Nuclear Science References (NSR)

Fast-Neutron Interaction with Collective Cadmium Nuclei

NUCLEAR REACTIONS Cd(n, n), (n, n'), E=1.5-10 MeV; measured σ(θ); deduced σ(E), model parameters. Optical-statistical, dispersive-optical, coupled-channels analysis.

doi: 10.1016/0375-9474(94)90199-6
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1994SM03 J.Phys.(London) G20, 795 (1994)

Fast-Neutron Scattering from Vibrational Nuclei: ¹⁰³Rh

NUCLEAR REACTIONS ¹⁰³Rh(n, n), (n, n'), E ≈ 1.5-10 MeV; measured σ(θ). Models comparison.

doi: 10.1088/0954-3899/20/5/013
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1994SM10 Ann.Nucl.Energy 21, 629 (1994)

Fast-Neutron Scattering from Vibrational Palladium Nuclei

NUCLEAR REACTIONS Pd(n, n'), E ≈ 1.5-10 MeV; measured σ(θ) vs E; deduced σ(E). Spherical optical, coupled-channels model analyses.

doi: 10.1016/0306-4549(94)90072-8
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1993SM02 J.Phys.(London) G19, 655 (1993)

Fast-Neutron Scattering Near Shell Closures: Scandium

NUCLEAR REACTIONS ⁴⁵Sc(n, n), (n, n'), E=1.5-10 MeV; measured σ(θ); analyzed σ(E); deduced model parameters. ⁴⁵Sc deduced levels. Optical-statistical models, energy dependent geometric parameters.

doi: 10.1088/0954-3899/19/4/019
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1992CH05 Phys.Rev. C45, 1260 (1992)

S.Chiba, P.T.Guenther, A.B.Smith, M.Sugimoto, R.D.Lawson

Fast-Neutron Interaction with Elemental Zirconium, and the Dispersive Optical Model

NUCLEAR REACTIONS Zr(n, n), (n, n'), E ≈ 1.5-10 MeV; measured σ(θ); deduced σ(E), model parameters. Optical-statistical models.

doi: 10.1103/PhysRevC.45.1260
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1992SM04 J.Phys.(London) G18, 629 (1992)

A.B.Smith, P.T.Guenther, J.F.Whalen, S.Chiba

Fast-Neutron Total and Scattering Cross Sections of ⁵⁸Ni and Nuclear Models

NUCLEAR REACTIONS ⁵⁸Ni(n, n), (n, n'), E ≈ 1-10 MeV; measured σ(θ), σ. White source technique. Optical-statistical, dispersive-optical models, coupled-channels methods.

doi: 10.1088/0954-3899/18/4/004
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1990CH40 Phys.Rev. C42, 2487 (1990)

S.Chiba, P.T.Guenther, R.D.Lawson, A.B.Smith

Neutron Scattering from Elemental Indium: Optical model and bound-state potential

NUCLEAR REACTIONS In(n, n), E=4.5-10 MeV; calculated σ(θ); deduced optical potential parameters. Other data input.

doi: 10.1103/PhysRevC.42.2487
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1990LA24 Nucl.Phys. A519, 487 (1990)

Ambiguities in the Elastic Scattering of 8 MeV Neutrons from Adjacent Nuclei

NUCLEAR REACTIONS ⁵¹V, Cr, ⁵⁹Co, ⁵⁸Ni, Cu, Zn, ⁸⁹Y, ⁹³Nb, Zr, In, Cd, ²⁰⁹Bi, Pb(n, n), E=8 MeV; measured σ(θ), ratio for adjacent nuclei; deduced ambiguities. Optical model.

doi: 10.1016/0375-9474(90)90442-O
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1989CH40 Ann.Nucl.Energy 16, 637 (1989)

S.Chiba, P.T.Guenther, A.B.Smith

Some Remarks on the Neutron Elastic-and Inelastic-Scattering Cross Sections of Palladium

NUCLEAR REACTIONS Pd(n, n), E=5.9, 7.1, 8 MeV; measured σ(θ). Analyzed other data. Elemental Pd target.

doi: 10.1016/0306-4549(89)90140-0
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1989LA09 Nucl.Phys. A493, 267 (1989)

Neutron Scattering and the Fermi Surface Anomaly in ⁵¹V

NUCLEAR REACTIONS ⁵¹V(n, n), (n, n'), E=4.5-10 MeV; measured σ(θ) versus E. Optical model interpretation.

doi: 10.1016/0375-9474(89)90398-9
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1989SU13 Nucl.Sci.Eng. 103, 37 (1989)

M.Sugimoto, P.T.Guenther, J.E.Lynn, A.B.Smith, J.F.Whalen

The Interaction of Fast Neutrons with Beryllium

NUCLEAR REACTIONS ⁹Be(n, n), E=1-10 MeV; measured σ(E), σ(θ). ⁹Be(n, n'), E=4.5-10 MeV; measured σ(θ); deduced angle-integrated σ.

doi: 10.13182/NSE89-A23658
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1988SM02 Nucl.Phys. A483, 50 (1988)

