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Search: Author = J.A.Biggerstaff

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1987GO01 Phys.Rev. C35, 137 (1987)

J.Gomez del Campo, D.E.DiGregorio, J.A.Biggerstaff, Y.D.Chan, D.C.Hensley, P.H.Stelson, D.Shapira, M.E.Ortiz

Correlations between α Particles and Evaporation Residues for the ¹⁴N + ¹²C Reaction at E(¹⁴N) = 180 MeV

NUCLEAR REACTIONS ¹²C(¹⁴N, xα), E=180 MeV; measured α(evaporation residues)(θ); deduced equilibrium, nonequilibrium effects. ΔE-E solid state detectors.

doi: 10.1103/PhysRevC.35.137
Citations: PlumX Metrics

1984GO05 Phys.Rev. C29, 1722 (1984)

J.Gomez del Campo, J.A.Biggerstaff, R.A.Dayras, D.Shapira, A.H.Snell, P.H.Stelson, R.G.Stokstad

Comparison of Fusion Cross Sections for the ¹⁰B + ¹⁶O and ¹²C + ¹⁴N Systems

NUCLEAR REACTIONS, ICPND ¹²C(¹⁴N, X), E=158, 248 MeV; ¹⁰B(¹⁶O, X), E=203.6 MeV; measured σ(fragment θ, E) for fragment Z=3, 10, fusion, reaction, direct σ(E), fragment velocity spectra. ¹⁶O(¹⁰B, X), E=42-169.7 MeV; measured fusion, reaction σ(E). ¹⁰B(¹⁶O, X), E=203.6 MeV; measured evaporation residue σ(θ). ¹²C(¹⁴N, X), E=182 MeV; measured evaporation residue relative yield. Monte Carlo Hauser-Feshbach calculations.

doi: 10.1103/PhysRevC.29.1722
Citations: PlumX Metrics

1983GO11 Phys.Rev.Lett. 51, 451 (1983)

J.Gomez del Campo, D.Shapira, J.A.Biggerstaff, C.D.Moak, P.D.Miller, N.Neskovic, R.W.Fearick, J.P.F.Sellschop

Measurements of Nuclear Deexcitation Times down to 10^-19 sec using Crystal Blocking of ¹⁶O on Diamond

NUCLEAR REACTIONS ¹²C(¹⁶O, X), E=120 MeV; measured evaporation residue yields vs θ; deduced evaporation residue deexcitation times. ¹²C(¹⁶O, ¹⁶O), E=80, 120 MeV; measured yield distributions; deduced smearing parameter. Blocking technique, thick diamond crystal. Monte-Carlo statistical model calculations.

doi: 10.1103/PhysRevLett.51.451
Citations: PlumX Metrics

1979GO09 Phys.Rev.Lett. 43, 26 (1979)

J.Gomez del Campo, R.A.Dayras, J.A.Biggerstaff, D.Shapira, A.H.Snell, P.H.Stelson, R.G.Stokstad

Comparison of Fusion Cross Sections for ¹⁰B + ¹⁶O → ²⁶Al and ¹²C + ¹⁴N → ²⁶Al

NUCLEAR REACTIONS ¹⁰B(¹⁶O, X), E(cm)=15-80 MeV; measured σ(fusion, E), σ(direct, E).

doi: 10.1103/PhysRevLett.43.26
Citations: PlumX Metrics

1979GO11 Phys.Rev. C19, 2170 (1979)

J.Gomez del Campo, R.G.Stokstad, J.A.Biggerstaff, R.A.Dayras, A.H.Snell, P.H.Stelson

Fusion and Peripheral Reactions of ¹²C + ¹⁴N at Energies up to 13 MeV/A

NUCLEAR REACTIONS ¹²C(¹⁴N, X), E=34.1-178.1 MeV; measured σ(θ) of evaporation residues; deduced fusion, direct, total σ. Hauser-Feshbach, optical model calculations.

doi: 10.1103/PhysRevC.19.2170
Citations: PlumX Metrics

1976ST07 Phys.Rev.Lett. 36, 1529 (1976)

R.G.Stokstad, J.Gomez del Campo, J.A.Biggerstaff, A.H.Snell, P.H.Stelson

Fusion of ¹⁴N + ¹²C at Energies up to 178 MeV

NUCLEAR REACTIONS ¹²C(¹⁴N, X), E=43-178 MeV; measured fusion σ(E).

doi: 10.1103/PhysRevLett.36.1529
Citations: PlumX Metrics

1974KE18 Aust.J.Phys. 27, 759 (1974)

M.J.Kenny, P.W.Martin, L.E.Carlson, J.A.Biggerstaff

Gamma Ray Transitions Following keV Neutron Capture in 2s-1d Shell Nuclei

NUCLEAR REACTIONS ¹⁹F(n, γ), E=27, 44, 49 keV; ²⁷Al(n, γ), E=35 keV; ²⁸Si(n, γ), E=38, 66.7 keV; ²⁹Si(n, γ), E=15, 26 keV; ³²S(n, γ), E=30, 43 keV; ⁴⁰Ar(n, γ), E=15-70 keV; measured Eγ, Iγ. ²⁰F, ^29,30Si, ²⁸Al, ³³S resonances deduced transitions, γ-width, E1, M1-strength.

doi: 10.1071/PH740759
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset30375.

