Nuclear Science References (NSR)

NUCLEAR STRUCTURE ²⁶Al; analyzed transition probability distributions, matrix elements; deduced role of isospin symmetry breaking. Statistical analysis, random matrix model.

doi: 10.1103/PhysRevE.62.1936
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1994GR14 Phys.Lett. 331B, 257 (1994)

M.Granzow, H.L.Harney, H.Kalka

Propagation of a Two-Body Force Into A-Body Space

doi: 10.1016/0370-2693(94)91047-2
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1992MU06 Phys.Rev. C45, 1955 (1992)

A.Muller, H.L.Harney

Parity Violation in Neutron Statistical Scattering

NUCLEAR STRUCTURE A=32-137; analyzed neutron scattering data; deduced transmission observables parity violation sensitivisty. Statistical model.

doi: 10.1103/PhysRevC.45.1955
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1990HA39 Nucl.Phys. A518, 35 (1990)

H.L.Harney, A.Hupper, A.Richter

Ericson FLuctuations, Detailed Balance and Time-Reversal Invariance

NUCLEAR REACTIONS ²⁷Al(p, α), E ≈ 7.40-11.38 MeV; ²⁴Mg(α, p), E ≈ 10.38-14.64 MeV; analyzed data. Ericson fluctuations, detailed balance, time-reversal invariance.

doi: 10.1016/0375-9474(90)90533-R
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1990MU16 Phys.Rev.Lett. 65, 1329 (1990)

A.Muller, E.D.Davis, H.L.Harney

Parity Violation in Compound-Nucleus Reactions

NUCLEAR REACTIONS ¹⁸¹Ta, ¹⁴⁶Nd, ¹³⁹La, ¹⁵⁰Sm, ²⁰⁴Pb, ⁸⁵Rb, ¹¹⁵In, ^94,91,90Zr, ⁸⁸Sr, ¹¹⁰Pd(polarized n, X), E ≈ 1 eV-10 keV; calculated transmission assymmetry rms value vs En. Statistical theory, parity violation.

doi: 10.1103/PhysRevLett.65.1329
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1990RE10 Z.Phys. A337, 121 (1990)

J.Reiter, H.L.Harney

Isospin Mixing Matrix Elements Extracted from Isobaric Analog Resonances

NUCLEAR STRUCTURE A=31-238; analyzed isobaric analog resonance data; deduced isospin mixing matrix elements, spreading widths.

1986BO10 Phys.Rev.Lett. 56, 2012 (1986)

D.Boose, H.L.Harney, H.A.Weidenmuller

Tests of Time-Reversal Symmetry in Compound-Nucleus Reactions

NUCLEAR STRUCTURE ²⁸Si; calculated symmetry breaking strength, associated spreading width for compound nucleus. Detailed balance violation, perturbative treatment.

doi: 10.1103/PhysRevLett.56.2012
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1984HA23 Z.Phys. A316, 177 (1984)

H.L.Harney

Are Resonance Decay Amplitudes Gaussian Variables ( Question )

NUCLEAR REACTIONS ⁴⁸Ti, ⁴⁸Ca, ⁵⁰Cr(p, p'), E ≈ resonance; calculated resonance decay amplitudes; deduced resonance amplitude, Gaussian variable relation validity.

doi: 10.1007/BF01412260
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1984HA33 Phys.Rev.Lett. 53, 537 (1984)

H.L.Harney

Proton Resonance Scattering Confirms the Gaussian Statistics of Decay Amplitudes

NUCLEAR REACTIONS ⁵⁰Cr, ⁴⁸Ti, ⁴⁴Ca, ⁵⁶Fe(p, p'), E=resonance; analyzed resonance decay amplitudes; deduced width correlation ratio, amplitude correlation expectation value, Gaussian statistics validity.

doi: 10.1103/PhysRevLett.53.537
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1983HA05 Nucl.Phys. A394, 369 (1983)

H.L.Harney, H.A.Weidenmuller, A.Richter

Autocorrelation Function of Fluctuating Nuclear Cross Sections in the Presence of Isospin Mixing

NUCLEAR REACTIONS ²⁸Si(d, α), ²⁹Si(p, α), E not given; analyzed data; deduced correlation strengths. ³⁰P deduced resonance widths. Autocorrelation function, fluctuations.