A.B.Smith, P.T.Guenther, R.D.Lawson

Energy Dependence of the Optical Model Potential for Fast Neutron Scattering from Cobalt

NUCLEAR REACTIONS ⁵⁹Co(n, n), (n, n'), E=1.5-10 MeV; measured σ(θ) vs E. Optical coupled-channels models.

doi: 10.1016/0375-9474(88)90064-4
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1987LA21 Phys.Rev. C36, 1298 (1987)

Energy Dependence of the Optical-Model Potential for Fast-Neutron Scattering from Bismuth

NUCLEAR REACTIONS ²⁰⁹Bi(n, n), E=4.5-10 MeV; measured σ(θ); deduced σ(E), potential energy dependence. Optical model, other data input.

doi: 10.1103/PhysRevC.36.1298
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1987SU16 Nucl.Sci.Eng. 97, 235 (1987)

M.Sugimoto, A.B.Smith, P.T.Guenther

Ratio of the Prompt Fission Neutron Spectrum of ²³⁹Pu to that of ²³⁵U

NUCLEAR REACTIONS ²³⁹Pu, ²³⁵U(n, F), E ≈ 0.55 MeV; measured prompt fission neutron spectrum; deduced average fission spectrum energy ratio. Tof, enriched target.

doi: 10.13182/NSE87-A23505
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1986GU01 Nucl.Phys. A448, 280 (1986)

P.T.Guenther, D.L.Smith, A.B.Smith, J.F.Whalen

Total, Scattering, and Gamma Production Cross Sections for Few-MeV Neutrons on Elemental Copper

NUCLEAR REACTIONS Cu(n, X), (n, n), (n, n'), (n, n'γ), E=0.6-4.5 MeV; measured σ(θ), σ(E). Spherical optical-statistical model, coupled-channels calculations.

doi: 10.1016/0375-9474(86)90092-8
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1986GU08 Radiat.Eff. 94, 281 (1986)

P.T.Guenther, A.B.Smith

Angular-Distribution Neutron-Emission Spectra of Niobium following Bombardment by Fast Neutrons

NUCLEAR REACTIONS ⁹³Nb(n, xn), E=5.9, 7.1, 8.4 MeV; measured emission neutron spectra, σ(θ). ⁹⁴Nb deduced Maxwellian temperature distribution on set.

doi: 10.1080/00337578608208392
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1986GU18 Ann.Nucl.Energy 13, 601 (1986)

P.T.Guenther, D.L.Smith, A.B.Smith, J.F.Whalen

Total, Scattering and γ-Ray-Production Cross Sections for Few-MeV Neutrons on ⁵⁴Fe

NUCLEAR REACTIONS ⁵⁴Fe(n, n), (n, n'), (n, γ), E=0.5-4 MeV; measured total, reaction, γ production σ(E), σ(θ), Eγ. ⁵⁴Fe deduced levels, γ-branching, J, π. Enriched target, tof. Spherical optical model.

doi: 10.1016/0306-4549(86)90017-4
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1986LA30 Phys.Rev. C34, 1599 (1986)

Search for the Fermi-Surface Anomaly in Fast-Neutron Scattering from Yttrium

NUCLEAR REACTIONS ⁸⁹Y(n, n), E=4-10 MeV; measured σ(θ, En); calculated σ(E); deduced no Fermi surface anomaly. Optical, statistical model analyses.

doi: 10.1103/PhysRevC.34.1599
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1986SM03 Nucl.Phys. A455, 344 (1986)

A.B.Smith, P.T.Guenther, R.D.Lawson

On the Energy Dependence of the Optical Model of Neutron Scattering from Niobium

NUCLEAR REACTIONS ⁹³Nb(n, n), E=1.5-10 MeV; measured σ(θ); deduced optical model parameters.

doi: 10.1016/0375-9474(86)90022-9
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1986SM08 Radiat.Eff. 92, 129 (1986)

A.B.Smith, P.T.Guenther, W.P.Poenitz, D.L.Smith, J.F.Whalen, R.J.Howerton

Fast-Neutron Interaction with Niobium

NUCLEAR REACTIONS ⁹³Nb(n, n), E=0.04-20 MeV; measured σ. ⁹³Nb(n, n), (n, n'), E=1.5-10 MeV; measured σ(θ); deduced potential parameters. ⁹³Nb(n, γ), E=0.1-2.6 MeV; measured capture σ(E).

doi: 10.1080/00337578608208305
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1986SM11 Radiat.Eff. 95, 285 (1986)

D.L.Smith, J.W.Meadows, P.T.Guenther

Investigation of Thick-Target Neutron Emission from Be-9(d, n)B-10 at E(d) = 7 MeV for Angles Other than Zero Degrees

NUCLEAR REACTIONS ⁹Be(d, n), E=7 MeV; measured neutron yields vs En, θn; deduced angular dependence anisotropy. Organic scintillation detectors, tof.

doi: 10.1080/00337578608208706
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1985SM01 J.Phys.(London) G11, 125 (1985)

