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93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 (1993). Nuclear Structure: 208 Pb; calculated giant resonance partial decay width. Continuum RPA.

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Page 1: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma01 Partial Decay Widths from Giant Resonances in 208Pb

E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 (1993).

Nuclear Structure: 208Pb; calculated giant resonance partial decay width. Continuum RPA.

Page 2: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma02 First Evidence for States in Hg Nuclei with Deformations between Normal and Super Deformation

W. C. Ma, J. H. Hamilton, A. V. Ramayya, L. Chaturvedi, J. K. Deng, W. B. Gao, Y. R. Jiang, J. Kormicki, X. W. Zhao, N. R.Johnson, J. D. Garrett, I. Y. Lee, C. Baktash, F. K. McGowan, W. Nazarewicz, R. Wyss, Phys. Rev. C47, R5 (1993).

Nuclear Reactions: 154Gd(36S,4n), E=159-175 MeV; measured γγ-coin. 186Hg deduced levels, J, π, T1/2, deformation betweennormal and superdeformed, configuration, Iγ, quadrupole moments.

Page 3: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma03 Core Polarization Effect on the Discrete Proton Hole States of 205Tl

R. Majumdar, Phys. Rev. C47, 178 (1993).

Nuclear Structure: 205Tl; calculated proton hole state distribution; deduced core polarization role. Hole-core vibrational scheme,208Pb(p,α) data input.

Page 4: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma04 Curium Fission Cross-Section Analysis

V. M. Maslov, Ann. Nucl. Energy 20, 163 (1993).

Nuclear Reactions: 242, 243, 244, 245, 246, 247, 248Cm(n,F), E ≤ 20 MeV; calculated fission σ(E).

Page 5: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma05 Investigation of Pion Absorption in Heavy-Ion Induced Subthreshold π0 Production

R. S. Mayer, W. Henning, R. Holzmann, R. S. Simon, H. Delagrange, F. Lefevre, T. Matulewicz, R. Merrouch, W. Mittig, R. W.Ostendorf, Y. Schutz, F. D. Berg, W. Kuhn, V. Metag, R. Novotny, M. Pfeiffer, A. L. Boonstra, H. Lohner, L. B. Venema, H.W. Wilschut, D. Ardouin, H. Dabrowski, B. Erazmus, C. Lebrun, L. Sezac, F. Ballester, E. Casal, J. Diaz, J. L. Ferrero, M.Marques, G. Martinez, H. Nifenecker, B. Fornal, L. Freindl, Z. Sujkowski, Phys. Rev. Lett. 70, 904 (1993).

Nuclear Reactions: 197Au(129Xe,xπ0), E=44 MeV/nucleon; measured σ(θ(π)). Optical model.

Page 6: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma06 Cross Section for Excitation of Nuclear Isomers in (γ,γ’)(m) Reactions at 4-15 MeV

V. M. Mazur, I. V. Sokolyuk, Z. M. Bigan, I. Yu. Kobal, Yad. Fiz. 56, No 1, 20 (1993); Phys. Atomic Nuclei 56, 10 (1993).

Nuclear Reactions: 77Se, 79Br, 87Sr, 111Cd, 115In, 137Ba(γ,γ’), E=4-15 MeV; measured σ(E), isomer excitation; deduced σ(iso-mer)/σ ratio energy dependence. Other data analyzed. Statistical model.

Page 7: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma07 Components of Collective Flow and Azimuthal Distribution in 40Ar + 27Al Collision with BUU Method

Y. Ma, W. Shen, J. Feng, Y. Ma, Z. Phys. A344, 469 (1993).

Nuclear Reactions: 27Al(40Ar,X), E=20=80 MeV/nucleon; calculated in-plane, out-of-plane collective flow components, flowangles vs E, proton azimuthal distribution. BUU simulation.

Page 8: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma08 Deformation Dependence of Low Lying M1 Strengths in Even Nd Isotopes

J. Margraf, R. D. Heil, U. Kneissl, U. Maier, H. H. Pitz, H. Friedrichs, S. Lindenstruth, B. Schlitt, C. Wesselborg, P. von Bren-tano, R. -D. Herzberg, A. Zilges, Phys. Rev. C47, 1474 (1993).

Nuclear Reactions: 146Nd(γ,γ’), E 4 MeV; measured γ linear polarization, azimuthal asymmetry. 142, 146, 148, 150Nd levelsdeduced B(λ), J, π, Γ, deformation dependence of M1 transition strengths.

Page 9: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma09 Studying the 16O + 12C Dynamic Polarization Potential by Inversion

R. S. Mackintosh, S. G. Cooper, Phys. Rev. C47, 1716 (1993).

Nuclear Reactions: 12C(16O,16O), E=168-311 MeV; calculated σ(θ); deduced dynamic polarization features. Coupled-channels,continuum discretized coupled-channels S-matricies, S(l)-V(r) inversion.

Page 10: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma10 Towards a New Understanding of the Low-Energy Excitations in the Even-Even Nuclei

H. Mach, B. Fogelberg, M. Hellstrom, D. Jerrestam, L. Spanier, Acta Phys. Pol. B24, 71 (1993).

Nuclear Structure: A 100; A 150; 132Sn; compiled, reviewed data; deduced low excitation levels features.

Page 11: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma11 E(*) and I Selection Techniques for Hot Nuclei Studies

A. Maj, J. J. Gaardhoje, Z. Zelazny, A. Bracco, F. Camera, M. Matiuzzi, B. Million, M. Pignanelli, Acta Phys. Pol. B24, 429(1993).

Nuclear Reactions: 114Cd(48Ti,X), E=225 MeV; measured Iγ(θ) for 162Yb decay; deduced hot nuclei GDR decay, width features.

Page 12: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma12 Microscopic Origin of Quantum Chaos in Rotational Dampling

M. Matsuo, T. Dossing, E. Vigezzi, R. A. Broglia, Phys. Rev. Lett. 70, 2694 (1993).

Nuclear Structure: 168Yb; calculated rotational spectrum; deduced order to chaos transition, rotational damping association.Cranked shell model, effective interaction.

Page 13: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma13 Comment on ’ Early Stages of Nucleus-Nucleus Collisions: A microscopic calculation of the inital number of degrees of free-dom ’

Y. Ma, W. Shen, J. Feng, Y. Ma, Phys. Rev. Lett. 70, 2972 (1993).

Nuclear Structure: A ≤ 200; analyzed 16O, 32S, 58Ni induced reactions on these targets. Initial number of degrees of freedom,nucleus-nucleus collision at early stages.

Page 14: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma14 Effect of Isospin on Three Nucleon Pion Absorption in Light Nuclei

A. Mateos, N. Simicevic, Phys. Rev. C47, R1842 (1993).

Nuclear Reactions: 4, 3He(π+,X), (π-,X), E=120, 165 MeV; 7, 6Li(π+,X), E=50-180 MeV; analyzed pion absorption data; deducedmechanism for absorption on three-nucleons. Isospin based model.

Page 15: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma15 Theoretical Treatment of Analog (p,n) Cross Sections for Odd Nuclei: Application to measurements of 105Pd at 26 MeV

V. A. Madsen, R. W. Bauer, J. D. Anderson, V. R. Brown, B. A. Pohl, C. H. Poppe, S. Stamer, E. Mordhorst, W. Scobel, S. M.Grimes, Phys. Rev. C47, 2077 (1993).

Nuclear Reactions: 105Pd(p,n), E=26 MeV; measured σ(θ), neutron spectra. 105Ag deduced IAS excitation mechanism. Modelcomparison.

Page 16: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma16 Global Properties of Proton-Hole Strengths in Mass 54 to 70 Nuclei

G. Mairle, M. Seeger, M. Ermer, P. Grabmayr, A. Mondry, G. J. Wagner, Phys. Rev. C47, 2113 (1993).

Nuclear Reactions: 66Zn(polarized d,3He), E=52 MeV; measured σ(θ), iT11(θ); deduced model parameters. 65Cu deduced levels,

J, π, C2S.

Nuclear Structure: 54, 56, 58Fe, 58, 60, 62, 64Ni, 64, 66Zn, 70Ge; calculated proton Fermi surface parameters.

Page 17: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma17 A Novel Path to Study the Total Reaction Cross Sections

Y. G. Ma, W. Q. Shen, J. Feng, Y. Q. Ma, Phys. Lett. 302B, 386 (1993).

Nuclear Reactions: 12C(12C,X), (11Li,X), E ≤ 1 GeV/ nucleon; calculated reaction σ vs E. Reaction dynamics framework.

Page 18: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma18 Scaling of Measured Nuclear Spin-Orbit Splittings

G. Mairle, Phys. Lett. 304B, 39 (1993).

Nuclear Structure: 12C, 16O, 40, 48Ca, 90Zr, 116Sn, 140Ce, 144Sm, 208Pb; A ≤ 200; analyzed proton-, neutron spin-orbit splittings;deduced scaling.

Page 19: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma19 The Proton Strength Distribution of the 1g9/2 State of 41Sc

R. Majumdar, Z. Phys. A345, 293 (1993).

Nuclear Structure: 41Sc; calculated 1g9/2 proton state strength distribution. Core-particle coupling model.

Page 20: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma20 Superdeformed State of the Rotating Nucleus 151Dy(N = 85)

N. Mansour, Yad. Fiz. 56, No 4, 3 (1993); Phys. Atomic Nuclei 56, 423 (1993).

Nuclear Reactions: 122Sn(35Cl,X), E=167 MeV/nucleon; measured Eγ, Iγ, γγ-coin. 151Dy deduced levels, J, π, superdeformedband. Comparison with other nuclei. The following note was published in Yad. Fiz. 56, No12 (1993) by the Editorial Board ofYadernaya Fizika in regard to this article: ’ Attention Readers: In Vol. 56, No. 4 of our journal for 1993 there was an article by N.Mansour entitled ’ Superdeformed state of the rotating nucleus 151Dy (N = 85) ’, a major part of which, without any refrences,contains experimentatal data of G. -E. Rathke et al., given in a paper entitled ’ A superdeformed band in 151Dy ’, published in1988 (Phys.Lett.B 209, 177 (1988)). The editorial board offers its apologies to the authors of that paper for the damage it mightcause and to the readers who were misled by this publication ’. The article by G. -E. Rathke et al., referred to has the <KEYNO>88Ra19 in the NSR file.

Page 21: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma21 Measurement of the Magnetic Form Factor of the Neutron

P. Markowitz, J. M. Finn, B. D. Anderson, H. Arenhovel, A. R. Baldwin, D. Barkhuff, K. B. Beard, W. Bertozzi, J. M. Cameron,C. C. Chang, G. W. Dodson, K. Dow, T. Eden, M. Farkhondeh, B. Flanders, C. Hyde-Wright, W. -D. Jiang, D. Keane, J. J.Kelly, W. Korsch, S. Kowalski, R. Lourie, R. Madey, D. M. Manley, J. Mougey, B. Ni, T. Payerle, P. Pella, T. Reichelt, P. M.Rutt, M. Spraker, D. Tieger, W. Turchinetz, P. E. Ulmer, S. Van Verst, J. W. Watson, L. B. Weinstein, R. R. Whitney, W. M.Zhang, Phys. Rev. C48, R5 (1993).

Nuclear Reactions: 2H(e,e’n), E not given; measured en-coin. 1n deduced magnetic form factor. Associated particle technique.

Page 22: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma22 40Ca(p,d)39Ca Reaction at 65 MeV

M. Matoba, O. Iwamoto, Y. Uozumi, T. Sakae, N. Koori, T. Fujiki, H. Ohgaki, H. Ijiri, T. Maki, M. Nakano, Phys. Rev. C48,95 (1993).

Nuclear Reactions: 40Ca(polarized p,d), E=65 MeV; measured σ(θ), analyzed power vs θ. 39Ca deduced levels, J, π, C2S.DWBA analysis.

Page 23: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma23 Mass and Charge Distributions of Cl-Induced Heavy-Ion Reactions

A. A. Marchetti, A. C. Mignerey, H. Madani, A. Gokmen, W. L. Kehoe, B. Libby, K. Morley, H. Breuer, K. Wolf, F. Obenshain,Phys. Rev. C48, 266 (1993).

Nuclear Reactions: 40Ca, 209Bi(37Cl,X), E=7.3 MeV/nucleon; 209Bi(35Cl,X), E=15 MeV/nucleon; measured fragment mass,charge distributions; deduced charge, mass centroids drifts.

Page 24: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma24 Improved Microscopic Calculation of Initial Exciton Number

Y. G. Ma, W. Q. Shen, J. Feng, Y. Q. Ma, Phys. Rev. C48, 448 (1993).

Nuclear Structure: A=24-200; analyzed (16O,X), (32S,X), (58Ni, X) data on targets; deduced initial exciton number. Improvedmicroscopic calculations.

Page 25: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma25 Study of the Total Reaction Cross Section via the Reaction Dynamical Model

Y. G. Ma, W. Q. Shen, J. Feng, Y. Q. Ma, Phys. Rev. C48, 850 (1993).

Nuclear Reactions: 12C(11Li,X), (11Be,X), 27Al(11Be, X), E < 1 GeV/nucleon; calculated reaction σ(E). Transport theory plusGlauber theory, optical limit.

Page 26: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma26 Beta Decay of 44V

G. Martinez-Pinedo, A. Poves, Phys. Rev. C48, 937 (1993).

Radioactivity: 44V(β+); calculated ground state, isomer decay Gamow-Teller transition strength function, T1/ 2.

Nuclear Structure: 44Sc, 44Ti; calculated levels. 41, 42, 43Sc, 42Ti; calculated Gamow-Teller transition strength function.

Page 27: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma27 Chaotic Behavior in Warm Deformed Nuclei Induced by Residual Two-Body Interactions

M. Matsuo, T. Dossing, B. Herskind, S. Frauendorf, E. Vigezzi, R. A. Broglia, Nucl. Phys. A557, 211c (1993).

Nuclear Structure: 168Yb; calculated band mixing; deduced rotational damping chaotic behavior causes.

Page 28: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma28 Neutron Capture and Total Cross Sections of 144Sm

R. L. Macklin, N. W. Hill, J. A. Harvey, G. L. Tweed, Phys. Rev. C48, 1120 (1993).

Nuclear Reactions: 144Sm(n,n), (n,γ), E=0.5 eV to 500 keV; measured σ(E); deduced Maxwellian average capture, capture reso-nance integral. 145Sm deduced s-, p-wave resonances, parameters gΓ(n), Γγ, L, J, average properties.

Page 29: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma29 Deconvolution of Mass Spectra

A. A. Marchetti, A. C. Mignerey, Nucl. Instrum. Methods Phys. Res. A324, 288 (1993)

Nuclear Reactions: 238U(64Ni,X), E=8.3 MeV/nucleon; analyzed fragment spectra data; deduced deconvolution technique advan-tages.

