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Search: Author = H.L.Harney

Found 49 matches.

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2010DI05      Phys.Lett. B 685, 263 (2010)

B.Dietz, H.L.Harney, A.Richter, F.Schafer, H.A.Weidenmuller

Cross-section fluctuations in chaotic scattering

doi: 10.1016/j.physletb.2010.01.074
Citations: PlumX Metrics


2004AB01      Phys.Lett. B 579, 278 (2004)

A.Y.Abul-Magd, H.L.Harney, M.H.Simbel, H.A.Weidenmuller

Statistics of 2+ levels in even-even nuclei

doi: 10.1016/j.physletb.2003.07.092
Citations: PlumX Metrics


2001KL13      Mod.Phys.Lett. A 16, 2409 (2001)

H.V.Klapdor-Kleingrothaus, A.Dietz, H.L.Harney, I.V.Krivosheina

Evidence for Neutrinoless Double Beta Decay

RADIOACTIVITY 76Ge(2β-); analyzed data; deduced 0ν-accompanied 2β-decay T1/2, neutrino effective mass.


2000BA66      Phys.Rev. E 62, 1936 (2000)

C.I.Barbosa, T.Guhr, H.L.Harney

Impact of Isospin Breaking on the Distribution of Transition Probabilities

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1692.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1779.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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