A.B.Smith, P.T.Guenther, J.F.Whalen, I.J.van Heerden, W.R.McMurray

Fast-Neutron Scattering from Indium

NUCLEAR REACTIONS In(n, n'), E=1.5-3.8 MeV; measured σ(θ). In(n, n'γ), E=0.86-2.4 MeV; measured Eγ, Iγ, σ(E); deduced optical model parameters. ¹¹⁵In deduced levels, γ-branching, J, π.

doi: 10.1088/0305-4616/11/1/018
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1985SM08 Nucl.Instrum.Methods 241, 507 (1985)

D.L.Smith, J.W.Meadows, P.T.Guenther

Neutron Emission from the ⁹Be(d, n)¹⁰B Thick-Target Reaction for 7 MeV Deuterons

NUCLEAR REACTIONS ⁹Be(d, n), E=7 MeV; measured thick target neutron yield vs θ; deduced anisotropy, role in neutron induced reaction σ.

doi: 10.1016/0168-9002(85)90604-7
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1984SM02 Nucl.Phys. A415, 1 (1984)

The Optical Model of Few-MeV Neutron Elastic Scattering from Z = 39 to 51 Targets

NUCLEAR REACTIONS ⁸⁹Y, Zr, ⁹³Nb, Mo, Rh, Pd, Ag, Cd, In, Sn, Sb(n, n), E ≈ 1.5-4 MeV; measured σ(θ); deduced optical model parameters, geometric, isospin, shell dependent effects. Spherical optical, statistical model analyses.

doi: 10.1016/0375-9474(84)90596-7
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1982BU08 Z.Phys. A306, 265 (1982)

C.Budtz-Jorgensen, P.T.Guenther, A.B.Smith, J.F.Whalen

Fast-Neutron Total and Scattering Cross Sections of ⁵⁸Ni

NUCLEAR REACTIONS ⁵⁸Ni(n, n), (n, n'), E=0.9-4.5 MeV; measured σ(total) vs E, σ(θ). Statistical, optical, coupled-channels models.

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset12752.

1982GU14 Nucl.Sci.Eng. 82, 408 (1982)

P.T.Guenther, A.B.Smith, J.F.Whalen

The Total, Elastic and Inelastic Scattering Fast Neutron Cross Sections of Natural Chromium

NUCLEAR REACTIONS Cr(n, n), (n, n'), E=1-4.5 MeV; measured σ(θ), σ(total), σ(elastic) vs E; deduced resonance structure. Optical, statistical model analyses.

doi: 10.13182/NSE82-A21455
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1982GU18 Phys.Rev. C26, 2433 (1982)

P.T.Guenther, A.B.Smith, J.F.Whalen

Fast-Neutron Total and Scattering Cross Sections of ¹⁸²W, ¹⁸⁴W, and ¹⁸⁶W

NUCLEAR REACTIONS ^182,184,186W(n, n), (n, n'), E=0.3-5 MeV; measured σ(θ), σ(total). ^182,184,186W deduced levels, band structure. Statistical, coupled-channels models.

doi: 10.1103/PhysRevC.26.2433
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1982SM02 Nucl.Phys. A373, 305 (1982)

Neutron Total and Scattering Cross Sections of ⁶Li in the Low-MeV Range

NUCLEAR REACTIONS ⁶Li(n, n), E=0.1-4.8 MeV; measured σ(total), σ(θ); ⁶Li(n, n'), E=3.5-4 MeV; measured σ(θ). R-matrix interpretation. Model parameters, reaction mechanisms discussed.

doi: 10.1016/0375-9474(82)90153-1
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1978GU01 Nucl.Sci.Eng. 65, 174 (1978)

P.T.Guenther, D.G.Havel, A.B.Smith

Neutron Scattering and the Optical Model Near A = 208 and Implications on the Inelastic Scattering Cross Section of Uranium-238

NUCLEAR REACTIONS ^206,207,208Pb, ²⁰⁹Bi(n, n), E=0.6-1.0 MeV; measured σ(E, θ); deduced optical model parameters.

doi: 10.13182/NSE78-A27140
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1974GU12 Nucl.Sci.Eng. 54, 273 (1974)

P.T.Guenther, P.A.Moldauer, A.B.Smith, J.F.Whalen

Cobalt Fast-Neutron Cross Sections

NUCLEAR REACTIONS ⁵⁹Co(n, n), (n, n'), E=1.8-4.0 MeV; ⁵⁹Co(n, X), E=2.0-4.5 MeV; measured σ(θ), σ(En', θ), σ. ⁵⁹Co deduced levels, J, π.

doi: 10.13182/NSE74-A23418
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1973SM10 Z.Phys. 264, 379 (1973)

Neutron Total and Scattering Cross Sections of Niobium in the Continuum Region

NUCLEAR REACTIONS ⁹³Nb(n, n), (n, n'), (n, X), E=1.8-4.0 MeV; measured σ(E;θ). ⁹³Nb deduced levels, J, π.

doi: 10.1007/BF01391707
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1968SM03 Phys.Rev. 168, 1344 (1968)