Page 30: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma30 Response of BGO Detectors to Photons of 3-50 MeV Energy

T. Matulewicz, W. Henning, H. Emling, R. Freifelder, H. Grein, E. Grosse, N. Herrmann, R. Holzmann, R. Kulessa, R. S.Simon, H. J. Wollersheim, B. Schoch, J. Vogt, M. Wilhelm, J. V. Kratz, R. Schmidt, R. V. F. Janssens, Nucl. Instrum. MethodsPhys. Res. A325, 216 (1993)

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93Ma31 Quenching of Scintillation in BaF2 for Light Charged Particles

T. Matulewicz, Nucl. Instrum. Methods Phys. Res. A325, 365 (1993)

Page 32: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma32 Multiquark Cluster Effect in a Three-Body System

W. -H. Ma, Q. Wu, L. S. Kisslinger, Nucl. Phys. A560, 997 (1993).

Nuclear Structure: 3He; calculated charge density; deduced multi-quark cluster effect role. Hybrid quark-hadron model.

Page 33: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma33 Neutron Emission Cross Sections at Low Bombarding Energies and the Novelty in Multistep Compound Reaction Model

A. Marcinkowski, J. Rapaport, R. W. Finlay, C. Brient, M. Herman, M. B. Chadwick, Nucl. Phys. A561, 387 (1993).

Nuclear Reactions: 165Ho, 181Ta(n,xn), E=6.7, 20 MeV; measured σ(E(n),θ); deduced reaction mechanism. Modified statisticalmultistep model analysis.

Page 34: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma34 On the Field Theoretical Approach to the Nucleon-Nucleon Scattering Problem in the Low-Energy Region

A. I. Machavariani, A. J. Chelidze, J. Phys. (London) G19, 1285 (1993).

Page 35: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma35 Absorption Mechanisms in Photon Induced Two-Body Knockout

L. Machenil, M. Vanderhaeghen, J. Ryckebusch, M. Waroquier, Phys. Lett. 316B, 17 (1993).

Nuclear Reactions: ICPND 16O(γ,np), (γ,2p), E=60-300 MeV; calculated σ(E), σ(θp,θn) vs proton momentum; deduced heavymeson exchange, intermediate ∆ creation roles.

Page 36: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma36 Temporal Nonlocality of Nuclear and Atomic Mean Fields

C. Mahaux, G. R. Satchler, Nucl. Phys. A560, 5 (1993).

Nuclear Reactions: 208Pb(n,n), E=-10 to 60 MeV; calculated optical potential components behavior, system self energy; deducedtemporary nonlocality features. Complex mean field.

Page 37: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma37 Components of Collective Flow Produced in 40Ar + 27Al Collision with BUU Method

Y. Ma, W. Shen, J. Feng, Chin. J. Nucl. Phys. 15, No 1, 27 (1993).

Nuclear Reactions: 27Al(40Ar,X), E=45-120 MeV/nucleon; calculated collective flow longitudinal, transverse components;deduced in-plane collective flow energy dependence. BUU simulation.

Page 38: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma38 Rotational Behavior in Intermediate Energy Heavy Ion Collisions

Y. G. Ma, W. Q. Shen, J. Feng, Y. Q. Ma, Phys. Rev. C48, R1492 (1993).

Nuclear Reactions: 27Al(40Ar,X), E=45 MeV/nucleon; calculated σ(φp); deduced midrapidity rotational behavior impact parameterdependence.

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93Ma39 Level Structure of the Odd Mass Pr Isotopes. III. Levels of 147Pr88 Populated in the Beta Decay of 56-s 147Ce

P. F. Mantica, J. D. Robertson, E. M. Baum, W. B. Walters, Phys. Rev. C48, 1579 (1993).

Radioactivity: 147Ce(β-); measured Eγ, Iγ, γγ-coin, I(ce). 147Pr deduced levels, J, π, γ-multipolarity, ICC. Model comparison.

Nuclear Structure: 142, 144, 146, 148Ce, 144, 146, 148, 150Nd; calculated total routhian surface plots. 145, 149Pr; calculated levels.147Pr; calculated levels, B(λ), ratios. Particle plus triaxial rotor model.

Page 40: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma40 Approximate Particle Number Projection for Rotating Nuclei

P. Magierski, S. Cwiok, J. Dobaczewski, W. Nazarewicz, Phys. Rev. C48, 1686 (1993).

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93Ma41 Role of Nuclear Compressibility on the Fission Path

M. M. Majumdar, J. N. De, C. Samanta, S. K. Samaddar, Phys. Rev. C48, 2093 (1993).

Nuclear Structure: 238U, 208Pb; calculated equilibrium density along fission path, deformation energy, volume, Coulomb, surfacecontributions; deduced nuclear compressibility role. Semi-macroscopic framework.

Page 42: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma42 Poisson and Porter-Thomas Fluctuations in Off-Yrast Rotational Transitions

M. Matsuo, T. Dossing, B. Herskind, S. Frauendorf, Nucl. Phys. A564, 345 (1993).

Nuclear Structure: 168Yb; calculated levels, density, E2 transition strength fluctuations. Cranked shell model.

Page 43: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma43 Rotation-Like Behavior as a Function of Projectile Energy and Target Mass

Y. Ma, W. Shen, J. Feng, Y. Ma, Z. Phys. A346, 285 (1993).

Nuclear Reactions: 197Au, V, Zn, Ag, Sm, U, 27Al(40Ar, X), E < 85 MeV/nucleon; calculated σ(fragment φ); deduced rotationalcollective motion evidence. Transport theory.

Page 44: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma44 Summary of the Small-x Sub-Group

A. D. Martin, J. Phys. (London) G19, 1603 (1993).

Nuclear Structure: 1H; analyzed ep-deep inelastic scattering data, structure function features.

Page 45: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma45 Electron-Induced Reactions on the Deuteron

L. Mathelitsch, Czech. J. Phys. B43, 363 (1993).

Nuclear Reactions: 2H(e,e), (e,e’), (polarized e,e), (polarized e,e’), E=140, 500 MeV; compiled, reviewed σ(θ), polarizationobservables data, analyses; deduced tensor force role, pion nucleon coupling related features.

Page 46: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma46 Hyperfine Quenching of the 1s22s2p63s3p3P0 Level in Magnesium-Like Ions

J. P. Marques, F. Parente, P. Indelicato, At. Data Nucl. Data Tables 55, 157 (1993).

Nuclear Moments: =14-92; calculated hyperfine interaction role in levels separation energy. Magnesium-like ions, multi-configuration Dirac-Fock approach.

Page 47: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma47 Elastic p-4He Scattering at Intermediate Energies

S. I. Manayenkov, Yad. Fiz. 56, No 10, 126 (1993); Phys. Atomic Nuclei 56, 1525 (1993).

Nuclear Reactions: 4He(p,p), E=695-991 MeV; calculated σ(θ). Corrections to Glauber theory.

Page 48: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma48 (3He,6Li) Reaction on 9Be, 12C, and 13C Nuclei

Yu. G. Mashkarov, E. I. Koshchy, I. I. Zalyubovsky, N. T. Burtebaev, A. D. Duisebaev, V. V. Adodin, A. T. Rudchik, Bull. Rus.Acad. Sci. Phys. 57, 889 (1993).

Nuclear Reactions: 9Be, 12, 13C(3He,6Li), E=60 MeV; 9Be(3He,3He), E=60 MeV; measured σ(θ); deduced model parameters.9Be, 12, 13C deduced 3H-pickup spectroscopic factors. Distorted waves, finite size interaction radius, recoil effects. Shell modelcomparison.

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93Ma49 Isomeric States in Nuclei

V. E. Makarenko, G. B. Yankov, Yad. Fiz. 56, No 12, 1 (1993); Phys. Atomic Nuclei 56, 1617 (1993).

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93Ma50 The Distribution of Proton-Hole Strengths in the (2s, 1d)-Shell of 35Cl, 37Cl and 39Cl

G. Mairle, M. Seeger, H. Reinhardt, T. Kihm, K. T. Knopfle, C. L. Wen, Nucl. Phys. A565, 543 (1993).

Nuclear Reactions: 36, 38, 40Ar(polarized d,3He), E=52 MeV; measured σ(θ), iT11(θ). 35, 37, 39Cl deduced levels, J, π, spectros-

copic factors, proton occupancies, single-particle energies, spreading widths. 39Cl deduced mass excess. Enriched 36, 38Ar gastargets. DWBA analysis.

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93Ma51 Proton Knockout from 16O and Relativistic Recoil Effects in the Dirac Impulse Approximation

O. V. Maxwell, E. D. Cooper, Nucl. Phys. A565, 740 (1993).

Nuclear Reactions: 16O(polarized p,2p), E=200 MeV; analyzed σ(θ1, θ2,E2), analyzing power data; deduced bound statemomentum distribution, elastic distorting potentials dependences. Dirac impulse approximation, relativistic recoil effects.

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93Ma52 L1 Fluorescence Yield of Yb abd Ir

M. I. Marques, M. C. Martins, F. Parente, J. G. Ferreira, J. Phys. (London) B26, 1263 (1993).

Radioactivity: 170Tm(β-), (EC); 191Os(β-); measured L X-ray-, K X-ray-, γ-spectra; deduced L1 fluorescence yield in Yb, Ir.

Page 53: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma53 Experimental and Theoretical Considerations on the Calibration Factor K between α-Activity Concentration and Track Densityfor Application in Radon Dosimetry

A. F. Maged, T. Tsuruta, S. A. Durrani, J. Radioanal. Nucl. Chem. 170, 423 (1993).

Radioactivity: 222Rn(α); measured Eα, Iα; deduced detector calibration factor K. Solid state nuclear track detectors.

Page 54: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma54 Reactions Induced by 150-350 keV Deuterons on 12C and 13C

D. R. Maxson, A. T. Sornborger, Nucl. Instrum. Methods Phys. Res. B79, 293 (1993)

Nuclear Reactions: ICPND 12C(d,p), 13C(d,p), (d,α), E=0.15-0.35 MeV; measured σ(θ); deduced astrophysical S-factors.

Page 55: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma55 Laser Optical Pumping of Potassium in a High Magnetic Field using Linearly Polarized Light

C. Martin, T. Walker, L. W. Anderson, D. R. Swenson, Nucl. Instrum. Methods Phys. Res. A335, 233 (1993)

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93Ma56 Hyperfine Structure and Isotope Shift of the 3s-3p Transitions of Atomic Oxygen

F. Marin, C. Fort, M. Prevedelli, M. Inguscio, G. M. Tino, J. Bauche, Z. Phys. D25, 191 (1993).

Nuclear Moments: +16}, 17, 18O; measured hfs, isotope shifts; deduced modified, normal, specific mass shifts. High resolutionsaturation spectroscopy.

Page 57: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma57 An Improved Microscopic Method for Calculating Initial Exciton Number

Y. Ma, W. Shen, J. Feng, Chin. Phys. Lett. 10, 93 (1993).

Nuclear Structure: A=30-200; calculated initial exciton number. Microscopic method.

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93Ma58 An Investigation into the Total Reaction Cross Section and Production Cross Section of Energetic Particles

Y. Ma, W. Shen, J. Feng, Y. Ma, Chin. Phys. Lett. 10, 464 (1993).

Nuclear Reactions: 12C(12C,X), E 0.02-1 GeV/nucleon; calculated reaction σ(E). 12C(12C, xπ), E 100-800 MeV/nucleon; calcu-lated total pion production σ(E). Transport theory.

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93Ma59 Energy and Target Dependence of Azimuthal Distributions at Mid-Rapidity in Mediate-Energy Nuclear Reactions

Y. Ma, W. Shen, J. Feng, Chin. Phys. Lett. 10, 660 (1993).

Nuclear Reactions: 27Al(40Ar,X), E=36-85 MeV/nucleon; analyzed mid-rapidity azimuthal distribution vs impact parameter, pro-jectile energy; deduced collective motion energy, impact parameter dependence.

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93Ma60 Meson Production Studied with the GEM Detector

H. Machner, A. Budzanowski, P. Cloth, H. Dabrowski, A. Djaloeis, M. Drochner, V. Druke, J. Ernst, W. Erven, D. Filges, D.Frekers, D. Grzonka, J. Holzer, St. Igel, R. Jahn, L. Jarczyk, K. Kilian, J. Konin, T. Kutsarova, M. Kystrin, B. J. Lieb, W. Meil-ing, H. P. Morsch, Ch. Nake, H. S. Plendl, D. Protic, G. Riepe, E. Roderburg, P. von Rossen, R. Schwierz, J. Smyrski, A.Strzalkowski, P. Turek, K. H. Watzlawik, K. Zwoll, and the GEM Collaboration, Acta Phys. Pol. B24, 1555 (1993).

Nuclear Reactions: 2H(p,π0), (p,X), E not given; compiled, reviewed π0, eta production σ data, analyses. 2H(p,X), E=903.4,1091.6 MeV; measured missing mass spectra. Ge wall plus magnetic spectrometer. Other aspects discussed.

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93Ma61 Low- and Intermediate-Energy Pion-Nucleus Interactions in the Cascade-Exciton Model

S. G. Mashnik, Acta Phys. Pol. B24, 1685 (1993).

Nuclear Reactions: Cu(π+,pX), (π-,pX), E at 1000 GeV/ c; C, 27Al, Ni, Ta(π+,pX), E=100 MeV; 64Ni(p,π+X), (p,π-X), E=201 MeV;analyzed data; deduced different pion absorption, particle production mechanisms contributions. Cascade-exciton model.

Page 62: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma62 Measuring Neutron Lifetime by Storing Ultracold Neutrons and Detecting Inelastically Scattered Neutrons

W. Mampe, L. N. Bondarenko, V. I. Morozov, Yu. N. Panin, A. I. Fomin, Pisma Zh. Eksp. Teor. Fiz. 57, 77 (1993); JETP Lett.(USSR) 57, 82 (1993).

Radioactivity: 1n(β-); measured T1/2. Ultra cold neutrons, simultaneous detection of neutrons scattered by storage vessel.

Page 63: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma63 A Review of Hypernuclear Spectroscopy: Problems, progress, prospects

L. Majling, R. A. Eramzhyan, Bull. Rus. Acad. Sci. Phys. 57, 1661 (1993).

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93Ma64 Anharmonic γ-Vibrations in a Simple Nuclear Model

E. R. Marshalek, R. G. Nazmitdinov, I. Ragnarsson, Bull. Rus. Acad. Sci. Phys. 57, 1709 (1993).

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93Ma65 Mossbauer Spectroscopic Study of FeAl(1-x)Co(x)

S. H. Mahmood, M. A. Gharaibeh, H. Abu-Safia, A. S. Saleh, Hyperfine Interactions 77, 255 (1993).

Nuclear Reactions: 57Fe(γ,γ), E=14.4 keV; measured Mossbauer spectra; deduced alloy system magnetic splitting, averagehyperfine field vs temperature. Alloys system FeAl(1-x)Co(x).

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93Ma66 TDPAC Measurements with Highly Oriented Pyrolytic Graphite Using the 19F(p,p’)19F(*) and 19F(α,n)22Na(*) Reactions

P. W. Martin, D. Surono, F. -J. Hambsch, H. Postma, P. Rietveld, Hyperfine Interactions 77, 315 (1993).

Nuclear Reactions: 19F(p,p’), E resonance; 19F(α, n), E=3.42 MeV; measured γ(θ,H,t); deduced quadrupole interactions for 19F,22Na levels, highly oriented pyrolytic host material.