doi: 10.1016/0375-9474(83)90110-0
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1983WA22 Phys.Rev. C28, 1538 (1983)

S.Wald, I.Tserruya, Z.Fraenkel, G.Doukellis, H.Gemmeke, H.L.Harney

Neutron, Proton, and Alpha Emission in Deep Inelastic Collisions of ¹⁶O on Three Ca Isotopes at 102 and 142 MeV

NUCLEAR REACTIONS ^40,44,48Ca(¹⁶O, X), E=102, 142 MeV; measured σ(fragment θ) for X=C, N, O, F. ^40,44,48Ca(¹⁶O, nX), (¹⁶O, pX), (¹⁶O, αX), E=102, 142 MeV; measured projectile fragment (light particle)-coin; deduced light particle multiplicities, production mechanism.

doi: 10.1103/PhysRevC.28.1538
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1982LI21 Nucl.Phys. A391, 205 (1982)

J.-Q.Li, H.L.Harney

Cross-Section Fluctuations in Isobaric Mirror Channels

NUCLEAR REACTIONS ¹²C(¹⁴N, t), (¹⁴N, ³He), E=40-50 MeV; analyzed data. ²⁶Al deduced isospin mixing parameter, mean Coulomb mixing matrix element, decay widths, level separation.

doi: 10.1016/0375-9474(82)90228-7
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1982WA03 Phys.Rev. C25, 1118 (1982)

S.Wald, I.Tserruya, Z.Fraenkel, G.Doukellis, H.Gemmeke, H.L.Harney

Neutron, Proton, and Alpha Emission in Deep Inelastic Collisions of ¹⁶O on ⁴⁸Ca at 142 MeV

NUCLEAR REACTIONS ⁴⁸Ca(¹⁶O, nX), (¹⁶O, pX), (¹⁶O, αX), E=142 MeV; measured nX-, pX-, αX-coin; deduced σ(θ), σ(E) for n-, p-, α-emission. Statistical evaporation, heavy fragments rest frame.

doi: 10.1103/PhysRevC.25.1118
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1981HA43 Nucl.Phys. A371, 32 (1981)

H.L.Harney, Tang Xue-Tian

Isospin Breaking Matrix Elements in Compound Nuclei

NUCLEAR STRUCTURE ³⁰P, ⁴⁹V, ⁵²Cr, ⁵⁵Mn, ⁵⁶Fe, ⁶⁰Ni, ⁶³Cu, ^66,64Zn, ⁶⁹Ga, ¹¹¹In; calculated isospin mixing. Statistical nuclear reaction transport theory.

doi: 10.1016/0375-9474(81)90743-0
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1981PO04 Nucl.Phys. A357, 237 (1981)

F.Porto, S.Sambataro, K.Kusterer, Liu Ken Pao, G.Doukellis, H.L.Harney

Reaction and Fusion Cross Sections for ³²S on ²⁷Al and ⁴⁸Ti

NUCLEAR REACTIONS ⁴⁸Ti(³²S, ³²S), (³²S, X), E(cm)=96 MeV; ²⁷Al(³²S, ³²S), (³²S, X), E(cm)=66.4, 73.2 MeV; measured σ(θ, elastic), σ(θ, evaporation residues); deduced σ(reaction).

doi: 10.1016/0375-9474(81)90636-9
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1980HA44 Phys.Lett. B96, 227 (1980)

H.L.Harney, H.A.Weidenmuller, A.Richter

Elastic Enhancement Factor in Charge Exchange Reactions

NUCLEAR REACTIONS ²⁹Si, ⁴⁸Ti, ⁵¹V, ⁵⁴Cr, ⁵⁵Mn, ⁵⁹Co, ⁶²Ni, ^63,65Cu, ⁶⁸Zn, ¹¹⁰Cd(p, n), E not given; calculated compound elastic scattering enhancement; deduced dependence on isospin mixing. ³⁰P, ⁴⁹V, ⁵²Cr, ⁵⁵Mn, ⁵⁶Fe, ⁶⁰Ni, ⁶³Cu, ^64,66Zn, ⁶⁹Ga, ¹¹¹In deduced width fluctuation factor.