1973BI11 Nucl.Data Tables 11, 433 (1973)

J.R.Bird, B.J.Allen, I.Bergqvist, J.A.Biggerstaff

Compilation of keV-Neutron-Capture Gamma-Ray Spectra

COMPILATION A=19-238; compiled γ-spectra following 5-300 keV neutron capture; deduced resonance parameters of compound nuclei.

doi: 10.1016/S0092-640X(73)80029-4
Citations: PlumX Metrics

1973CA31 Aust.J.Phys. 26, 459 (1973)

L.E.Carlson, M.R.Najam, W.F.Davidson, J.A.Biggerstaff, P.W.Martin

The Placement of the 188 keV Transition in ⁷⁰Ga

NUCLEAR REACTIONS ⁷⁰Zn, ⁷¹Ga(p, nγ), E=3 MeV; measured Eγ, γ(t). ⁷⁰Ga level deduced T_1/2.

doi: 10.1071/PH730459
Citations: PlumX Metrics

1970CO17 Phys.Rev. C2, 149 (1970)

R.G.Couch, J.A.Biggerstaff, F.G.Perey, S.Raman, K.K.Seth

Spectroscopy of ^65,67,69Ga by (d, n) Reaction

NUCLEAR REACTIONS ^64,66,68Zn(d, n), E=10 MeV; measured σ(En, θ). ^65,67,69Ga deduced levels, L(p), J, π, S.

doi: 10.1103/PhysRevC.2.149
Citations: PlumX Metrics

1970GO19 Priv.Comm. (1970)

W.Good, J.H.Gibbons, J.A.Biggerstaff, K.K.Seth

Neutron Total Cross Sections of ²⁰³Tl and ²⁰⁵Tl

1970MI04 Phys.Rev. C1, 763 (1970)

T.G.Miller, J.A.Biggerstaff

Polarization of Neutrons from the Be⁹(d, n)B¹⁰ Reaction with 0.9- to 2.48-MeV Deuterons

NUCLEAR REACTIONS ⁹Be(d, n), E=0.9-2.48 MeV; measured σ(E;θ), P(E;θ).

doi: 10.1103/PhysRevC.1.763
Citations: PlumX Metrics

1969CO10 Phys.Letters 29B, 657 (1969)

T.G.Couch, F.G.Perey, J.A.Biggerstaff, K.K.Seth

Isobaric Spin Dependence in Proton Transfer Reactions

NUCLEAR REACTIONS ⁵⁴Fe(d, n), E=10 MeV; measured σ(En, θ). ⁵⁵Co deduced levels, J, π, L(p), S, t. Enriched ⁵⁴Fe target.

doi: 10.1016/0370-2693(69)90102-6
Citations: PlumX Metrics

1969MI04 Nucl.Phys. A124, 637(1969)

T.G.Miller, J.A.Biggerstaff

Scattering of 3.2 to 4.2 MeV Polarized Neutrons by Carbon Using a Diamond Scintillator

NUCLEAR REACTIONS ¹²C(polarized n, n), E=3.2-4.2 MeV; measured polarization P(E; 135°).

doi: 10.1016/0375-9474(69)90655-1
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13017.

1969MI20 Phys.Rev. 187, 1266 (1969)

T.G.Miller, J.A.Biggerstaff

Polarization of Neutrons from the B¹¹(d, n)C¹² Reaction at 2 MeV

NUCLEAR REACTIONS ¹¹B(d, n), E=2 MeV; measured σ(En), P(n)(θ).

doi: 10.1103/PhysRev.187.1266
Citations: PlumX Metrics

1967BE36 Phys.Rev. 158, 1049(1967)

I.Bergqvist, J.A.Biggerstaff, J.H.Gibbons, W.M.Good

Gamma Rays from keV Resonance Neutron Capture in Some (2s-1d)-Shell Nuclei

NUCLEAR REACTIONS ¹⁹F, ²³Na, ²⁴Mg, ²⁷Al, ³²S, ³⁵Cl(n, γ), E=20-120 keV; measured Eγ, Iγ. ²⁰F, ²⁴Na, ²⁵Mg, ²⁸Al, ³³S, ³⁶Cl deduced resonances, level-width, J, π.

doi: 10.1103/PhysRev.158.1049
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset11471.

