar Neutron Capture Cross Sections of 134Ba and 136Ba

NUCLEAR REACTIONS 134,136Ba(n, γ), (n, X), E=20 eV-500 keV; measured capture σ(E), transmission; deduced σ vs E; calculated astrophysical reaction rates. 135,137Ba levels deduced l, J, π, Γn, Γγ, (gΓnΓγ)/Γ. Enriched targets. R-matrix analysis.

doi: 10.1103/PhysRevC.54.1463
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13729.


1987SP07      Nucl.Sci.Eng. 96, 318 (1987)

R.R.Spencer, J.A.Harvey, N.W.Hill, L.W.Weston

Parameters of the 1.056-eV Resonance in 240Pu and the 2200 m/s Neutron Total Cross Sections of 235U, 239Pu, and 240Pu

NUCLEAR REACTIONS 240Pu(n, X), E ≈ 1 eV; measured transmission ratios. 241Pu deduced resonance parameters Γγ, Γn. 235U, 239,240Pu(n, X), E=thermal; measured transmission; deduced total σ. Tof, 6Li glass scintillator.

doi: 10.13182/NSE87-A16395
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset12941.


1986GW01      Radiat.Eff. 93, 253 (1986)

R.Gwin, R.R.Spencer, R.W.Ingle

Measurement of the Energy Dependence of Prompt Fission Neutron Emission from 233U, 235U, and 239Pu for E = 0.0005 to 10 MeV Relative to Emission from Spontaneous Fission of 252Cf

NUCLEAR REACTIONS 233,235U, 239Pu(n, F), E=0.0005-10 MeV; measured per fission prompt neutron average number. Fissile sample, 252Cf standard enclosed in large volume liquid scintillator loaded with Gd.

doi: 10.1080/00337578608207465
Citations: PlumX Metrics


1986GW02      Nucl.Sci.Eng. 94, 365 (1986)

R.Gwin, R.R.Spencer, R.W.Ingle

Measurements of the Energy Dependence of Prompt Neutron Emission from 233U, 235U, and 239Pu for E(n) = 0.0005 to 10 MeV Relative to Emission from Spontaneous Fission of 252Cf

RADIOACTIVITY 252Cf(SF); measured prompt neutron emission vs E; deduced ν-bar(E) ratio relative to 233,235U, 239Pu(n, F) reaction.

NUCLEAR REACTIONS 233,235U, 239Pu(n, F), E=0.0005-10 MeV; measured prompt neutron emission vs E following fission; deduced model parameters, ν-bar(E) ratio relative to 252Cf(SF). Liquid scintillator loaded with Gd, 252Cf standard.

doi: 10.13182/NSE86-A18347
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13101.


1986SP03      Radiat.Eff. 93, 245 (1986)

R.R.Spencer, J.A.Harvey, N.W.Hill, L.W.Weston

Neutron Total Cross Section of 240Pu below 6 eV and the Parameters of the 1.056-eV Resonance

NUCLEAR REACTIONS 240Pu(n, X), E ≤ 6 eV; measured transmission. 241Pu resonance deduced Γn, Γγ, ΓnΓγ.

doi: 10.1080/00337578608207463
Citations: PlumX Metrics


1984GW01      Nucl.Sci.Eng. 88, 37 (1984)

R.Gwin, R.R.Spencer, R.W.Ingle, J.H.Todd, S.W.Scoles

Measurements of the Neutron Fission Cross Sections of 235U(E(n) = 0.01 eV to 30 keV) and 239Pu(E(n) = 0.01 to 60 eV)

NUCLEAR REACTIONS 235U(n, F), E=0.00001-30 keV; 239Pu(n, F), E=0.01-60 eV; measured fission σ(E).

doi: 10.13182/NSE84-A17138
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset12905.