doi: 10.1016/0370-2693(80)90754-6
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1979GA12 Z.Phys. A291, 347 (1979)

A.Gamp, H.L.Harney, J.C.Roynette, E.Plagnol, H.Fuchs, H.Doubre, J.C.Jacmart, N.Poffe

Out-of-Plane Correlations of α-Particles and Heavy Ions in the Reaction of 373 MeV ³²S with Gold

NUCLEAR REACTIONS ¹⁹⁷Au(³²S, X), E=373 MeV; measured σ(θ, φ) for P, S, Si+α, Al+α; deduced reaction mechanism.

doi: 10.1007/BF01408385
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1979OE03 Nucl.Phys. A325, 463 (1979)

H.Oeschler, H.L.Harney, D.L.Hillis, K.S.Sim

On the Determination of the Reaction Cross Section from Elastic Scattering

NUCLEAR REACTIONS ¹⁴⁶Nd(¹⁶O, ¹⁶O), E=81.5, 106.3 MeV; ¹³⁰Te(³²S, ³²S), E=139.5 MeV; measured nothing; calculated σ(reaction). Coupled-channels method.

doi: 10.1016/0375-9474(79)90027-7
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1978BA19 Nucl.Phys. A299, 147 (1978)

J.Barrette, P.Braun-Munzinger, C.K.Gelbke, H.L.Harney, H.E.Wegner, B.Zeidman, K.D.Hildenbrand, U.Lynen

Nuclide Distributions in Deep Inelastic Reactions

NUCLEAR REACTIONS ^42,48Ca, ⁵⁰Ti, ⁵⁰Cr, ⁵⁶Fe, ⁶⁰Ni(⁴⁰Ar, X), E(lab)=236 MeV; measured deep inelastic σ(A, Z, θ).

doi: 10.1016/0375-9474(78)90214-2
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1978TS04 Phys.Rev. C18, 1688 (1978)

I.Tserruya, Y.Eisen, D.Pelte, A.Gavron, H.Oeschler, D.Berndt, H.L.Harney

Total Fusion Cross Section for the ¹⁶O + ¹⁶O System

NUCLEAR REACTIONS ¹⁶O(¹⁶O, X), E=27-66 MeV; measured fusion σ(E); deduced barrier, critical parameters. Statistical model analysis.

doi: 10.1103/PhysRevC.18.1688
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1541.

1977BA15 Nucl.Phys. A279, 125 (1977)

J.Barrette, P.Braun-Munzinger, C.K.Gelbke, H.E.Wegner, B.Zeidman, A.Gamp, H.L.Harney, T.Walcher

Fission Characteristics of the Composite System ³²S + ⁵⁰Ti (II). Energy and Angular Dependence

NUCLEAR REACTIONS ⁵⁰Ti(³²S, X), E=110-166 MeV; measured σ(E, A, θ), A=35-60.

doi: 10.1016/0375-9474(77)90425-0
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1976BA16 Nucl.Phys. A261, 491 (1976)

J.Barrette, P.Braun-Munzinger, C.K.Gelbke, H.L.Harney, J.Kuzminski, I.Tserruya

Unexpected Interference Patterns Observed in the ¹²C(¹⁴N, ¹³N)¹³C Reaction at Energies Close to the Coulomb Barrier

NUCLEAR REACTIONS ¹²C(¹⁴N, ¹³N), E=28, 32, 34, 36 MeV; measured σ(E(¹³N), θ); deduced symmetry violation, existence of complex reaction mechanism. Enriched targets.

doi: 10.1016/0375-9474(76)90162-7
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1841.

1976BR04 Phys.Rev.Lett. 36, 849 (1976)

P.Braun-Munzinger, C.K.Gelbke, J.Barrette, B.Zeidman, M.J.LeVine, A.Gamp, H.L.Harney, T.Walcher

Experimental Proof for Binary Mass Division of a Composite System with A ≈ 80

NUCLEAR REACTIONS ⁵⁰Ti(³²S, X), E=140 MeV; measured two-particle coin; deduced binary mass division.

doi: 10.1103/PhysRevLett.36.849
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1976GA37 Nukleonika 21, 753 (1976)

A.Gamp, P.Braun-Munzinger, C.K.Gelbke, H.L.Harney

Exchange Symmetries in Heavy Ion Reactions

NUCLEAR REACTIONS ¹³C(¹⁵N, ¹⁴N), E=30, 32, 45 MeV; measured σ(θ); deduced reaction mechanism.