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93Ma67 Beta-NMR Detection of Beta-Emitting Fragment 43Ti

K. Matsuta, A. Ozawa, Y. Nojiri, T. Minamisono, M. Fukuda, S. Momota, T. Ohtsubo, S. Fukuda, K. Sugimoto, I. Tanihata, K.Yoshida, K. Omata, J. R. Alonso, G. F. Krebs, T. J. M. Symons, Hyperfine Interactions 78, 123 (1993).

Radioactivity: 43Ti(β+) [from C(46Ti,X), E 116 MeV/nucleon]; measured β-NMR in Pt; deduced µ, meson exchange, configurationmixing effects role.

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93Ma68 Fragment Polarization of 43Tl in the 46Ti + C Collision

K. Matsuta, A. Ozawa, Y. Nojiri, T. Minamisono, M. Fukuda, S. Momota, T. Ohtsubo, S. Fukuda, K. Sugimoto, I. Tanihata, K.Yoshida, K. Omata, J. R. Alonso, G. F. Krebs, T. J. M. Symons, Hyperfine Interactions 78, 127 (1993).

Nuclear Reactions: C(46Ti,X), E=116 MeV/nucleon; measured projectile fragmentation, 43Ti fragment spin polarization; deducedreaction mechanism. Beta asymmetry technique.

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93Ma69 PAC Measurements of In-Pt Intermetallic Compounds

M. Marszalek, B. Wodniecka, P. Wodniecki, A. Z. Hrynkiewicz, Hyperfine Interactions 80, 1029 (1993).

Radioactivity: 111In(EC); measured γγ(θ,H,t); deduced 111Cd quadrupole interaction parameters in In-Pt intermetallic compounds.

Page 70: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma70 57Fe Mossbauer Spectra and Spin-Crossover Behavior of [Fe(mbpN)(lut)]BPh4

Y. Maeda, Y. Noda, H. Oshio, Y. Takashima, Hyperfine Interactions 80, 1099 (1993).

Nuclear Reactions: 57Fe(γ,γ), E=14.4 keV; measured Mossbauer spectra; deduced [Fe(mbpN)(1ut)]BPh4 spin-crossoverbehavior.

Page 71: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma71 129I and 125Te Mossbauer Studies of Polyvinyl Alcohol Films Doped with Iodine

Y. Maeda, M. Seto, T. Matsuyama, H. Yamaoka, H. Sakai, Hyperfine Interactions 80, 1103 (1993).

Nuclear Reactions: 125Te(γ,γ), E=35.46 keV; measured not given; deduced Iodine-PVA complex structural arrangement.129Xe(γ,γ), E=39.57 keV; measured Mossbauer spectra. Emission Mossbauer spectroscopy, 125, 129I sources.

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93Ma72 Production of Unstable Nuclei Far from the Stability Line: Its scope and limitations

K. Matsuta, A. Ozawa, Y. Nojiri, T. Minamisono, M. Fukuda, S. Momota, T. Ohtsubo, S. Fukuda, K. Sugimoto, I. Tanihata, K.Yoshida, K. Omata, J. R. Alonso, G. F. Krebs, T. J. M. Symons, Hyperfine Interactions 80, 1219 (1993).

Radioactivity: 20, 21F(β-); 37, 39Ca(β+); compiled, reviewed T1/2 data. 43Ti(β-); compiled, reviewed µ, T1/2 data. Production andstudy of unstable nuclei.

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93Ma73 Nuclear Data Sheets Update for A = 207

M. J. Martin, Nucl. Data Sheets 70, 315 (1993).

Compilation: 207Hg, 207Tl, 207Pb, 207Bi, 207Po, 207At, 207Rn, 207Fr, 207Ra; compiled, evaluated structure data.

Page 74: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma74 High Resolution Measurement for Photoabsorption Cross Sections in the Autoionization Regions of Ar, Kr and Xe

K. Maeda, K. Ueda, K. Ito, J. Phys. (London) B26, 1541 (1993).

Atomic Physics: r, Kr, Xe(γ,X), E not given; measured photoabsorption σ.

Page 75: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma75 Neutrino Cross Sections and the Small Atmospheric ν(µ)/ν(e) Ratio

A. K. Mann, Phys. Rev. D48, 422 (1993).

Nuclear Reactions: 16O(ν,ν), E ≤ 2000 MeV; calculated σ(E); deduced ν(µ)/ν(e) ratio implications.

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93Ma76 Calculation on a Personal Computer of Partial and Total X- and γ-Ray Interaction Cross Sections

O. S. Marenkov, At. Energ. 75, 481 (1993); Sov. At. Energy 75, 974 (1993).

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93Ma77 Formulas for Calculating the Integral Incoherent-Scattering Cross Sections for X- and γ-Rays in Hydrogen and Helium

O. S. Marenkov, At. Energ. 75, 486 (1993); Sov. At. Energy 75, 981 (1993).

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93Ma78 NMR Study of Y2(Co(1-x)T(x))14B(T = Mn, Fe,Ni) Compounds

F. Maruyama, H. Nagai, K. Adachi, J. Phys. Soc. Jpn. 62, 3741 (1993).

Nuclear Moments: +59}Co; measured NMR; deduced anisotropy change, hyperfine fields relationship, Y2(Co(1-x)T(x))B, T=Mn,Fe, Ni magnetic properties.

Page 79: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Ma79 Nuclear Data Sheets for A = 175

A. O. Macchiavelli, E. Browne, Nucl. Data Sheets 69, 903 (1993).

Compilation: 175Tm, 175Yb, 175Lu, 175Hf, 175Ta, 175W, 175Re, 175Os, 175Ir, 175Pt, 175Au, 175Hg; compiled, evaluated structure dta.

Page 80: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93MaZK Correspondence Interpretation of the Low-Lying Bands in the Neutron-Rich Sm and Gd Nuclei

H. Mach, M. Hellstrom, B. Fogelberg, D. Jerrestam, L. Spanier, Proc. 6th Intern. Conf. on Nuclei Far from Stability + 9th Intern.Conf. on Atomic Masses and Fundamental Constants, Bernkastel-Kues, Germany, 19-24 July, 1992, R. Neugart, A. Wohr,Eds., p. 715 (1993)

Radioactivity: 152Pm(β-); measured βγγ(t). 152Sm levels deduced T1/2, B(λ), 0+ → 0+ transition rates. Model comparison.

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93MaZL Lifetime Measurements in 118, 120Xe

P. F. Mantica, P. K. Joshi, S. J. Robinson, E. F. Zganjar, R. L. Gill, W. B. Walters, D. Rupnik, H. K. Carter, J. Kormicki, C. R.Bingham, Proc. 6th Intern. Conf. on Nuclei Far from Stability + 9th Intern. Conf. on Atomic Masses and Fundamental Constants,Bernkastel-Kues, Germany, 19-24 July, 1992, R. Neugart, A. Wohr, Eds., p. 667 (1993)

Radioactivity: 118, 120Cs(β+), (EC) [from 92Mo(32S, X), E=175 MeV]; measured βγ-coin, time-to-amplitude conversion. 118, 120Xelevel deduced B(E2), mean T1/2.

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93MaZM The Evidence for Production of the Superheavy Element with Z = 112 via Secondary and Direct Heavy-Ion Reactions

A. Marinov, S. Gelberg, D. Kolb, Proc. 6th Intern. Conf. on Nuclei Far from Stability + 9th Intern. Conf. on Atomic Masses andFundamental Constants, Bernkastel-Kues, Germany, 19-24 July, 1992, R. Neugart, A. Wohr, Eds., p. 437 (1993)

Nuclear Reactions: ICPND 184W(88Sr,X), E=5.1 MeV/nucleon; measured (particle)(X-ray)-, (particle)(particle)-coin; deduced evi-dence for 271, 272112. 184W(88Sr, X), E(cm)=245-285 MeV; calculated fusion σ(E).

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93MaZN NMR on Beta-Emitting Fragment 43Ti

K. Matsuta, A. Ozawa, Y. Nojiri, T. Minamisono, M. Fukuda, S. Momota, T. Ohtsubo, S. Fukuda, K. Sugimoto, I. Tanihata, A.Yoshida, K. Omata, J. R. Alonso, G. F. Krebs, T. J. M. Symons, Proc. 6th Intern. Conf. on Nuclei Far from Stability + 9th Intern.Conf. on Atomic Masses and Fundamental Constants, Bernkastel-Kues, Germany, 19-24 July, 1992, R. Neugart, A. Wohr,Eds., p. 229 (1993)

Radioactivity: 43Ti(β+) [from C(46Ti,X), E=116 MeV/nucleon]; measured β-decay asymmetry, NMR; deduced µ, meson exchangecurrents role.

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93MaZO Ground State Properties of Exotic Nuclei in a Relativistic Point Coupling Model

D. G. Madland, T. Hoch, B. A. Nikolaus, P. Manakos, Proc. 6th Intern. Conf. on Nuclei Far from Stability + 9th Intern. Conf. onAtomic Masses and Fundamental Constants, Bernkastel-Kues, Germany, 19-24 July, 1992, R. Neugart, A. Wohr, Eds., p. 97(1993)

Nuclear Structure: 70Ca, 48, 78Ni, 100Sn, 164Pb; calculated binding energy, charge, nucleon rms radii. Relativistic Hartree approxi-mations.

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93MaZP Partial Decay Widths from the Giant Monopole Resonance in 208Pb

E. Maglione, R. J. Liotta, T. Vertse, ATOMKI 1992 Ann. Rept., p. 42 (1993).

Nuclear Structure: 208Pb; calculated giant monopole resonance partial decay widths. Continuum RPA.

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93MaZQ CDCC Analysis for 22 MeV Deuteron Elastic Scattering from 52Cr and 206Pb

M. Masaki, S. Nakagawa, K. Katoh, N. Nakamoto, Y. Mukouhara, H. Kishita, Y. Tagishi, Y. Aoki, Univ. Tsukuba, TandemAccel. Center, Ann. Rept., 1992, p. 25 (1993).

Nuclear Reactions: 52Cr, 206Pb(polarized d,d), (polarized d,p), E=22 MeV; analyzed σ(θ), T20, T21, iT11, T22. CDCC analysis.

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93MaZR A New Method of Elastic S-Matrix Estimation

M. Masaki, Y. Aoki, Univ. Tsukuba, Tandem Accel. Center, Ann. Rept., 1992, p. 20 (1993).

Nuclear Reactions: Sn, 197Au, U(α,α), E=24.7 MeV; 148, 154Sm(α,α), E=50 MeV; 40Ca, 206Pb(d, d), E=22 MeV; calculated elasticS-matrices, σ. Proposed a new method to estimate the elastic S matrix.

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93MaZS Production and Identification of Projectile-Like Fragments in 24Mg + Pt Reaction at 9.7A MeV

K. Matsuta, S. Fukuda, T. Izumikawa, M. Tanigaki, M. Fukuda, T. Ohtsubo, Y. Nojiri, T. Minamisono, J. R. Alonso, G. F.Krebs, R. J. McDonald, T. J. M. Symons, Osaka Univ. Lab. Nucl. Studies, Ann. Rept., 1992, p. 75 (1993).

Nuclear Reactions: Pt(24Mg,X), E=9.7 MeV/nucleon; measured β-spectra; deduced 23Mg σ(θ). E-∆E telescope.

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93MaZT NMR-Line Width of 12B in Pt Detected by β-NMR

K. Matsuda, T. Araki, M. Mori, T. Ohtsubo, M. Fukuda, K. Matsuta, Y. Nojiri, T. Minamisono, Osaka Univ. Lab. Nucl. Studies,Ann. Rept., 1992, p. 50 (1993).

Radioactivity: 12B(β-); measured NMR-line widths. β-NMR method.

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93MaZU Beta-Ray Angular Distribution from Nuclear Spin Polarized 12N

K. Matsuda, T. Araki, M. Mori, M. Fukuda, K. Matsuta, Y. Nojiri, T. Minamisono, Osaka Univ. Lab. Nucl. Studies, Ann. Rept.,1992, p. 47 (1993).

Nuclear Moments: +12}N(β+) [from 10B(3He,n), E=3 MeV]; measured β(E,θ) from spin polarized 12N implanted in Al; deducedpolarization correlation coefficient. β-NMR method.

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93MaZV Decay Properties of 245Cf

M. Magara, N. Shinohara, K. Tsukada, Y. Hatsukawa, S. -I. Ichikawa, Y. Nagame, M. Oshima, Japan Atomic Energy Res. Inst.Tandem VDG Ann. Rept., 1992, p. 86 (1993).

Radioactivity: 245Cf(α), (EC), (β+) [from U(12C, xn), E=76 MeV]; measured Eγ, Eα, αγ-, (X-ray)γ-coin. 241Cm deduced levels, J, π.245Bk deduced transition Eγ.

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93MaZW Spin Polarization of 43Ti Fragment from 116 A MeV 46Ti Beam

K. Matsuta, A. Ozawa, T. Minamisono, Y. Nojiri, M. Fukuda, A. Kitagawa, T. Ohtsubo, S. Momota, S. Fukuda, K. Sugimoto, I.Tanihata, K. Yoshida, K. Omata, J. R. Alonso, G. F. Krebs, T. J. M. Symons, RIKEN-92, p. 27 (1993).

Radioactivity: 43Ti(β+) [from 197Au, 12C(46Ti, 43Ti), E=116 MeV/nucleon]; measured β-ray asymmetry; deduced source spin polari-zation.

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93MaZX Elastic and Inelastic Scattering of Polarized 7Li from 208Pb at 33 MeV

I. Martel-Bravo, C. O. Blyth, N. M. Clarke, P. R. Dee, B. R. Fulton, J. A. R. Griffith, S. J. Hall, N. Keeley, K. Rusek, G. Tun-gate, N. J. Davis, K. A. Connell, J. S. Lilley, M. W. Bailey, J. Gomez-Camacho, Daresbury Lab., 1992-1993 Ann. Rept., Appen-dix, p. 56 (1993).

Nuclear Reactions: 208Pb(polarized 7Li,7Li), (polarized 7Li,7Li’), E=33 MeV; measured σ(θ), T20(θ). Coupled-channels analysis.

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93MaZY Inelastic Proton Scattering from 40Ca at 200 MeV

B. C. Markham, L. C. Bland, D. S. Carman, P. Li, P. Schwandt, T. Gu, H. Breuer, N. S. Chant, J. Huffman, M. Khayat, P. G.Roos, B. S. Flanders, G. M. Huber, Bull. Am. Phys. Soc. 38, No. 2, 1052, N7 6 (1993)

Nuclear Reactions: 40Ca(polarized p,p’), E=200 MeV; measured σ(θ), analyzing power, polarization observables vs θ. Inclusive,(p,2p) reactions included.