1967BI03 Phys.Rev. 154, 1136 (1967)

J.A.Biggerstaff, J.R.Bird, J.H.Gibbons, W.M.Good

Radiative Transitions in ²⁰⁷Pb and ²⁰⁸Pb Following Resonance Neutron Capture in ²⁰⁶Pb and ²⁰⁷Pb

NUCLEAR STRUCTURE ²⁰⁸Pb, ²⁰⁷Pb; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.154.1136
Citations: PlumX Metrics

1967BI07 Phys.Letters 25B, 273 (1967)

J.A.Biggerstaff, C.Bingham, P.D.Miller, J.Solomon, K.K.Seth

Proton Particle-Hole States in ¹¹⁶Sn

NUCLEAR STRUCTURE ¹¹⁶Sn; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0370-2693(67)90011-1
Citations: PlumX Metrics

1967SE10 Phys.Rev. 164, 1450 (1967)

K.K.Seth, J.A.Biggerstaff, P.D.Miller, G.R.Satchler

Study of Proton Particle-Hole States in ⁴⁰Ca by the ³⁹K(³He, D)⁴⁰Ca Reaction

NUCLEAR STRUCTURE ⁴⁰Ca; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.164.1450
Citations: PlumX Metrics

1966BI06 Priv.Comm. (1966)

J.A.Biggerstaff, R.Farrell

1966BI15 ORNL-TM-1665, p.3 (1966)

J.A.Biggerstaff, Y.Cassagnou, W.E.Kinney, M.V.Harlow, Jr., J.M.McConnell, F.G.Perey, P.H.Stelson

Neutron Inelastic Scattering Program

NUCLEAR STRUCTURE ⁵⁹Ni, ⁵⁹Cu, ⁵⁹Co, ⁵¹V, ²⁸Si, ⁶⁰Cu, ⁶⁵Zn, ⁵⁶Fe, ⁵³Mn, ⁵¹Cr, ⁵⁵Fe, ⁴⁰Ca, ³⁹K, ¹²C, ⁸⁹Y, ²⁷Al, ²³Na; measured not abstracted; deduced nuclear properties.

1966SE08 Phys.Rev.Letters 17, 1294 (1966)

K.K.Seth, R.G.Couch, J.A.Biggerstaff, P.D.Miller

Reaction ³⁹K(³He, P)⁴¹Ca and Two-Particle, One-Hole States

NUCLEAR STRUCTURE ⁴¹Ca; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRevLett.17.1294
Citations: PlumX Metrics

1965BE20 Phys.Letters 18, 323 (1965)

I.Bergqvist, J.A.Biggerstaff, J.H.Gibbons, W.M.Good

Neutron Resonance Capture in 2s-1d shell Nuclei

NUCLEAR STRUCTURE ³³S, ²⁸Al, ²⁵Mg; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(65)90356-2
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset11471.

1965BI03 Phys.Rev. 138, B20 (1965)

J.R.Bird, J.A.Biggerstaff, J.H.Gibbons, W.M.Good

Study of the Gamma-Ray Spectra Emitted in the Resonance Capture of Neutrons by ¹⁹F

NUCLEAR STRUCTURE ¹⁹F; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.138.B20
Citations: PlumX Metrics

1965SE01 Bull.Am.Phys.Soc. 10, No.1, 10, AC8 (1965)

K.K.Seth, G.Walter, P.D.Miller, J.A.Biggerstaff

¹⁵N(³He, p) Reaction and Intermediate States

NUCLEAR STRUCTURE ¹⁵N; measured not abstracted; deduced nuclear properties.

1964BE18 WASH-1048, p. 77 (1964)

I.Bergqvist, J.A.Biggerstaff, J.H.Gibbons, W.M.Good

Neutron Capture γ-Ray Spectra

NUCLEAR STRUCTURE ²⁰⁸Pb, ²⁰⁷Pb; measured not abstracted; deduced nuclear properties.

1964BI05 Bull. Am. Phys. Soc. 9, No. 4, 433, EC4 (1964)

J.A.Biggerstaff, J.H.Gibbons, W.M.Good, R.L.Macklin, P.J.Pasma

Kev-Range Neutron Resonances in ³²S, ⁵⁶Fe, ²⁰⁶Pb, ²⁰⁷Pb, and ²⁰⁸Pb

1964BI12 ORNL-3582, p. 68 (1964)

J.A.Biggerstaff, J.H.Gibbons, W.M.Good, I.Bergqvist

Gamma-Ray Spectra from Resonant Neutron Capture on F¹⁹

NUCLEAR STRUCTURE ²⁰F; measured not abstracted; deduced nuclear properties.