1984GW02      Nucl.Sci.Eng. 87, 381 (1984)

R.Gwin, R.R.Spencer, R.W.Ingle

Measurements of the Energy Dependence of Prompt Neutron Emission from 233U, 235U, 239Pu, and 241Pu for E(n) = 0.005 to 10 eV Relative to Emission from Spontaneous Fission of 252Cf

NUCLEAR REACTIONS 233,235U, 239,241Pu(n, F), E=0.005-10 eV; measured prompt neutron energy dependence following fission; deduced average prompt neutron number ratio relative to 252Cf(SF) decay.

doi: 10.13182/NSE84-A18506
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset12833.


1982SP04      Nucl.Sci.Eng. 80, 603 (1982)

R.R.Spencer, R.Gwin, R.Ingle

A Measurement of the Average Number of Prompt Neutrons from Spontaneous Fission of Californium-252

RADIOACTIVITY, Fission 252Cf(SF); measured prompt neutron number. Liquid scintillator detector, high precision.

doi: 10.13182/NSE82-A18973
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset10954.


1979BE18      Nucl.Sci.Eng. 70, 98 (1979)

H.Beer, R.R.Spencer

The Total Neutron Cross Section of Boron-10 between 90 and 420 keV

NUCLEAR REACTIONS 10B(n, X), E=90-420 keV; measured σ(E). 11B deduced S-wave resonance. R-matrix analysis. Thick target.

doi: 10.13182/NSE79-A18932
Citations: PlumX Metrics


1978BE04      Z.Phys. A284, 173 (1978)

H.Beer, R.R.Spencer, F.Kappeler

Measurement of Partial Radiation Widths of High Energy Transitions from keV Capture Resonances in 56Fe and 58,60Ni

NUCLEAR REACTIONS 56Fe, 58,60Ni(n, γ), E=7-70 keV; measured σ(Eγ). 57Fe, 59,61Ni deduced resonances, partial radiation Γ, M1 strength.

doi: 10.1007/BF01411325
Citations: PlumX Metrics


1976SP13      Nucl.Sci.Eng. 61, 346 (1976)

R.R.Spencer, R.L.Macklin

Neutron Capture Cross Section of Cobalt-59 in the Energy Range 2.5 to 1000 keV

NUCLEAR REACTIONS 59Co(n, γ), E ≤ 1 MeV; measured σ(E). 60Co deduced resonances, Γγ.

doi: 10.13182/NSE76-A26920
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset10543.


1976SP14      Nucl.Sci.Eng. 60, 390 (1976)

R.R.Spencer, H.Beer

Measurement of Neutron Radiative Capture in Cobalt-59

NUCLEAR REACTIONS 59Co(n, γ), E=6-200 keV; measured σ(E, Eγ). 60Co deduced resonances, Γn, Γγ.

doi: 10.13182/NSE76-A26900
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset20555.


1975BE07      Nucl.Phys. A240, 29 (1975)

H.Beer, R.R.Spencer

keV Neutron Radiative Capture and Total Cross Section of 50,52,53Cr, 54,57Fe, and 62,64Ni

NUCLEAR REACTIONS 50,52,53Cr, 54,57Fe, 62,64Ni(n, γ), E=5-200 keV; 50,52Cr, 54Fe, 62,64Ni(n, t), E=10-300 keV; measured σ(E, Eγ), σ(E, Et). 51,53,54Cr, 55,58Fe, 63,65Ni deduced resonances, J, L, n-width, γ-width. Enriched targets.

doi: 10.1016/0375-9474(75)90435-2
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset20374.


1974BE81      Astron.Astrophys. 37, 197 (1974)

H.Beer, R.R.Spencer, A.Ernst

The s-Process near the Iron Seed - Some Improved Capture Cross Sections

NUCLEAR REACTIONS 50,52,53Cr, 54,56,57Fe, 59Co, 58,60,61,62,64Ni(n, γ), E=5-75 keV; measured reaction products, Eγ, Iγ; deduced σ, Maxwellian-averaged σ, 62Ni neutron resonance parameters.

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset20374.