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93MaZZ Compton Scattering from the Proton from 68 to 150 MeV

B. MacGibbon, G. Garino, A. Nathan, G. Feldman, B. Dolbilkin, Bull. Am. Phys. Soc. 38, No. 2, 915, A7 3 (1993)

Nuclear Reactions: 1H(γ,γ), E=100-150 MeV bremsstrahlung; deduced σ(θ); deduced electric, magnetic polarizabilities role.

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93Mc01 Elastic-Scattering Phenomenology by Inversion: (I). 12C + 12C from 140 to 2400 MeV

M. A. McEwan, S. G. Cooper, R. S. Mackintosh, Nucl. Phys. A552, 401 (1993).

Nuclear Reactions: 12C(12C,12C), E=0.14-2.4 GeV; calculated σ(θ); deduced potential parameters. Local internuclear potential,two-step procedure.

Page 97: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Mc02 Isospin Effects in the Photodisintegration of Light Nuclei

K. G. McNeill, M. N. Thompson, A. D. Bates, J. W. Jury, B. L. Berman, Phys. Rev. C47, 1108 (1993).

Nuclear Reactions: 13, 14C, 15N, 17, 18O, 25, 26Mg, 29, 30Si(γ,p), (γ,n), (γ,2n), E < 36 MeV; analyzed σ(E); deduced isospin com-ponent splitting.

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93Mc03 Isomeric Decay Studies using a Recoil Mass Separator. Exotic N = 82 and 83 Nuclei 153Yb, 153Lu, 154Lu and 154Hf

J. H. McNeill, A. A. Chishti, P. J. Daly, W. Gelletly, M. A. C. Hotchkis, M. Piiparinen, B. J. Varley, P. J. Woods, J. Blomqvist, Z.Phys. A344, 369 (1993).

Nuclear Reactions: 102Pd(54Fe,X), E=245 MeV; measured γ(recoil)-, γγ-coin. 153Yb, 153, 154Lu deduced isomer decay, levels, J,π, B(λ), transition Iγ, configuration. 154Hf deduced levels, J, π, configuration.

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93Mc04 np-Elastic Analyzing Power A(N0) and Spin Transfer K(NN)

M. W. McNaughton, K. Johnston, D. R. Swenson, D. Tupa, R. L. York, D. A. Ambrose, P. Coffey, K. H. McNaughton, P. J.Riley, G. Glass, J. C. Hiebert, R. H. Jeppesen, H. Spinka, I. Supek, G. E. Tripard, H. Woolverton, Phys. Rev. C48, 256(1993).

Nuclear Reactions: 1H(polarized n,n), E=485-788 MeV; measured analyzing power, spin transfer parameter.

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93Mc05 1266-keV Gamma Branch in 31Si Decay

S. C. McGuire, T. Z. Hossain, R. J. Soave, Phys. Rev. C48, 1434 (1993).

Radioactivity: 31Si(β-) [from 30Si(n,γ), E=thermal]; measured Eγ, Iγ, γ(t), T1/ 2. 31P transition deduced Iγ.

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93Mc06 The Faure Cylotron Neutron Source and a Particle Spectrometer for Neutron Induced Emission of Charged Particles at Ener-gies between 60 and 200 MeV

W. R. McMurray, D. G. Aschman, K. Bharuth-Ram, R. W. Fearick, Nucl. Instrum. Methods Phys. Res. A329, 217 (1993)

Nuclear Reactions: 12C(n,p), (n,d), E=64 MeV; measured p-, d-spectra; deduced system particle identification capabilities. Faurecyclotron neutron source, particle spectrometer.

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93Mc07 Coulomb Excitation of States in 232Th

F. K. McGowan, W. T. Milner, Nucl. Phys. A562, 241 (1993).

Nuclear Reactions: 232Th(α,α’γ), E=18 MeV; measured Iγ, Eγ, γ(θ) following Coulomb excitation. 232Th deduced levels, B(λ), J,π, δ.

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93Mc08 Analyzing Power in nd Elastic Scattering at E(n)(lab) = 3 MeV. Measurement and Calculation

J. E. McAninch, W. Haeberli, H. Witala, W. Glockle, J. Golak, Phys. Lett. 307B, 13 (1993).

Nuclear Reactions: 2H(polarized n,n), E < breakup threshold; measured analyzing power vs θ; deduced charge independencebreaking component in NN-interaction role. Rigorous 3-body calculations.

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93Mc09 Thermal Calorimeters for High Resolution X-Ray Spectroscopy

D. McCammon, W. Cui, M. Juda, J. Morgenthaler, J. Zhang, R. L. Kelley, S. S. Holt, G. M. Madejski, S. H. Moseley, A. E.Szymkowiak, Nucl. Instrum. Methods Phys. Res. A326, 157 (1993)

Radioactivity: 55Fe(EC); measured K X-ray spectra. Thermal calorimeters, high resolution.

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93Me01 High Momentum Transfer R(T,L) Response Functions for 3, 4He

Z. -E. Meziani, J. P. Chen, D. Beck, G. Boyd, L. M. Chinitz, D. B. Day, L. C. Dennis, G. E. Dodge, B. W. Filippone, K. L.Giovanetti, J. Jourdan, K. W. Kemper, T. Koh, W. Lorenzon, J. S. McCarthy, R. D. McKeown, R. G. Milner, R. C. Minehart, J.Morgenstern, J. Mougey, D. H. Potterveld, O. A. Rondon-Aramayo, R. M. Sealock, I. Sick, L. C. Smith, S. T. Thornton, R. C.Walker, C. Woodward, Nucl. Phys. A553, 701c (1993).

Nuclear Reactions: 3, 4He(e,e’X), E=0.9-4.3 GeV; measured inclusive σ; deduced longitudinal, transverse response functions,Coulomb sum rule saturation.

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93Me02 Evidence for a Nuclear Halo from 11Li Elastic Scattering Measured at 637 MeV Incident Energy on a 12C Target

M. C. Mermaz, Phys. Rev. C47, 2213 (1993).

Nuclear Reactions: 12C(11Li,11Li), E=637 MeV; 12C(11C, 11C), E=620 MeV; analyzed σ(θ); deduced model parameters. 11Lideduced halo evidence.

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93Me03 Quasifree Pion Production in the Three-Nucleon System

H. O. Meyer, J. A. Niskanen, Phys. Rev. C47, R2474 (1993).

Nuclear Reactions: 1n(p,π0), 2H(p,pπ0), E not given; calculated σ; deduced quasifree process role in pd → pdπ0.

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93Me04 Energy Dependence of the Angular Distributions of the New Resonance Seen in 12C(12C,12C(0+2))12C(0+

2)

A. C. Merchant, W. D. M. Rae, J. Phys. (London) G19, L89 (1993).

Nuclear Reactions: 12C(12C,12C’), E(cm) 32-36 MeV; analyzed σ(θ). 24Mg deduced resonance features.

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93Me05 Investigation of a Technique for Calculating Energy-Independent Effective Interactions

M. R. Meder, S. W. Walker, B. R. Caldwell, Nucl. Phys. A556, 228 (1993).

Nuclear Structure: 2, 3H, 4He; calculated binding energy; deduced effective interaction characteristics.

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93Me06 Polarization Transfer in (p(pol),n(pol)) Reactions at 318 and 494 MeV and the Effective Interaction

D. J. Mercer, T. N. Taddeucci, L. J. Rybarcyk, X. Y. Chen, D. L. Prout, R. C. Byrd, J. B. McClelland, W. C. Sailor, S. DeLucia,B. Luther, D. G. Marchlenski, E. Sugarbaker, E. Gulmez, C. A. Whitten, Jr., C. D. Goodman, J. Rapaport, Phys. Rev. Lett. 71,684 (1993).

Nuclear Reactions: 2H, 12, 14C(polarized p,n), E=318, 494 MeV; measured polarization transfer observable; deduced mediumeffects modification to effective interaction.

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93Me07 Pion Production Near Threshold

H. O. Meyer, Phys. Scr. 48, 54 (1993).

Nuclear Reactions: 1H(p,pπ0), E=325 MeV; 2H(p,pπ0), E not given; analyzed data; deduced quasifree pion production role.

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93Me08 Distorted-Wave Calculation of the (p,p’π+) Reaction

R. Mehrem, J. T. Londergan, G. E. Walker, Phys. Rev. C48, 1192 (1993).

Nuclear Reactions: 16O(p,p’π+), E(cm)=450, 800 MeV; calculated σ(θ(π),θ(p’),E’). Two-nucleon model.

Page 113: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Me09 Electrodisintegration of Polarized Deuterons

Yu. P. Melnik, A. V. Shebeko, Phys. Rev. C48, 1259 (1993).

Nuclear Reactions: 2H(e,e’p), E not given; calculated vector, tensor asymmetries following target disintegration. Polarized tar-get.

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93Me10 The 9Be(d,n) Thick-Target Neutron Spectra for Deuteron Energies between 2.6 and 7.0 MeV

J. W. Meadows, Nucl. Instrum. Methods Phys. Res. A324, 239 (1993)

Nuclear Reactions: 9Be(d,n), E=2.6-7 MeV; measured thick target neutron spectra. Tof techniques, 235, 238U fisssion ionchambers.

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93Me11 Determination of the On-Target Polarization of an Optically-Pumped Polarized Lithium Ion Beam

A. J. Mendez, E. G. Myers, K. W. Kemper, P. L. Kerr, E. L. Reber, B. G. Schmidt, Nucl. Instrum. Methods Phys. Res. A329, 37(1993)

Nuclear Reactions: 12C(polarized 6Li,α), E=33 MeV; measured σ(Eα), on-target t20(θ) for beam. Optically pumped polarizedlithium ion source.

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93Me12 Dipole Cascades in 194Pb

D. Mehta, W. Korten, H. Hubel, K. Theine, W. Schmitz, P. Willsau, C. X. Yang, F. Hannachi, D. B. Fossan, H. Grawe, H.Kluge, K. H. Maier, Z. Phys. A346, 169 (1993).

Nuclear Reactions: 158Gd(40Ar,4n), E=178 MeV; measured γγ-coin, Iγ. 194Pb deduced levels, J, π, γ-multipolarity, B(λ) ratios.

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93Me13 Excited States in Neutron-Deficient Iridium Nuclei Populated in Radioactive Decays of 177-181Pt

F. Meissner, H. Salewski, W. -D. Schmidt-Ott, U. Bosch-Wicke, V. Kunze, R. Michaelsen, Phys. Rev. C48, 2089 (1993).

Radioactivity: 177, 178, 179, 180, 181Pt(β+) [from 146, 148Nd(36Ar,xn), E=172-201 MeV]; measured T1/2, Eγ, Iγ, γγ-coin. 177, 179, 181Irdeduced levels, J, π. Enriched targets, Ge(Li) detectors, He-jet.

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93Me14 Geometry, Scaling, and Universality in the Mass Distributions in Heavy Ion Collisions

A. Z. Mekjian, S. J. Lee, Phys. Rev. C48, 2999 (1993).

Nuclear Reactions: Cu, Ta, 197Au, Ag(p,X), E ≤ 29 GeV; calculated fragment mass distributions, cluster, charge distributions.Exactly soluble canonical ensemble model.

Page 119: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Me15 SU(6) Configuration Mixing and the Spin Asymmetry of the Neutron

D. I. Melikhov, Yad. Fiz. 56, No 12, 205 (1993); Phys. Atomic Nuclei 56, 1741 (1993).

Nuclear Structure: 1n; calculated spin asymmetry; deduced role of SU(6) mixing in wave function. SU(6) configuration mixing.

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93Me16 L-Shell X-Ray Production Cross Sections for 29Cu, 31Ga, 32Ge, 35Br, 39Y, 60Nd, 64Gd, 67Ho, 70Yb, 79Au, and 82Pb for 2-25 MeVCarbon Ions

R. Mehta, J. L. Duggan, F. D. McDaniel, M. R. McNeir, Y. C. Yu, D. K. Marble, G. Lapicki, Nucl. Instrum. Methods Phys. Res.B79, 175 (1993)

Nuclear Reactions: Cu, Ga, Ge, Br, 89Y, Nd, Gd, 165Ho, Yb, 197Au, Pb(C,X), E=2-25 MeV; measured L X-ray production σ;deduced Si(Li) detector efficiency. Multiple normalization techniques.

Atomic Physics: u, Ga, Ge, Br, 89Y, Nd, Gd, 165Ho, Yb, 197Au, Pb(C,X), E=2-25 MeV; measured L X-ray production σ; deducedSi(Li) detector efficiency. Multiple normalization techniques.

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93Me17 Elementary Amplitudes in the Multiple Diffraction Theory of pp and (p-bar)p Elastic Scattering

M. J. Menon, Phys. Rev. D48, 2007 (1993); Erratum Phys. Rev. D51, 1427 (1995).

Nuclear Reactions: 1H(p,p), (p-bar,p-bar), E=high; analyzed data; deduced models parton-parton amplitudes comparison. Multi-ple diffraction theory, other data analyses input.

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93Me18 Isoscalar Giant Resonances in 58Ni, 64Ni, and 120Sn Nuclei at Inelastic Scattering of α-Particles with the Energy of about 100MeV

V. I. Medvedev, Yu. N. Pavlenko, V. M. Pugach, Bull. Rus. Acad. Sci. Phys. 57, 759 (1993).

Nuclear Reactions: 58, 64Ni, 120Sn(α,α’), E=97.3 MeV; measured σ(θ,Eα). 58, 64Ni, 120Sn deduced giant resonance parameters.

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93Me19 From NN → NNπ to Pion Production in Nuclei

H. O. Meyer, Acta Phys. Pol. B24, 1735 (1993).

Nuclear Reactions: 1, 2H(p,pπ0), E < 425 MeV; compiled, reviewed σ(E), other data; deduced medium modification on pion pro-duction, axial current enhancement evidence.

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93Me20 The ICEBall: A Multiple element array for in-beam internal conversion electron spectroscopy

M. P. Metlay, J. X. Saladin, I. Y. Lee, O. Dietzsch, Nucl. Instrum. Methods Phys. Res. A336, 162 (1993)

Radioactivity: 207Bi(EC), (β+); 133Ba(EC); measured I(ce); deduced device efficiency. Multiple-element mini-orange spectrome-ter.

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93MeZW An Experimental Approach to Nuclear Cosmochronology

K. A. Mezilev, Yu. N. Novikov, A. V. Popov, Yu. Ya. Sergeev, V. I. Tikhonov, Proc. 6th Intern. Conf. on Nuclei Far from Stability+ 9th Intern. Conf. on Atomic Masses and Fundamental Constants, Bernkastel-Kues, Germany, 19-24 July, 1992, R. Neugart,A. Wohr, Eds., p. 875 (1993)

Radioactivity: 226, 228, 230, 232Fr, 232, 234Ac, 233, 234Ra(β-) [from Th, U(p,X), E=1 GeV]; measured X-ray, β-, γ-spectra; deduced β-delayed fission probability for 230, 232, 228Fr, 232, 234Ac, Q(β) for 226Fr, 232, 234Ac. A=227-234; compiled, reviewed T1/2 data, calcu-lations.