1976GE13 Nucl.Phys. A269, 460 (1976)

C.K.Gelbke, P.Braun-Munzinger, J.Barrette, B.Zeidman, M.J.Levine, A.Gamp, H.L.Harney, T.Walcher

Fission Characteristics of the Composite System ³²S + ⁵⁰Ti (I). Correlations between Coincident Fragments

NUCLEAR REACTIONS ⁵⁰Ti(³²S, X), E=140 MeV; measured fragment-fragment coin, σ(E, M), M=37-59, Q-value distributions, in-, out-of-plane angular correlations.

doi: 10.1016/0375-9474(76)90693-X
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1975BA45 Z.Phys. A274, 121 (1975)

J.Barrette, P.Braun-Munzinger, C.K.Gelbke, E.Grosse, H.L.Harney, J.Kuzminski, I.Tserruya, T.Walcher

Observation of a Fission-Like Process in the Bombardment of ⁴⁸Ti and ⁵⁰Ti by ³²S

NUCLEAR REACTIONS ^48,50Ti(³²S, X), E=105, 130, 144 MeV; measured σ(E(fragment mass), θ).

doi: 10.1007/BF01408463
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1975GA17 Nucl.Phys. A250, 341 (1975)

A.Gamp, P.Braun-Munzinger, C.K.Gelbke, H.L.Harney, H.G.Bohlen, W.Bohne, K.D.Hildenbrand, J.Kuzminski, W.Von Oertzen, I.Tserruya

Interfering Proton and Neutron Transfer in the Reaction ¹³C(¹⁵N, ¹⁴N)¹⁴C

NUCLEAR REACTIONS ¹³C(¹⁵N, ¹⁴N)(¹⁵N, ¹⁴C), E=30, 32, 45 MeV; measured σ(θ); deduced spectroscopic amplitudes. Enriched targets.

doi: 10.1016/0375-9474(75)90264-X
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1975TS01 Nucl.Phys. A242, 345 (1975)

I.Tserruya, W.Bohne, P.Braun-Munzinger, C.K.Gelbke, W.Grochulski, H.L.Harney, J.Kuzminski

Transfer Reactions Induced by ¹⁶O on ^29,30Si

NUCLEAR REACTIONS ^28,29,30Si(¹⁶O, ¹⁶O), ^29,30Si(¹⁶O, ¹⁵N), ²⁹Si(¹⁶O, ¹⁵O), ^29,30Si(¹⁶O, ¹⁷O), ³⁰Si(¹⁶O, ¹⁴C), ³⁰Si(¹⁶O, ¹⁸O), E(lab)=73.5 MeV; measured σ(θ). ^28,29,30Si, ^30,31P, ³²S levels deduced S. Recoil DWBA analysis. Enriched targets.

doi: 10.1016/0375-9474(75)90054-8
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1974BO15 Nucl.Phys. A222, 117 (1974)

W.Bohne, C.K.Gelbke, P.Braun-Munzinger, W.Grochulski, H.L.Harney, H.Oeschler

Elastic Transfer of a 1p₃/₂ Hole in the Scattering of ¹²C on ¹¹B

NUCLEAR REACTIONS ¹¹B(¹²C, ¹²C), E=15, 17, 20, 24 MeV; measured σ(θ). Enriched targets.

doi: 10.1016/0375-9474(74)90587-9
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1974BR18 Nucl.Phys. A223, 381 (1974)

P.Braun-Munzinger, H.L.Harney

An Approximate Treatment of Recoil Effects in Heavy Ion Transfer Reactions

NUCLEAR REACTIONS ¹²C(¹⁴N, ¹³N), E=78 MeV; calculated recoil, finite range effects.

doi: 10.1016/0375-9474(74)90421-7
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1974BR37 Nucl.Phys. A235, 190 (1974)