1969FA01      Nucl.Phys. A123, 616 (1969)

K.T.Faler, R.R.Spencer, R.A.Harlan

Excited States in 178Hf from Resonance Neutron-Capture Gamma-Ray Studies

NUCLEAR REACTIONS 177Hf(n, γ), E=0.06-8.8 eV; measured Eγ, γγ-coin, resonance capture; deduced Q. 178Hf deduced levels. Enriched target, Ge(Li) detector.

doi: 10.1016/0375-9474(69)91009-4
Citations: PlumX Metrics


1968FA07      Phys.Rev. 175, 1495 (1968)

K.T.Faler, R.R.Spencer, R.A.Harlan

A Kπ = 0+ Band in 184W

NUCLEAR STRUCTURE 184W; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.175.1495
Citations: PlumX Metrics


1967SP03      Phys.Rev. 155, 1368 (1967)

R.R.Spencer, K.T.Faler

Neutron-Capture Gamma-Ray Studies in Isotopes of Tungsten

NUCLEAR STRUCTURE 187W, 184W, 183W; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.155.1368
Citations: PlumX Metrics


1966FA11      Bull.Am.Phys.Soc. 11, No.3, 336, DB14 (1966)

K.T.Faler, R.R.Spencer, D.R.Dixon

Thermal and Resonance Neutron-Capture Gamma Rays in W-184

NUCLEAR STRUCTURE 184W; measured not abstracted; deduced nuclear properties.


1960SP08      Nuclear Phys. 21, 310 (1960)

R.R.Spencer, G.C.Phillips, T.E.Young

Energy Levels of Be9 and B9

NUCLEAR STRUCTURE 9B, 9Be; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(60)90056-0
Citations: PlumX Metrics


1959RA01      Bull.Am.Phys.Soc. 4, No.2, 96, C9 (1959)

D.A.A.S.N.Rao, T.E.Young, R.R.Spencer, E.H.Beckner, G.C.Phillips

Excited States in F18 from O16(He3, p)F18


1959SP17      Bull.Am.Phys.Soc. 4, No.2, 95, C4 (1959); Oral Report

R.R.Spencer, G.C.Phillips

Low Excited States in Be9 and B9


1959YO19      Phys.Rev.Letters 3, 535 (1959)

T.E.Young, G.C.Phillips, R.R.Spencer

Nuclear Energy Levels in C13, N13, N14, N15, O15, and F18 from He3-Induced Reactions

doi: 10.1103/PhysRevLett.3.535
Citations: PlumX Metrics


1959YO25      Phys.Rev. 116, 962 (1959)

T.E.Young, G.C.Phillips, R.R.Spencer, D.A.A.S.N.Rao

Nuclear Energy Levels in C13, N13, N14, N15, O15, and F18 from He3 Induced Reactions

doi: 10.1103/PhysRev.116.962
Citations: PlumX Metrics


1957DA10      Bull.Am.Phys.Soc. 2, No.6, 304, E9 (1957)

R.H.Davis, F.W.Prosser, Jr., R.R.Spencer, T.E.Young, J.H.Johnson

Elastic Scattering of Protons from Ca Observed at 180°


1957SP90      Phys.Rev. 108, 69 (1957)

R.R.Spencer, G.C.Phillips, T.E.Young

Inelastic Scattering of Protons from Cu65, Ni58, Ni60, and Ni62

doi: 10.1103/PhysRev.108.69
Citations: PlumX Metrics


1957YO01      Bull.Am.Phys.Soc. 2, No.2, 104, J6 (1957)

T.E.Young, G.C.Phillips, R.R.Spencer

Energy Levels in O16, F19, and Cu65


1957YO04      Phys.Rev. 108, 72 (1957)

T.E.Young, G.C.Phillips, R.R.Spencer

Nuclear Energy Levels in O16, O18, and F19

doi: 10.1103/PhysRev.108.72
Citations: PlumX Metrics


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