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93MeZX Directional Polarization of h11/2 Proton Pair in the 14966Dy83 Ground State from a Study of Its Gammow-Teller Decay

W. Meczynski, K. Zuber, R. Broda, R. Menegazzo, P. Kleinheinz, M. C. Bosca, P. Paris, C. F. Liang, J. Blomqvist, Proc. 6thIntern. Conf. on Nuclei Far from Stability + 9th Intern. Conf. on Atomic Masses and Fundamental Constants, Bernkastel-Kues,Germany, 19-24 July, 1992, R. Neugart, A. Wohr, Eds., p. 695 (1993)

Radioactivity: 149Dy(β+), (EC) [from Gd(3He, xn), E=240 MeV]; measured Eγ, Iγ, γγ-coin, I(ce); deduced Gamow-Teller transitionstrength. 149Tb deduced levels, possible J, π, band structure. 149Dy level deduced configuration.

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93MeZY Investigation of I(ce) Spectrum in 57Fe

R. Ya. Metskhvarishvili, Z. N. Miminoshvili, M. A. Elizbarashvili, L. V. Nekrasova, N. M. Marchilashvili, I. V. Zhorzholiani, Pro-gram and Thesis, Proc. 43rd Ann. Conf. Nucl. Spectrosc. Struct. At. Nuclei, Dubna, p. 51 (1993).

Radioactivity: 57Co(EC); measured I(ce). 57Fe deduced ICC ratios. Magnetic β-spectrometer.

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93MeZZ

F. Meissner, Priv. Comm. (1993).

Radioactivity: 177Pt(β+), (EC), (α) [from 146Nd(36Ar, X)]; measured T1/2. 173Os, 177Ir deduced transitions.

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93Mi01 Multiple Nucleon Emission from 232Th following Intermediate-Energy Photon Excitation

G. J. Miller, J. C. McGeorge, I. Anthony, R. O. Owens, D. Ryckbosch, Nucl. Phys. A551, 135 (1993).

Nuclear Reactions: ICPND 232Th(γ,xnyp), E=40-150 MeV bremsstrahlung; measured reaction yields; deduced partial σ(E).Activation technique. Virtual photon analysis, pre-equilibrium decay models.

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93Mi02 Strong Impact Parameter Dependence of Hard Photon Production in Intermediate Energy Heavy Ion Collisions

E. Migneco, C. Agodi, R. Alba, G. Bellia, R. Coniglione, A. Del Zoppo, P. Finocchiaro, C. Maiolino, P. Piattelli, G. Russo, P.Sapienza, A. Badala, R. Barbera, A. Palmeri, G. S. Pappalardo, F. Riggi, A. C. Russo, A. Peghaire, A. Bonasera, Phys. Lett.298B, 46 (1993).

Nuclear Reactions: 197Au(129Xe,X), E=44 MeV/nucleon; measured light charged particle production, γ production probability vsparticle multiplicity; deduced impact parameter role.

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93Mi03 Parity-Violating Muon and Heavy Lepton Scattering in the 12C → 12C(*) Nuclear Transition

S. L. Mintz, M. Pourkaviani, Phys. Rev. C47, 873 (1993).

Nuclear Reactions: 12C(polarized µ,µ’), E not given; calculated asymmetry vs lepton energy.

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93Mi04 Complete Spectroscopy of 90Y via the 89Y(n, γ) and 89Y(d(pol),p) Reactions

S. Michaelsen, A. Harder, K. P. Lieb, G. Graw, R. Hertenberger, D. Hofer, P. Schiemenz, E. Zanotti, H. Lenske, A. Weigel, H.H. Wolter, S. J. Robinson, A. P. Williams, Nucl. Phys. A552, 232 (1993).

Nuclear Reactions: 89Y(n,γ), E=thermal; measured Eγ, Iγ. 89Y(polarized d,p), E=22 MeV; measured σ(θ), vector analyzing powerA(y)(θ). 90Y deduced levels, J, π, neutron binding energy, level density. Comparison with shell model, RPA calculations.

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93Mi05 Measurement of the Analyzing Power Components in Photodisintegration of the Polarized Deuteron

S. I. Mishnev, D. M. Nikolenko, S. G. Popov, I. A. Rachek, A. B. Temnykh, D. K. Toporkov, E. P. Tsentalovich, B. B.Woitsekhowski, S. L. Belostotsky, V. V. Nelyubin, V. V. Sulimov, V. N. Stibunov, Phys. Lett. 302B, 23 (1993).

Nuclear Reactions: 2H(e,e’), E not given; measured vector analyzing power components following disintegration. Polarized tar-get. Model comparison.

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93Mi06 Anomalies in the Scattering of p-Wave Neutrons by Tellurium Nuclei

L. V. Mitsina, G. S. Samosvat, Yad. Fiz. 56, No 2, 23 (1993); Phys. Atomic Nuclei 56, 159 (1993).

Nuclear Reactions: 128, 130Te(n,n), E ≤ 300 keV; measured σ(θ). 129, 131Te deduced p-wave strength function, scattering radii,resonance parameters, doorway formation.

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93Mi07 A Rotational Band in 82Zr

S. Mitarai, T. Kuroyanagi, A. Odahara, J. Mukai, H. Tomura, S. Suematsu, D. Jerrestam, J. Nyberg, G. Sletten, A. Atac, N.Gjorup, J. Jongman, S. E. Arnell, H. A. Roth, O. Skeppstedt, Z. Phys. A344, 405 (1993).

Nuclear Reactions: 58Ni(28Si,2n2p), E=128 MeV; measured γγ-coin. 82Zr deduced levels, J, π, band structure.

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93Mi08 Mass-Measurements of Exotic Nuclei

W. Mittig, Nucl. Phys. A553, 473c (1993).

Nuclear Reactions: 9Be(13C,12N), E=336 MeV; compiled, reviewed this and other reaction data; deduced status of exotic nucleimass determination.

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93Mi09 Quadrupole Moment of the Doubly-Closed-Shell-Plus-One-Nucleon Nucleus 41Sc and Its Core Deformation

T. Minamisono, S. Fukuda, T. Ohtsubo, A. Kitagawa, Y. Nakayama, Y. Someda, S. Takeda, M. Fukuda, K. Matsuta, Y. Nojiri,Nucl. Phys. A559, 239 (1993).

Radioactivity: 41Sc(β+) [from 40Ca(d,n), E=4.1 MeV]; measured β asymmetry; deduced quadrupole moment. Recoil polarization,β-NMR technique, asymmetric β-distribution method.

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93Mi10 Octupole Correlations in Superdeformed High-Spin States

S. Mizutori, T. Nakatsukasa, K. Arita, Y. R. Shimizu, K. Matsuyanagi, Nucl. Phys. A557, 125c (1993).

Nuclear Structure: 158, 156, 154, 152, 150, 148, 146, 144, 142Gd, 184, 186, 188, 190, 192, 194, 196, 198, 200Hg; calculated curvature againstoctupole deformation, stretched octupole strengths; deduced octupole instability, superdeformed shape relationship.

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93Mi11 Band Structures of Nuclei Around N, Z = 40 Selected by Charged Particle Detection

S. Mitarai, T. Kuroyanagi, A. Odahara, J. Mukai, H. Tomura, S. Suematsu, T. Morikawa, D. Jerrestam, J. Nyberg, G. Sletten,A. Atac, M. Piiparinen, S. E. Arnell, D. Foltescu, H. A. Roth, O. Skeppstedt, Nucl. Phys. A557, 381c (1993).

Nuclear Reactions: 58Ni(28Si,4p), E=128 MeV; 58Ni(32S, 4p), E=125 MeV; measured relative yield with respect to 1p, 2p, 3p exitchannels. 58Ni(28Si, pα), E=100 MeV; 58Ni(32S,p2α), (32S, pα), E=120, 125 MeV; measured γγ-, pα-coin. 85Nb, 81Y deduced lev-els, J, π, yrast band dynamic moment of inertia. 58Ni(28Si, 2n2p), E=128 MeV; measured γ(particle)-coin. 82Zr deduced levels, J,π. 58Ni(32S,2n2p), E=125 MeV; measured γγ-coin. 86Mo deduced possible yrast level transtions.

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93Mi12 Nuclear Data Sheets Update for A = 126

K. Miyano, Nucl. Data Sheets 69, 429 (1993).

Compilation: 126Cd, 126In, 126Sn, 126Sb, 126Te, 126I, 126Xe, 126Cs, 126Ba, 126La, 126Ce, 126Pr; compiled, evaluated structure data.

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93Mi13 Precise Measurement of γ-Ray Emission Probabilities for 66Cu

H. Miyahara, K. Hara, C. Mori, Y. Kasugai, K. Kawade, Nucl. Instrum. Methods Phys. Res. A324, 219 (1993)

Radioactivity: 66Cu(β-) [from 65Cu(n,γ), E=thermal]; measured Eγ, Iγ, βγ-coin. 66Zn levels deduced γ-emission probabilities.

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93Mi14 Cryogenic Thermal Detector with LiF Absorber for Direct Dark Matter Search Experiment

M. Minowa, M. Sakamoto, Y. Ito, T. Watanabe, W. Ootani, Y. Ootuka, Nucl. Instrum. Methods Phys. Res. A327, 612 (1993)

Radioactivity: 241Am(α); measured Eγ, Iγ. Cryogenic thermal detector with LiF absorber.

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93Mi15 Mass Dependence of Pion Production in Heavy Ion Collisions Near, But Below Threshold

J. Miller, G. F. Krebs, J. Panetta, L. S. Schroeder, P. N. Kirk, Z. -F. Wang, W. Bauer, W. Benenson, D. Cebra, M. Cronqvist,B. -A. Li, R. Pfaff, T. Reposeur, J. Stevenson, A. Vander Molen, G. Westfall, J. S. Winfield, B. Young, T. Murakami, T. Suzuki,I. Tanihata, Phys. Lett. 314B, 7 (1993).

Nuclear Reactions: 139La(139La,X), 197Au(197Au, X), E=183, 236 MeV/nucleon; measured π- inclusive production σ vs E(π),charged particle multiplicity, beam energy; deduced pion production mechanism.

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93Mi16 Level and Width Statistics for a Decaying Chaotic System

S. Mizutori, V. G. Zelevinsky, Z. Phys. A346, 1 (1993).

Nuclear Structure: N=2-160; calculated levels, widths, correlations. Decaying chaotic systems.

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93Mi17 Inclusive Fragment Production in 84Kr + 197Au at E/A = 35 MeV

U. Milkau, M. L. Begemann-Blaich, E. -M. Eckert, G. Imme, P. Kreutz, A. Kuhmichel, M. Lattuada, U. Lynen, C. Mazur, W. F.J. Muller, J. B. Natowitz, C. Ngo, J. Pochodzalla, G. Raciti, M. Ribrag, H. Sann, W. Trautmann, R. Trockel, Z. Phys. A346,227 (1993).

Nuclear Reactions: 197Au(84Kr,X), E=35 MeV/nucleon; measured σ(fragment θ,E) for X=Li-Ar; deduced moving source parame-ters, multi-fragment processes evidence.

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93Mi18 Magnetic Properties of Collective States for 156, 158, 160, 162, 164Dy Isotopes

I. N. Mikhailov, P. N. Usmanov, A. A. Okhunov, S. Brianson, R. Kulessa, Bull. Rus. Acad. Sci. Phys. 57, 15 (1993).

Nuclear Structure: 156, 158, 160, 162, 164Dy; calculated levels, g(R) factor, B(λ) vs spin, δ. Phenomenological model, Coriolis mix-ing.

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93Mi19 Detailed Balance Test of Time Reversal Invariance with Interfering Resonances

G. E. Mitchell, E. G. Bilpuch, C. R. Bybee, J. M. Drake, J. F. Shriner, Jr., Nucl. Phys. A560, 483 (1993).

Nuclear Reactions: 23Na, 27Al, 31P, 35Cl, 39K(p, p), (p,α), E not given; compiled, reviewed resonance data; calculated σ(θ) differ-ence; deduced detailed balance tests related features.

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93Mi20 Invisible Axion Search in 139La M1 Transition

M. Minowa, Y. Inoue, T. Asanuma, M. Imamura, Phys. Rev. Lett. 71, 4120 (1993).

Radioactivity: 139Ce(EC); measured γ(X-ray)-coin. 139La transition deduced Γ(axion)/Γγ upper limit. 139Ce deduced second for-bidden EC-decay branching ratio.

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93Mi21 Hypertriton Calculation with Meson-Theoretical Nucleon-Nucleon and Hyperon-Nucleon Interactions

K. Miyagawa, W. Glockle, Phys. Rev. C48, 2576 (1993).

Nuclear Structure: A=3; calculated hypertriton binding energy features. Faddeev calculations, (lambda)NN-, ΣNN-coupled sys-tems.

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93Mi22 6He(Lambda)(Lambda) Hypernucleus in α + 2(Lambda) Cluster Model

M. Mian, Pramana 41, 145 (1993).

Nuclear Structure: A=6; calculated double hypernucleus 6He(lambda)(lambda) binding energy. Density dependent effective(Lambda)N force, α+(2 lambda) cluster.

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93Mi23 Influence of Giant Angular Resonances on the Electromagnetic Characteristics of Low-Lying States

I. N. Mikhailov, Ph. N. Usmanov, Ann. Phys. (Leipzig) 2, 239 (1993).

Nuclear Structure: 164, 166, 168Er; calculated levels, B(λ) ratio, δ. Two-rotor model, Feshbach projection operator.

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93Mi24 The Chemical Fate of 212Bi-DOTA Formed by β- Decay of 212Po(DOTA)(2-)

S. Mirzadeh, K. Kumar, O. A. Gansow, Radiochim. Acta 60, 1 (1993).

Radioactivity: 212Pb(β-); measured 212Bi-DOTA complex chemical fate; deduced internal conversion γ-ray role in kinetic, elec-tronic excitation of 212Bi.

Page 153: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Mi25 Detailed Balance Study of Time Reversal Invariance with Interfering Resonances

G. E. Mitchell, E. G. Bilpuch, C. R. Bybee, J. M. Drake, J. F. Shriner, Jr., Nucl. Instrum. Methods Phys. Res. B79, 290 (1993)

Nuclear Reactions: 23Na, 27Al, 31P, 35Cl, 39K(p, α), E=resonance; compiled, reviewed resonance data, analyses; deduceddetailed balance tests sensitivity features.

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93Mi26 On 10Be Standards and the Half-Life of 10Be

R. Middleton, L. Brown, B. Dezfouly-Arjomandy, J. Klein, Nucl. Instrum. Methods Phys. Res. B82, 399 (1993)

Radioactivity: 10Be(β-); analyzed 9, 10Be isotope ratio data; deduced T1/2. Accelerator mass spectrometry.

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93Mi27 A Program for Evaluation of Gamma-Spectra (ANA)

P. Mishev, J. Radioanal. Nucl. Chem. 176, 199 (1993).

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93Mi28 A Device for Ballistic Deficit Correction in Solid State Detector Spectrometers

M. A. Mikhaiov, Nucl. Instrum. Methods Phys. Res. A334, 447 (1993)

Radioactivity: 60Co(β-); measured Eγ, Iγ. Solid state detector spectrometers, ballistic deficit correction.