1964BI13 ORNL-3582, p. 71 (1964)

J.A.Biggerstaff, J.H.Gibbons, W.M.Good, I.Bergqvist

Resonant Neutron Capture Gamma-Ray Spectra from Nuclei in the s-d Shell

NUCLEAR STRUCTURE ³³S, ²⁴Na, ²⁵Mg, ²⁸Al; measured not abstracted; deduced nuclear properties.

1964BI14 ORNL-3582, p. 75 (1964)

J.A.Biggerstaff, J.H.Gibbons, W.M.Good, R.L.Macklin, P.Pasma

High Resolution Neutron Total Cross Section

1964BI15 ORNL-3582, p. 82 (1964)

J.A.Biggerstaff, W.M.Good, H.Kim

The Strength Functions of the Isotopes of Zirconium

NUCLEAR STRUCTURE ⁹³Zr, ⁹¹Zr, ⁹⁵Zr, ⁹⁷Zr; measured not abstracted; deduced nuclear properties.

1964BI17 ORNL-3778, p. 76 (1964)

J.A.Biggerstaff, W.M.Good, H.Kim

A Study of the Resonance Structure of the Even Zirconium Isotopes at below 60-keV Neutron Energy

1963BI06 Bull.Am.Phys.Soc. 8, No.4, 333, K1 (1963)

J.A.Biggerstaff, J.R.Bird, J.H.Gibbons, W.M.Good

Resonant Neutron-Capture Spectra in Fe^{54, 56} and Ca^{40, 42, 44}

NUCLEAR STRUCTURE ⁴¹Ca, ⁴³Ca, ⁵⁵Fe, ⁵⁷Fe, ⁴⁵Ca; measured not abstracted; deduced nuclear properties.

1963BI16 WASH-1044, p.62 (1963)

J.A.Biggerstaff, H.J.Kim, W.M.Good

Total Neutron Cross Sections of Zr⁹⁰, ⁹¹, ⁹², ⁹⁴, ⁹⁶

NUCLEAR STRUCTURE ⁹⁷Zr, ⁹⁵Zr, ⁹³Zr, ⁹²Zr, ⁹¹Zr; measured not abstracted; deduced nuclear properties.

1963GI10 ORNL-3425, p.57 (1963)

J.H.Gibbons, W.M.Good, J.R.Bird, J.A.Biggerstaff

Resonant Neutron Capture Gamma-Ray Spectra

NUCLEAR STRUCTURE ²⁰⁸Pb, ²⁰⁷Pb, ⁴¹Ca, ⁵⁵Fe, ⁵⁷Fe; measured not abstracted; deduced nuclear properties.

1963KI09 ORNL-3425, p.32 (1963)

H.J.King, J.A.Biggerstaff, W.M.Good

Total Neutron Cross Sections in Isotopes of Zr, Fe, Cr, and Ca

NUCLEAR STRUCTURE ⁵⁴Cr, ⁴⁴Ca, ⁵⁸Fe, ⁹⁵Zr, ⁹⁷Zr, ⁹¹Zr, ⁹³Zr, ⁹²Zr; measured not abstracted; deduced nuclear properties.

1963KI20 Bull.Am.Phys.Soc. 8, No.7, 556, K1 (1963)

H.Kim, J.A.Biggerstaff, W.M.Good

Total Neutron Cross Sections in Isotopes of Zr, Fe, Cr, and Ca

NUCLEAR STRUCTURE ⁹²Zr, ⁹³Zr, ⁹¹Zr, ⁹⁷Zr, ⁹⁵Zr, ⁴⁴Ca, ⁵⁴Cr; measured not abstracted; deduced nuclear properties.

1962BI11 Nuclear Phys. 36, 631 (1962)

J.A.Biggerstaff, R.F.Hood, H.Scott, M.T.McEllistrem

Differential Cross Sections for (d, α) and (d, t) Reactions in Be⁹

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

doi: 10.1016/0029-5582(62)90488-1
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0095.

1961BI02 Bull.Am.Phys.Soc. 6, No.3, 226, AA6 (1961)

J.A.Biggerstaff, R.F.Hood, M.T.McEllistrem

Be⁹ + p and Be⁹ + d Reactions at Low Energies

NUCLEAR STRUCTURE ⁷Li, ⁸Be; measured not abstracted; deduced nuclear properties.

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