P.Braun-Munzinger, H.L.Harney, S.Wenneis

Numerical Calculation of Recoil Effects for Surface Reactions

NUCLEAR REACTIONS ¹²C(¹⁴N, ¹³N), E=78, 100, 150 MeV; calculated σ(E(¹³N), θ). ¹⁴⁴Sm(¹⁶O, ¹⁴C), E=104 MeV; calculated σ(E(¹⁴C), θ).

doi: 10.1016/0375-9474(74)90185-7
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1974GE01 Nucl.Phys. A219, 253 (1974)

C.K.Gelbke, G.Baur, R.Bock, P.Braun-Munzinger, W.Grochulski, H.L.Harney, R.Stock

Interference between Inelastic Scattering and Transfer in the Scattering of ¹⁶O on ¹⁷O

NUCLEAR REACTIONS ¹⁷O(¹⁶O, ¹⁶O'), E(lab)=22, 24, 28, 32 MeV; measured σ(θ), for θ(cm)=129° measured σ(E); enriched targets.

doi: 10.1016/0375-9474(74)90065-7
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1974HA45 Z.Phys. 269, 339 (1974)

H.L.Harney, P.Braun-Munzinger, C.K.Gelbke

On the Semiclassical Interpretation of Heavy Ion Reactions

NUCLEAR REACTIONS ⁶⁴Ni(¹⁶O, ¹⁶O), E=56 MeV; ⁴⁸Ca(¹⁴N, ¹⁴N), E=50 MeV; ³²S(¹⁶O, ¹⁶O), E=45 MeV; calculated deflection functions.

doi: 10.1007/BF01668605
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1974MA12 Phys.Rev. C9, 1694 (1974)

J.A.Macdonald, J.Cerny, J.C.Hardy, H.L.Harney, A.D.Bacher, G.R.Plattner

Analyzing Powers for Two-Nucleon Transfer Reactions in the 1p Shell

NUCLEAR REACTIONS ¹⁶O, ¹⁵N(p, t), (p, ³He), E=43.8 MeV; ¹³C(p, t), (p, ³He), E=49.6 MeV; measured σ(Et, E(³He), θ), A(θ). ¹⁴O, ^13,14N, ^11,13C, ¹¹B deduced levels, L.

doi: 10.1103/PhysRevC.9.1694
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1973BR25 Phys.Rev.Lett. 31, 1423 (1973)

P.Braun-Munzinger, W.Bohne, C.K.Gelbke, W.Grochulski, H.L.Harney, H.Oeschler

Strongly Oscillating Angular Distributions in the Reaction ³²S(¹⁶O, ¹²C)³⁶Ar at E(c.m.) = 30 MeV

NUCLEAR REACTIONS ³²S(¹⁶O, ¹²C), (¹⁶O, ¹⁶O), E=45 MeV; measured σ(θ). ³⁶Ar deduced transitions.

doi: 10.1103/PhysRevLett.31.1423
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1973RO21 Phys.Rev. C8, 153 (1973)

D.Robson, A.Richter, H.L.Harney

Consequences of Isospin and Other Conserved Quantum Numbers for Compound-Nucleus Reactions

NUCLEAR REACTIONS ⁵⁴Cr(p, p), (p, α); measured nothing, calculated level-width, d, p-width, α-width, t.

doi: 10.1103/PhysRevC.8.153
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1973WI06 Phys.Rev.Lett. 30, 866 (1973)

K.H.Wilcox, N.A.Jelley, G.J.Wozniak, R.B.Weisenmiller, H.L.Harney, J.Cerny

New Spectroscopic Measurements via Exotic Nuclear Rearrangement; the Reaction ²⁶Mg(⁷Li, ⁸B)²⁵Ne

NUCLEAR REACTIONS ²⁶Mg(⁷Li, ⁸B), E=79 MeV; measured σ(E(⁸B)), Q. ²⁵Ne deduced levels.

doi: 10.1103/PhysRevLett.30.866
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1972BA32 Nucl.Phys. A184, 641 (1972)

D.Bachelier, M.Bernas, H.L.Harney, J.C.Jourdain, P.Radvanyi, M.Roy-Stephan

Charge Symmetry in the Mirror Reactions ³H(d, ³He)2n and ³He(d, t)2p At 83 MeV

NUCLEAR REACTIONS ³H, ³He(d, ³He), (d, t), E=83 MeV; measured σ(E(3He), θ), σ(Et, θ); analysed final-state interactions; deduced n-n scattering parameters. Enriched targets.