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93Mi29 Conversion Transitions in 187W Decay

N. F. Mitrokhovich, L. P. Sidorenko, A. I. Feoktistov, Bull. Rus. Acad. Sci. Phys. 57, 1599 (1993).

Radioactivity: 187W(β-); measured I(ce). 187Re transitions deduced ICC, δ, M2 component penetration parameter. π square root2 spectrometer.

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93Mi30 Anomalous Conversion in the Decay of 181Hf

N. F. Mitrokhovich, L. P. Sidorenko, A. I. Feoktistov, Bull. Rus. Acad. Sci. Phys. 57, 1610 (1993).

Radioactivity: 181Hf(β-); measured I(ce). 181Ta deduced transitions ICC, penetration parameter. Multi-channel magnetic π squareroot 2 β-spectrometer.

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93Mi31 Emission Probability for the 443 keV γ-Rays of 128I

H. Miyahara, H. Matumoto, K. Yanagida, Y. Takenaka, C. Mori, Nucl. Instrum. Methods Phys. Res. A336, 385 (1993)

Radioactivity: 128I(EC), (β+), (β-); measured βγ-coin. 128Xe level deduced γ-emission probability.

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93Mi32 Time Component of the Mirror Beta Decays of 12B and 12N

T. Minamisono, A. Kitagawa, K. Matsuta, Y. Nojiri, Hyperfine Interactions 78, 77 (1993).

Radioactivity: 12B(β-) [from 11B(d,p), E=1.5 MeV]; 12N(β+) [from 10B(3He, n), E=3 MeV]; measured Iβ(θ); deduced alignmentcoefficients, Gamow-Teller matrix elements axial vector time component ratio.

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93Mi33 Precise Measurement of the Magnetic Moment of Doubly Closed Shell+1 Nucleon Nucleus 17F(I(π) = (5/2)+, T1/2 = 64.5s)

T. Minamisono, T. Ohtsubo, S. Fukuda, Y. Nakayama, T. Araki, K. Mashitani, K. Matsuda, E. Takahashi, M. Tanigaki, M.Tanaka, H. Shiohara, Y. Someda, Y. Aoki, A. Kitagawa, M. Fukuda, K. Matsuta, Y. Nojiri, Hyperfine Interactions 78, 111(1993).

Radioactivity: 17F(β+); measured β-NMR spectra asymmetry change in NaF; deduced µ.

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93Mi34 New Determination of Quadrupole Coupling Constants of Li Isotopes in Single Crystals LiIO3 and LiNbO3

T. Minamisono, T. Ohtsubo, Y. Nakayama, S. Fukuda, T. Izumikawa, M. Tanigaki, M. Matsui, S. Takeda, N. Nakamura, M.Fukuda, K. Matsuta, Y. Nojiri, Hyperfine Interactions 78, 159 (1993).

Radioactivity: 8Li(β-); measured modified β-NMR spectra in LiO3, LiNbO3; deduced quadrupole moment, quadrupole couplingconstants.

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93Mi35 Giant Quadrupole Moment and Proton Halo Discovered in 8B

T. Minamisono, T. Ohtsubo, I. Minami, A. Kitagawa, S. Fukuda, Y. Nakayama, M. Fukuda, K. Matsuta, Y. Nojiri, S. Takeda,H. Sagawa, H. Kitagawa, Hyperfine Interactions 78, 165 (1993).

Radioactivity: 8B(β+); calculated quadrupole moment; deduced proton halo role.

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93Mi36 Precise Measurement of Quadrupole Moment of 8B by Use of a Modified β-NMR

T. Minamisono, T. Ohtsubo, I. Minami, S. Fukuda, A. Kitagawa, Y. Nakayama, M. Fukuda, K. Matsuta, Y. Nojiri, HyperfineInteractions 78, 169 (1993).

Radioactivity: 8B(β+); 12B(β-); measured modified β-NMR spectra in Mg; deduced quadrupole moment.

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93Mi37 Quadrupole Moment of 41Sc by Use of New Nuclear Quadrupole Resonance Detection

T. Minamisono, S. Fukuda, T. Ohtsubo, M. Tanigaki, A. Kitagawa, M. Fukuda, K. Matsuta, Y. Nojiri, S. Takeda, HyperfineInteractions 78, 191 (1993).

Radioactivity: 41Sc(β+); measured β-NMR spectra in TiO2; deduced quadrupole moment.

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93Mi38 First Principles Theory of Hyperfine Interactions in Spinels: ZnAl2O4

D. W. Mitchell, S. B. Sulaiman, N. Sahoo, T. P. Das, W. Potzel, G. M. Kalvius, W. Schiessl, H. Karzel, M. Steiner, HyperfineInteractions 78, 403 (1993).

Nuclear Moments: +27}Al, 67Zn; calculated quadrupole interactions in spinel ZnAl2O4. Hartree-Fock cluster procedure.

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93Mi39 Hyperfine Interactions in Icosahedral Quasicrystals: A Mossbaruer study

M. Miglierini, S. Nasu, T. Kuwano, Hyperfine Interactions 80, 977 (1993).

Nuclear Reactions: 57Fe(γ,γ), E=14.4 keV; measured Mossbauer spectra; deduced hyperfine interaction parameters inicosahedral quasicrystals.

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93Mi40 New Nuclear Quadrupole Resonance Technique in β-NMR

T. Minamisono, T. Ohtsubo, S. Fukuda, I. Minami, Y. Nakayama, M. Fukuda, K. Matsuta, Y. Nojiri, Hyperfine Interactions 80,1315 (1993).

Radioactivity: 41Sc(β+) [from 40Ca(d,n), E=4.1 MeV]; measured NQR spectra; deduced quadrupole coupling constant, quadrupolemoment. Modified β-NMR technique, 45Sc data input.

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93Mi41 Two-Center Shell Model with Mass-Asymmetry and Necking-In

M. Mirea, D. N. Poenaru, D. Mirea, Roum. J. Phys. 38, 71 (1993).

Nuclear Structure: 234U; calculated asymmetric fission one-body levels, 100Zr light fragment. Two-center shell model, massasymmetry, necking-in.

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93MiZO High Spin States in 82Zr

S. Mitarai, T. Kuroyanagi, A. Odahara, J. Mukai, H. Tomura, S. Suematsu, D. Jerrestam, J. Nyberg, G. Sletten, A. Atac, N.Gjorup, J. Jongman, S. E. Arnell, H. A. Roth, O. Skeppstedt, Kyushu Univ. Tandem Acc. Lab. Rept., 1991-1992, p. 82 (1993).

Nuclear Reactions: 58Ni(28Si,2n2p), E=128 MeV; measured Eγ, Iγ, γγ-coin. 82Zr deduced high-spin levels, J, π. NORDBALLspectrometer, n-, γ-multiplicity filter.

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93MiZP Band Structures of 81Y

S. Mitarai, T. Kuroyanagi, A. Odahara, J. Mukai, H. Tomura, S. Suematsu, T. Morikawa, D. Jerrestam, J. Nyberg, G. Sletten,A. Atac, M. Piiparinen, S. E. Arnell, D. Foltescu, H. A. Roth, O. Skeppstedt, Kyushu Univ. Tandem Acc. Lab. Rept., 1991-1992,p. 75 (1993).

Nuclear Reactions: 58Ni(28Si,pα), E=100 MeV; 58Ni(32S, p2α), E=120, 125 MeV; measured Eγ, Iγ, γ(θ). 81Y deduced high-spinlevels, J, π. NORDBALL spectrometer, n-, γ-multiplicity filter.

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93MiZQ Test Experiment to Measure High Energy Gamma Rays from the 12C(12C,γ)24Mg Reaction

S. Mitsuoka, K. Nakamoto, M. Hijiya, K. Utsunomiya, T. Mukae, S. Niiya, T. Okamoto, H. Fujita, T. Sugimitsu, S. Morinobu,Kyushu Univ. Tandem Acc. Lab. Rept., 1991-1992, p. 34 (1993).

Nuclear Reactions: 12C(12C,γ), E=16.24 MeV; measured Eγ, γ(particle)-coin.

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93MiZR Vector and Tensor Analyzing Powers in H(d(pol),d) Scattering at E(d) = 8 18 MeV

T. Miwa, N. Nishimori, S. Ueno, R. Koyasako, K. Nakashima, H. Akiyoshi, H. Ochiishi, S. Shimizu, K. Maeda, H. Nakamura,K. Sagara, T. Nakashima, Kyushu Univ. Tandem Acc. Lab. Rept., 1991-1992, p. 10 (1993).

Nuclear Reactions: 1H(polarized d,d), E=8-18 MeV; measured iT11(θ), T20(θ), T21(θ), T22(θ). Gas target. Exact Coulomb calcula-tion, Faddeev calculation.

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93MiZS Microscopic Kaonic Atom Optical Potential in Finite Nuclei with (Lambda)(1405) and Σ(1385) Resonances

M. Mizoguchi, S. Hirenzaki, H. Toki, RIKEN-AF-NP-151 (1993).

Atomic Physics: esic-Atoms 12C; calculated kaonic level shift, width. Microscopic kaonic atom optical potential.

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93MiZT Elastic and Inelastic Scattering of 30 and 35 MeV Neutrons by 12C

S. Miyamoto, H. Orihara, K. Ishii, M. Hosaka, G. Zhong, Y. Ishimaru, T. Nakagawa, A. Terakawa, A. Narita, T. Inomata, T.Matsumoto, T. Niizeki, Cyclotron Rad. Center, Tohoku Univ., Ann. Rept., 1992, p. 1 (1993).

Nuclear Reactions: 12C(n,n), (n,n’), E=30, 35 MeV; measured σ(θ). Dispersive optical model.

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93MiZU Investigation of Conversion Spectrum in Decay of 187W

N. F. Mitrokhovich, L. P. Sidorenko, A. I. Feoktistov, Program and Thesis, Proc. 43rd Ann. Conf. Nucl. Spectrosc. Struct. At.Nuclei, Dubna, p. 109 (1993).

Radioactivity: 187W(β-); measured I(ce). 187Re transitions deduced ICC, δ, M2-penetration parameter. Double-focusing β-spectrometer.

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93MiZV Investigation of Anomalous Conversion in Decay of 181Hf

N. F. Mitrokhovich, L. P. Sidorenko, A. I. Feoktistov, Program and Thesis, Proc. 43rd Ann. Conf. Nucl. Spectrosc. Struct. At.Nuclei, Dubna, p. 104 (1993).

Radioactivity: 181Hf(β-); measured I(ce). 181Ta transitions deduced ICC, δ, M2-, M3-penetration parameters. Double-focusing β-spectrometer.

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93MiZW 40Ca(p,2p) and Medium Modifications

D. N. Mihailidis, A. Sethi, N. M. Hintz, N. S. Chant, P. G. Roos, Bull. Am. Phys. Soc. 38, No. 2, 1052, N7 11 (1993)

Nuclear Reactions: 40Ca(p,2p), (polarized p,2p), E=200, 300 MeV; analyzed data. Density dependent DWIA.

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93MiZX Dispersion-Corrected Mean Fields for Strong- and Weak-Coupling Models of 116Sn + n

M. C. Mirzaa, M. T. McEllistrem, J. L. Weil, Bull. Am. Phys. Soc. 38, No. 2, 1051, N7 5 (1993)

Nuclear Reactions: 116Sn(n,n), E not given; analyzed data; deduced coupled-channels approach suitability. Dispersioncorrected mean fields.

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93MiZY High Spin States in the (p,t) Reaction

D. Mihailidis, N. M. Hintz, A. Sethi, E. J. Stephenson, A. Bacher, J. Liu, X. L. Xhang, S. Wells, Bull. Am. Phys. Soc. 38, No. 2,1050, N6 13 (1993)

Nuclear Reactions: 208Pb(p,t), (polarized p,t), E=120 MeV; measured triton spectra, analyzing power. 206Pb deduced levels, J,π, L.

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93MiZZ Inclusive Neutrino Reactions in Nuclei

S. L. Mintz, M. Pourkaviani, Bull. Am. Phys. Soc. 38, No. 2, 913, A6 2 (1993)

Nuclear Reactions: 12C(ν,X), E ≤ 100 MeV; measured average σ for Michel spectrum.

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93Mo01 Evidence Against a 17 keV Neutrino from 35S Beta Decay

J. L. Mortara, I. Ahmad, K. P. Coulter, S. J. Freedman, B. K. Fujikawa, J. P. Greene, J. P. Schiffer, W. H. Trzaska, A. R. Zeuli,Phys. Rev. Lett. 70, 394 (1993).

Radioactivity: 35S(β-); measured β-spectrum; deduced evidence against 17 keV neutrino. Mixed 35S, 14C source.

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93Mo02 Particle Evaporation from Hot Nuclei with A ≤ 85 Mainly Prior to Scission

H. Morgenstern, W. Bohne, S. Proschitzki, Z. Phys. A344, 259 (1993).

Nuclear Reactions: 27Al, 58Ni(58Ni,X), (58Ni, F), E=14.4 MeV/nucleon; measured fusion-fission fragment σ(θ); deduced light parti-cle evaporation mechanism in fission.

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93Mo03 Molecular-Orbital Study of Late-Fission Times in Deep-Inelastic 238U + 238U Collisions

J. D. Molitoris, W. E. Meyerhof, Ch. Stoller, R. Anholt, D. W. Spooner, L. G. Moretto, L. G. Sobotka, R. J. McDonald, G. J.Wozniak, M. A. McMahan, L. Blumenfeld, N. Colonna, M. Nessi, E. Morenzoni, Phys. Rev. Lett. 70, 537 (1993).

Nuclear Reactions: 238U(238U,X), (238U,F), E=7.5 MeV/ nucleon; measured K-vacancy production probability for no-fission,single-, double fission channels; deduced U-like products late fission time scales.

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93Mo04 How Accurate are the ’ Muonic ’ Quadrupole Moments in Eu ( Question )

W. Moller, H. Huhnermann, G. Alkhazov, V. Panteleev, Phys. Rev. Lett. 70, 541 (1993).

Radioactivity: 145, 146, 147Eu(EC), (β+); analyzed hfs data; deduced hyperfine coupling constants. 151, 153Eu; analyzed hfs data;deduced hyperfine coupling constants, electric quadrupole moment ratio, deviation from muonic data. Collinear laser ion beamspectroscopy.

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93Mo05 Polarized-Proton Scattering by Even-Mass Germanium and Selenium Isotopes at 22 MeV Incident Energy

W. H. L. Moonen, P. J. van Hall, S. S. Klein, G. J. Nijgh, C. W. A. M. van Overveld, R. M. A. L. Petit, O. J. Poppema, J. Phys.(London) G19, 635 (1993).

Nuclear Reactions: 70, 72, 74, 76Ge, 76, 78, 80Se(polarized p,p’), E=22.3 MeV; measured σ(θ), A(θ); deduced optical model param-eters. 70, 72, 74, 76Ge, 76, 78, 80Se levels deduced deformation, mixing of one, two-photon states. Coupled-channels calculations,interacting boson approximation.

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93Mo06 Radial Excitation of the P11(1440 MeV) Resonance and the Compressibility of the Nucleon

H. P. Morsch, Nucl. Phys. A553, 645c (1993).

Nuclear Reactions: 1H(α,α’), E 1 GeV/c; measured missing energy spectra; deduced evidence for strong Roper resonance exci-tation.

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93Mo07 Orbital M1 versus E2 Strength in Deformed Nuclei: A new new energy weighted sum rule

E. Moya de Guerra, L. Zamick, Phys. Rev. C47, 2604 (1993).

Nuclear Structure: 146, 148, 150Nd, 148, 150, 152, 154Sm, 156, 158, 160Gd, 162, 164Dy; calculated orbital 1+ strength low energy linearenergy weighted sum rule. Bohr-Mottelson unified model.

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93Mo08 Nucleon Polarization in Deuteron Electrodisintegration

B. Mosconi, J. Pauschenwein, P. Ricci, Phys. Rev. C48, 332 (1993).

Nuclear Reactions: 2H(polarized e,X), E not given; calculated vector, tensor target polarization transfer, tensor target-beampolarization transfer following target breakup; deduced neutron charge form factor role. Standard theory.

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93Mo09 Asymmetric Fission at Relativistic Energies

G. Mouze, Nuovo Cim. 106A, 715 (1993).

Nuclear Structure: 238U; analyzed asymmetric fission; deduced high energy Coulomb excitation role. Relativistic 238U ions onPb target.

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93Mo10 Neutron Resonance Parameters and Thermal-Neutron Capture by 43Ca

M. C. Moxon, J. A. Harvey, S. Raman, J. E. Lynn, W. Ratynski, Phys. Rev. C48, 553 (1993).

Nuclear Reactions: 43Ca(n,X), E=0.005-500 keV; measured transmission. 44Ca deduced resonances, J, Γn.

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93Mo11 Alpha Scattering and Capture Reactions in the A = 7 System at Low Energies

P. Mohr, H. Abele, R. Zwiebel, G. Staudt, H. Krauss, H. Oberhummer, A. Denker, J. W. Hammer, G. Wolf, Phys. Rev. C48,1420 (1993).

Nuclear Reactions: ICPND 4He(3He,3He), E=1.2-3 MeV; measured σ(θ). 4He(3He,3He), (t,t), E ≤ 10 MeV; analyzed phase shiftsdata. 3H, 3He(α,γ), E(cm) ≤ 1 MeV; calculated astrophysical S-factor vs E; deduced multipole contributions.

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93Mo12 Effect of Channel Coupling on Spin Distribution at and above Coulomb Barrier Energies

A. K. Mohanty, S. K. Kataria, M. S. Samant, Phys. Rev. C48, 1445 (1993).

Nuclear Reactions: 154Sm(16O,X), E=58-68 MeV; 122Sn(40Ar, X), E=108, 113 MeV; 100Mo(64Ni,X), E=130.1, 141.7 MeV;152Sm(16O,X), E=60, 80 MeV; calculated fusion partial σ energy, l dependence; deduced channel coupling role in spin distribution.

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93Mo13 Timing Properties of Philips XP2020UR Photomultiplier

M. Moszynski, Nucl. Instrum. Methods Phys. Res. A324, 269 (1993)

Radioactivity: 60Co(β-); 22Na(β+), (EC); measured induced photoelectron time spectra; deduced scintillation counters timing pro-perties. Small NE111 plastic scintillators, XP2020UR photomultipliers.

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93Mo14 Low-Lying Level Structure of 73Kr

D. M. Moltz, J. D. Robertson, E. B. Norman, J. Burde, C. W. Beausang, Nucl. Phys. A562, 111 (1993).

Nuclear Reactions: ICPND 16O, 40Ca(36Ar,n2p), E 90-110 MeV; measured nγγ-coin; deduced σ(E). 73Kr deduced levels.

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93Mo15 Scattering of 20.4 MeV Polarized Protons from Even-Mass Zinc Isotopes

W. H. L. Moonen, J. H. A. M. Krabbenborg, H. P. Offermans, J. F. A. G. Ruyl, P. J. van Hall, S. S. Klein, G. J. Nijgh, C. W. A.M. van Overveld, R. M. A. L. Petit, O. J. Poppema, J. Phys. (London) G19, 1191 (1993).

Nuclear Reactions: 64, 66, 68, 70Zn(polarized p,p’), (polarized p,p), E=20.4 MeV; measured σ(θ), analyzing power vs θ; deducedoptical model parameters. 64, 66, 68, 70Zn levels deduced deformation parameters.

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93Mo16 Prompt Neutron Emission and the Second Step of Asymmetric Nuclear Fission

G. Mouze, C. Ythier, Nuovo Cim. 106A, 835 (1993).

Nuclear Reactions: 235U(n,F), E=thermal; calculated second-step reaction energy release following fission.

Radioactivity: 236U(SF); calculated second-step reaction energy release following fission.

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93Mo17 Effect of the Closing of Shells on the Multipole Mixing Parameter δ(E2/M1) in l-Forbidden Magnetic Dipole Transitions

V. A. Morozov, Yad. Fiz. 56, No 8, 31 (1993); Phys. Atomic Nuclei 56, 1009 (1993).

Nuclear Structure: A=29-211; analyzed δ(E2/M1)/(Eγ) for l-forbidden M1 transitions; deduced shell closure effects role.

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93Mo18 Decay Properties of Heavy Mendelevium Isotopes

K. J. Moody, R. W. Lougheed, J. F. Wild, R. J. Dougan, E. K. Hulet, R. W. Hoff, C. M. Henderson, R. J. Dupzyk, R. L. Hahn,K. Summerer, G. D. O’Kelley, G. R. Bethune, Nucl. Phys. A563, 21 (1993).

Nuclear Reactions: ICPND 254Es(18O,X)256Md/255Md/ 257Md/258Md/258mMd/259Md/260Md, E=105 MeV;254Es(22Ne,X)256Md/255Md/ 257Md/258Md/258mMd/259Md/260Md, E=126 MeV; measured Eα, Iα; deduced residual nuclei productionσ.

Radioactivity: 256Md(EC), (α); 257Md(EC), (α), (SF); 258Md(α), (SF), (EC), (β-); 258mMd(EC), (α), (SF), (β-); 259Md(SF), (α); meas-ured Eα, Iα, γ-spectra, SF-decay; deduced T1/2, branching ratio. 256, 257, 258Md deduced mass excess. 259Md deduced SF-decay

hindrance factor. 252, 253, 254Es deduced levels, J, π, γ transitions.

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93Mo19 Spectroscopy of the Superdeformed Band in 196Pb

E. F. Moore, Y. Liang, R. V. F. Janssens, M. P. Carpenter, I. Ahmad, I. G. Bearden, P. J. Daly, M. W. Drigert, B. Fornal, U.Garg, Z. W. Grabowski, H. L. Harrington, R. G. Henry, T. L. Khoo, T. Lauritsen, R. H. Mayer, D. Nissius, W. Reviol, M. Sfer-razza, Phys. Rev. C48, 2261 (1993).

Nuclear Reactions: 170Er(30Si,4n), E=142-151 MeV; measured Eγ, Iγ, γγ-coin, DSA. 196Pb deduced superdeformed band transi-tions, intrinsic quadrupole moment, dynamic moment of inertia. Model comparison.

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93Mo20 Experimental Signature for Statistical Multifragmentation

L. G. Moretto, D. N. Delis, G. J. Wozniak, Phys. Rev. Lett. 71, 3935 (1993).

Nuclear Reactions: 27Al, 51V, Cu(197Au,F), E=60 MeV/ nucleon; analyzed fission data; deduced binary, ternary, quaternary,quinary fission branching ratios, statistical competition role.

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93Mo21 The Neutron-Proton Interaction Energy of the Valence Nucleons. III. - The Valence Shells of 40Ca

G. Mouze, S. Bidegainberry, A. Rocaboy, C. Ythier, Nuovo Cim. 106A, 885 (1993).

Nuclear Structure: A=42-56; calculated neutron-proton interaction energies; deduced shell closure effect role, anomaly features.

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93Mo22 On the Symmetric Mass Division of Some Trans-Bk Nuclei

G. Mouze, Nuovo Cim. 106A, 961 (1993).

Nuclear Structure: 259Lr; calculated fission fragment mass yield curve. 259, 258Fm, 258, 262No, 260Md; calculated symmetric massdivision following fission; deduced nuclear matter phase change possibility consequences.

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93Mo23 Precise Widths of the 3089 and 3684 keV Levels in 13C

R. Moreh, O. Beck, I. Bauske, W. Geiger, R. D. Heil, U. Kneissl, J. Margraf, H. Maser, H. H. Pitz, Phys. Rev. C48, 2625(1993).

Nuclear Reactions: 13C(γ,γ’), E=4.7 MeV bremsstrahlung; measured precise Eγ, Iγ. 13C levels deduced Γ0. Self-absorption tech-

nique, enriched target, amorphous 13C absorbers.

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93Mo24 Timing Study with Fast Photomultipliers Equipped with a Screening Grid at the Anode

M. Moszynski, Nucl. Instrum. Methods Phys. Res. A330, 100 (1993)

Radioactivity: 22Na(β+), (EC); 60Co(β-); measured γ spectra; deduced time resolution. Small NE111 scintillators.

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93Mo25 Magic Energies in Auger Electron Spectra

R. Monreal, S. P. Apell, Nucl. Instrum. Methods Phys. Res. B83, 459 (1993)

Atomic Physics: i(α,e), E=4-100 keV; analyzed electron kinetic energy distributions; deduced incoming ion level broadening role.

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93Mo26 Charged Particle Detector System for Coulomb Excitation Experiment with NORDBALL

T. Morikawa, H. Inoue, Y. Iwata, T. Matsuoka, H. Otsuka, N. Kato, S. Mitarai, Y. Yoshizawa, Nucl. Instrum. Methods Phys.Res. A335, 453 (1993)

Nuclear Reactions: 154Sm(58Ni,58Ni’), E=220 MeV; measured Eγ, Iγ, γγ-, pγγ-coin following Coulomb excitation. 154Sm(32S,32S’),E not given; measured not given. 154Sm levels deduced Coulomb excitation probability vs θ. Charged particle plus multi-γ-raydetector systems.

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93Mo27 Pion Scattering at Energies Above the ∆ Resonance

C. L. Morris, J. M. O’Donnell, J. D. Zumbro, Acta Phys. Pol. B24, 1659 (1993).

Nuclear Reactions: 12C(π+,π+), (π-,π-), E=180-673 MeV; analyzed σ(θ). 12C, 208Pb(π+, π+X), (π-,π-X), E=500 MeV; compiled,reviewed data, analyses; deduced virtual ∆-components measuring possibility.

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93Mo28 An Electron-Positron Pair Spectrometer for High Energy Decays of Nuclei

C. P. Montoya, S. Schadmand, R. Varma, P. H. Zhang, R. Butsch, I. Dioszegi, D. J. Hofman, P. Paul, Nucl. Instrum. MethodsPhys. Res. A334, 437 (1993)

Radioactivity: 8Li(β-) [from 7Li(d,p)]; measured β-decay end point energy; deduced detector calibration. Segmented phoswichplastic scintillator array (e+, e-) pair spectrometer.

Nuclear Reactions: 19F(p,α), E=5.2 MeV; measured Eγ, Iγ, for GDR region in 20Ne; deduced spectrometer efficiency. Seg-mented phoswich plastic scintillator array (e+,e-) pair spectrometer.

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93Mo29 Particle Identification by Digital Charge Comparison Method Applied to CsI(Tl) Crystal Coupled to Photodiode

M. Moszynski, D. Wolski, T. Ludziejewski, S. E. Arnell, O. Skeppstedt, W. Klamra, Nucl. Instrum. Methods Phys. Res. A336,587 (1993)

Radioactivity: 137Cs(β-); measured Eγ, Iγ. 232Th(α); measured α-spectra; deduced device particle identification capabilities. Digi-tal charge comparison method, CsI(Tl)-photodiode assembly, proton spectra studied.

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93Mo30 Induced Pseudoscalar Interaction in Weak Nucleon Current and Muon Capture in Hyperfine States of Muonic Deuterium

M. Morita, R. Morita, M. Doi, T. Sato, H. Ohtsubo, K. Koshigiri, Hyperfine Interactions 78, 85 (1993).

Atomic Physics: esic-Atoms 2H; calculated muon capture rate in muonic deuterium.

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93Mo31 Investigation of Expected Location of Muonium in Normal State in III-V Semiconductors and Associated Muon HyperfineInteraction

S. M. Mohapatra, N. Sahoo, K. C. Mishra, T. Briere, S. S. Nunes, F. Hagelberg, A. Catia, O. Donzelli, T. P. Das, HyperfineInteractions 79, 659 (1993).

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93Mo32 Theory for Position of Muonium in α-Quartz and Associated Hyperfine Interaction

S. M. Mohapatra, N. Sahoo, K. C. Mishra, T. Briere, F. Hagelberg, T. P. Das, Hyperfine Interactions 79, 739 (1993).

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93Mo33 Hyperfine Quantum Beat of Short-Lived Beta-Emitter 8Li Polarized by the Tilted Foil Technique

S. Momota, Y. Nojiri, M. -B. Tanaka, T. Yanagisawa, M. Fukuda, K. Mutsuta, T. Minamisono, Hyperfine Interactions 80, 1275(1993).

Radioactivity: 8Li(β-) [from 7Li(d,p), E=3 MeV]; measured polarization quantum beat vs two tilted foils distance.

Page 215: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Mo34 Nuclear Spin Dependence of Polarization Enhancement by Multi-Tilted Foils Studied by Short-Lived Beta-Emitters 8B and 12B

S. Momota, Y. Nojiri, M. -B. Tanaka, T. Yanagisawa, M. -Y. Tanaka, M. Fukuda, K. Matsuta, T. Minamisono, HyperfineInteractions 80, 1281 (1993).

Radioactivity: 8B(β+) [from 6Li(3He,n), E=4.5 MeV]; measured polarization vs tilted foils number; deduced nuclear spin dependentenhancement features.

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93Mo35 Prospects for New Fast Photomultipliers

M. Moszynski, Nucl. Instrum. Methods Phys. Res. A337, 154 (1993)

Radioactivity: 60Co(β-); 22Na(EC), (β+); measured γ(t); deduced fast photomultipliers development implications. Different scintilla-tor detectors coupled to various photomultipliers.

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93Mo36 The Status of Two-Neutrino and Neutrinoless Double Beta Decay Searches

M. K. Moe, Int. J. Mod. Phys. E2, 507 (1993).

Radioactivity: 48Ca, 76Ge, 82Se, 100Mo, 128, 130Te, 136Xe, 150Nd; compiled, reviewed 0ν-accompanied T1/2, majoron limits data,other nuclei, other aspects.