doi: 10.1016/0375-9474(72)90435-6
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1972BA89 Nucl.Phys. A195, 361 (1972)

D.Bachelier, M.Bernas, J.L.Boyard, H.L.Harney, J.C.Jourdain, P.Radvanyi, M.Roy-Stephan

Exchange Effect in the 166 MeV α-Particle Elastic Scattering on ⁶Li

NUCLEAR REACTIONS ⁶Li(α, α), Eα=166 MeV; measured angular distribution σ(θ); analysed pick-up contribution. Enriched target.

doi: 10.1016/0375-9474(72)91064-0
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1972WO10 Phys.Rev.Lett. 28, 1278 (1972); Erratum Phys.Rev.Lett. 29, 760 (1972)

G.J.Wozniak, H.L.Harney, K.H.Wilcox, J.Cerny

α-Particle Transfer via the (¹²C, ⁸Be) Reaction: Application to Studies of ¹⁶O and ²⁰Ne

NUCLEAR REACTIONS ¹²C(¹²C, ⁸Be), ¹⁶O(¹²C, ⁸Be), E=62.6 MeV; measured σ(E(⁸Be)). ¹⁶O, ²⁰Ne deduced levels.

doi: 10.1103/PhysRevLett.28.1278
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1971CL02 Nucl.Phys. A161, 49 (1971)

R.G.Clarkson, P.von Brentano, H.L.Harney

Reduced Widths from Isobaric Analog Resonance

NUCLEAR STRUCTURE ²⁰⁹Bi, ¹³⁹La, ¹⁴¹Pr; calculated isobaric analog resonance widths.

doi: 10.1016/0375-9474(71)90319-8
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1970HA13 Nucl.Phys. A145, 282 (1970)

H.L.Harney, P.von Brentano, E.Grosse, J.L.Escudie, J.C.Faivre, P.Foissel, J.Gosset, B.Mayer, L.Papineau

Analog Resonances and Polarization

NUCLEAR REACTIONS ²⁰⁸Pb(p, p'), E=14.85-15.05 MeV; measured polarization analyzing power Ap(E;Ep', θ). Enriched target.

doi: 10.1016/0375-9474(70)90319-2
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1970HA26 Phys.Rev. C2, 421 (1970)

H.L.Harney, A.Richter

Comment on the Number of Degrees of Freedom in Fluctuation Analysis

NUCLEAR REACTIONS ²⁷Al(α, p), E=6.3 MeV; ³¹P(d, α), E=9.5 MeV; calculated number of⁰ of freedom.

doi: 10.1103/PhysRevC.2.421
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1969ER04 Nucl.Phys. A136, 87 (1969)

J.Ernst, H.L.Harney, K.Kotajima

A Statistical Model Analysis of Fluctuations in the Elastic and Inelastic Proton Scattering on ⁵⁴Cr and ⁵⁶Fe

NUCLEAR REACTIONS ⁵⁴Cr(p, p), (p, p'), (p, α), E = 9.30-10.11 MeV; ⁵⁶Fe(p, p), (p, p'), E = 9.00-11.90 MeV; measured σ(E;Ep', θ), σ(E;Eα, θ). ⁵⁵Mn, ⁵⁷Co deduced level-width, mean level spacings, auto-correlations; compound nucleus cross sections, cross correlations. Enriched, natural targets.

doi: 10.1016/0375-9474(69)90041-4
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1969HE13 Nucl.Phys. A135, 591 (1969)

A.Heusler, H.L.Harney, J.P.Wurm

Structure of Generalized Neutron Particle-Hole States in ¹⁴⁰Ce

NUCLEAR STRUCTURE ¹⁴⁰Ce; calculated neutron particle - hole states.

doi: 10.1016/0375-9474(69)90007-4
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1968HA02 Phys.Letters 26B, 204 (1968)

H.L.Harney, C.A.Wiedner, J.P.Wurm

Spectroscopic Factors from Isobaric Analog Resonances in Elastic Proton Scattering

doi: 10.1016/0370-2693(68)90341-9
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