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93MoZP Gamow-Teller Strength in the Beta Decay of Proton Rich T(z) = (-3/2) Nuclei of 25Si and 29S

S. Morinobu, S. Hatori, H. Miyatake, T. Shimoda, Kyushu Univ. Tandem Acc. Lab. Rept., 1991-1992, p. 69 (1993).

Radioactivity: 25Si(β+p) [from 24Mg(3He, 2n), E=35 MeV]; 29S(β+p) [from 28Si(3He, 2n), E=35 MeV]; measured β-delayed E(p),βp-, γp-coin, T1/2; deduced GT strength functions. 25Al, 29P deduced levels. Silicon detector, β-counter telescope.

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93MoZQ Collective Excitations Evinced by Fast Dipole Transitions

G. Molnar, B. Fazekas, A. Veres, T. Belgya, R. A. Gatenby, E. M. Baum, E. L. Johnson, S. W. Yates, J. R. S. Vanhoy, T.Otsuka, T. T. Dinh, M. Grinberg, C. Stoyanov, Proc. 6th Intern. Conf. on Nuclei Far from Stability + 9th Intern. Conf. on AtomicMasses and Fundamental Constants, Bernkastel-Kues, Germany, 19-24 July, 1992, R. Neugart, A. Wohr, Eds., p. 679 (1993)

Nuclear Reactions: 134Ba, 144Sm(n,n’γ), E not given; measured not given. 144Sm deduced levels, possible J, π, γ multipolarity.134Ba deduced levels, J, π, γ multipolarity, B(λ).

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93MoZR New Nuclei Along the Proton Drip Line Near Z = 40

M. F. Mohar, S. J. Yennello, W. Benenson, D. J. Morrissey, N. A. Orr, B. M. Sherrill, J. A. Winger, Proc. 6th Intern. Conf. onNuclei Far from Stability + 9th Intern. Conf. on Atomic Masses and Fundamental Constants, Bernkastel-Kues, Germany, 19-24July, 1992, R. Neugart, A. Wohr, Eds., p. 397 (1993)

Nuclear Reactions: 58Ni(92Mo,X), E=70 MeV/nucleon; measured fragment mass spectra; deduced evidence for 78Y, 82Nb, 85Mo,86Tc, 89Ru.

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93MoZS Measurements of Angular Distributions for the 11Li + p and 9Li + p Elastic Scattering

C. -B. Moon, M. Fujimaki, N. Inabe, K. Katori, J. C. Kim, T. Kobayashi, T. Kubo, H. Kumagai, S. Shimoura, T. Suzuki, I. Tan-ihata, Proc. 6th Intern. Conf. on Nuclei Far from Stability + 9th Intern. Conf. on Atomic Masses and Fundamental Constants,Bernkastel-Kues, Germany, 19-24 July, 1992, R. Neugart, A. Wohr, Eds., p. 277 (1993)

Nuclear Reactions: 1H(11Li,11Li), E=62 MeV; 1H(9Li, 9Li), E=61 MeV; measured σ(θ); deduced model parameters.

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93MoZT Some Fundamental Aspects of Energetic Structure of Nuclear Ground States

G. Mouze, C. Ythier, Proc. 6th Intern. Conf. on Nuclei Far from Stability + 9th Intern. Conf. on Atomic Masses and FundamentalConstants, Bernkastel-Kues, Germany, 19-24 July, 1992, R. Neugart, A. Wohr, Eds., p. 101 (1993)

Nuclear Structure: 18, 20, 22, 24, 26O; calculated detachment energy variation.

Page 223: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93MoZU Critical Assessment of Nuclear Mass Models

P. Moller, J. R. Nix, Proc. 6th Intern. Conf. on Nuclei Far from Stability + 9th Intern. Conf. on Atomic Masses and FundamentalConstants, Bernkastel-Kues, Germany, 19-24 July, 1992, R. Neugart, A. Wohr, Eds., p. 43 (1993)

Nuclear Structure: N ≤ 160; compiled, reviewed atomic mass model estimates; deduced mass model development possibilities.

Atomic Physics: ≤ 160; compiled, reviewed atomic mass model estimates; deduced mass model development possibilities.

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93MoZV Hyperfine Interactions of Short-Lived Beta-Emitter 8Li in Ferromagnetic Ni

S. Momota, T. Yanagisawa, M. -B. Tanaka, M. Nakazato, M. Fukuda, K. Matsuta, Y. Nojiri, T. Minamisono, Osaka Univ. Lab.Nucl. Studies, Ann. Rept., 1992, p. 67 (1993).

Radioactivity: 8Li(β-) [from 7Li(d,p), E=3.7 MeV]; measured NMR; deduced magnetic hyperfine field, relaxation time. β-NMRmethod.

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93MoZW Nuclear Spin Dependence of Polarization Enhancement by Multi-Tilted Foils Studied by Short-Lived Beta-Emitter 8B and 12B

S. Momota, M. -B. Tanaka, T. Yanagisawa, M. Nakazato, M. Fukuda, K. Matsuta, Y. Nojiri, T. Minamisono, Osaka Univ. Lab.Nucl. Studies, Ann. Rept., 1992, p. 63 (1993).

Radioactivity: 8B(β+) [from 6Li(3He,n), E=4.5 MeV]; measured nuclear polarization; deduced nuclear spin dependence of polariza-tion enhancement. Tilted-foil technique, β-NMR method, comparison with 12B data.

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93MoZX Measurements of 11Li + p and 9Li + p Elastic Scatterings at 60 MeV

C. -B. Moon, M. Fujimaki, S. Hirenzaki, N. Inabe, K. Katori, J. C. Kim, Y. K. Kim, T. Kobayashi, T. Kubo, H. Kumagai, S. Shi-moura, T. Suzuki, I. Tanihata, RIKEN-92, p. 21 (1993).

Nuclear Reactions: 1H(9Li,9Li), E=60 MeV/nucleon; 1H(11Li, 11Li), E=62 MeV/nucleon; measured σ(θ); deduced reactionmechanism. Radioactive beam, inverse kinematics.

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93MoZY Coulomb Breakup of 8B

T. Motobayashi, M. Gai, N. Iwasa, Y. Ando, Th. Delbar, R. H. France III, K. Furutaka, Y. Futami, K. I. Hahn, N. Inabe, M.Ishihara, T. Kubo, M. Kurokawa, H. Murakami, T. Nakamura, J. Ruan, S. Shimoura, S. Shirato, T. Teranishi, Y. Watanabe, Z.Zhao, RIKEN-92, p. 19 (1993).

Nuclear Reactions: 208Pb(8B,p7Be), E=47 MeV/nucleon; measured σ(θ,Ep,E(7Be)); deduced 8B breakup reaction mechanism.Radioactive beam.

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93MoZZ Energy Dependence of Double Giant Resonances in Pion Double Charge Exchange

C. F. Moore, K. Johnson, J. Johnson, H. Ward, C. Whitley, S. Mordechai, S. Greene, C. L. Morris, J. O’Donnell, Y. Grof, Bull.Am. Phys. Soc. 38, No. 2, 942, C7 4 (1993)

Nuclear Reactions: 13C(π+,π-), E=140-295 MeV; measured σ(E). 13O deduced double giant resonance, spin-flip excitations.

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93Mu01 Deuteron Quadrupole Moment and 3S1-3D1 State Properties

M. M. Mustafa, Phys. Rev. C47, 473 (1993).

Nuclear Structure: 2H; calculated quadrupole moment, rms matter radius, asymptotic D/S ratio. Nonrelativistic potential models,short range attractive nonlocality.

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93Mu02 Low-Energy Parameters of the dt and d3He Systems

V. D. Mur, B. M. Karnakov, S. G. Pozdnyakov, V. S. Popov, Yad. Fiz. 56, No 2, 125 (1993); Phys. Atomic Nuclei 56, 217(1993).

Nuclear Reactions: ICPND 3H(d,n), 3He(d,p), E ≤ 2 MeV; calculated astrophysical S-factor vs E, scattering lengths, effectiveranges.

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93Mu03 High-Spin Isomeric State in 144Pm

T. Murakami, Y. Gono, A. Ferragut, Y. H. Zhang, K. Morita, A. Yoshida, M. Ogawa, M. Nakajima, B. J. Min, H. Kumagai, M.Oshima, T. Morikawa, M. Sugawara, H. Kusakari, Z. Phys. A345, 123 (1993).

Nuclear Reactions: 14N(136Xe,6n), E=8.5 MeV/nucleon; measured γγ-coin. Ba(10B,X), E=22.5-55 MeV; measured 144Pm produc-tion σ(E), σ(E,Eγ). 144Pm deduced transition, isomer, T1/2 lower limit, possible J, π.

Page 232: E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B, 1 ... · 93Ma01 Partial Decay Widths from Giant Resonances in 208 Pb E. Maglione, R. J. Liotta, T. Vertse, Phys. Lett. 298B,

93Mu04 Low-Energy Excitations and Occupation Probabilities

H. Muther, L. D. Skouras, Nucl. Phys. A555, 541 (1993).

Nuclear Structure: 16O; calculated single particle strength distribution; deduced fragmentation. Green function, shell modelapproaches comparison, realistic nucleon-nucleon interaction.

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93Mu05 Perturbed Alignments within an i13/2 Neutron Intruder Band in 141Gd

S. M. Mullins, A. Omar, L. Persson, D. Prevost, J. C. Waddington, H. R. Andrews, G. C. Ball, A. Galindo-Uribarri, V. P. Jan-zen, D. C. Radford, D. Ward, T. E. Drake, D. B. Fossan, D. LaFosse, P. Vaska, M. Waring, R. Wadsworth, Phys. Rev. C47,R2447 (1993).

Nuclear Reactions: 112Sn(32S,n2p), E=155 MeV; 112Sn(33S, 2n2p), E=170 MeV; measured γγ-, γγ(charged particle)-coin. 141Gddeduced levels, J, π, configuration, alignment features. Cranked shell model.

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93Mu06 Excitations of 144Sm in (p,p’)

E. Muller-Zanotti, R. Hertenberger, H. Kader, D. Hofer, G. Graw, Gh. Cata-Danil, G. Lazzari, P. F. Bortignon, Phys. Rev. C47,2524 (1993).

Nuclear Reactions: 144Sm(p,p’), E=22 MeV; measured σ(θ); deduced direct, sequential strength distributions. 144Sm levelsdeduced L, deformation parameters, B(λ). DWBA, coupled-channels analyses.

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93Mu07 Correlations in Nuclei. Self-Consistent Treatment and the BAGEL Approach

H. Muther, L. D. Skouras, Phys. Lett. 306B, 201 (1993).

Nuclear Structure: 16O; calculated single particle energies, occupation probabilities, strengths. Self-consistent treatment.

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93Mu08 Coulomb Effect in Operator Expansion Method for Two-Neutrino Double Beta Decay

K. Muto, Phys. Rev. C48, 402 (1993).

Radioactivity: 76Ge, 130Te(2β); calculated 2ν-accompanied 2β-decay matrix element. Operator expansion method, Coulombeffect.

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93Mu09 Population Effects in the Highly-Deformed Bands of 131Ce and 135Nd from 18, 16O-Induced Reactions

S. M. Mullins, J. Nyberg, A. Maj, M. S. Metcalfe, P. J. Nolan, P. H. Regan, R. Wadsworth, R. A. Wyss, Phys. Lett. 312B, 272(1993).

Nuclear Reactions: 117Sn(18O,4n), E=85 MeV; measured Eγ, Iγ, γγ-coin, DSA. 122Te(16O, 3n), E=85 MeV; measured Eγ, Iγ, γγ-coin. 131Ce, 135Nd deduced levels, J, π, highly deformed band structure.

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93Mu10 Realistic Level Densities in Fragment Emission at High Excitation Energies

M. G. Mustafa, M. Blann, A. V. Ignatyuk, Phys. Rev. C48, 588 (1993).

Nuclear Structure: 100Ru; calculated fragment (Z ≤ 14) yields; deduced level density models dependence.

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93Mu11 Radius and Radial Moments of the Deuteron

M. M. Mustafa, Phys. Rev. C48, 929 (1993).

Nuclear Structure: 2H; analyzed (e,d), (e,p) data; deduced rms matter radius, radial moments.

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93Mu12 Calculation of the Vertex Constant for the Decay 6Li → α + d in the Three-body Model

A. M. Mukhamedzhanov, Kh. D. Razikov, N. K. Timofeyuk, R. Yarmukhamedov, Yad. Fiz. 56, No 7, 145 (1993); Phys. AtomicNuclei 56, 937 (1993).

Nuclear Structure: 6Li; calculated (α+d) breakup vertex constant. Three-body model.

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93Mu13 ππ-Angular Correlations for π-p → π+π-n in the Region of the ∆ Dominance

R. Muller, R. Baran, U. Bohnert, P. Helbig, G. Herrmann, A. Hofmann, O. Jakel, H. Kruger, D. Malz, W. Menzel, H. -W.Ortner, L. Schweinzer, S. Wirth, Phys. Rev. C48, 981 (1993).

Nuclear Reactions: 1H(π-,π+π-), E=284 MeV; measured σ(θ(π+),θ(π-)) vs E(π+), invariant mass distribution; deduced reactionmechanism. Weinberg’s Lagrangian based models, relativistic corrections, contribution of nonlinear terms.

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93Mu14 Accurate Measurement of the Intensity of 255.1 keV Gamma Ray in the Decay of 113Sn(115.1d)

A. Mukherjee, S. Bhattacharya, B. Dasmahapatra, Appl. Radiat. Isot. 44, 731 (1993).

Radioactivity: 113Sn(EC); measured Eγ, Iγ; deduced log ft. 113In deduced transition Iγ, EC branching ratio. High accuracy, largevolume hyperpure Ge detectors.

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93Mu15 Thomas-Fermi Approach to Thermal Quantum Hadrodynamics

H. Muller, R. M. Dreizler, Nucl. Phys. A563, 649 (1993).

Nuclear Structure: 40Ca, 208Pb; calculated temperature, binding energy, neutron, proton rms radii. Relativistic, thermalThomas-Fermi model.

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93Mu16 Superdeformation in 144Eu

S. M. Mullins, G. Hackman, A. Galindo-Uribarri, D. C. Radford, J. C. Waddington, D. Ward, Z. Phys. A346, 327 (1993).

Nuclear Reactions: 122Sn(27Al,5n), E=142 MeV; measured γγ-coin. 144Eu deduced superdeformed band evidence.

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93Mu17 K-Electron Capture Probabilities in 161Ho

G. S. K. Murty, N. V. S. Vara Prasad, M. V. S. C. Rao, M. Ravi Kumar, G. Satyanarayana, D. L. Sastry, Nuovo Cim. 106A,1043 (1993).

Radioactivity: 161Ho(EC); measured Eγ, Iγ, E X-ray, I X-ray. 161Dy levels deduced K-capture probabilities.

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93Mu18 Meson-Exchange Currents and the Strangeness Radius of 4He

M. J. Musolf, T. W. Donnelly, Phys. Lett. 318B, 263 (1993).

Nuclear Structure: 4He; calculated meson exchange current contribution to the strangeness radius ρ(s); deduced ρ(s) extraction(from 4He(e,e) parity violating asymmetry) implications.

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93Mu19 First Observation of a Proton Intruder Band Below the Z = 50 Major Shell Gap. Spectroscopy of 111In

S. M. Mullins, V. P. Janzen, P. Vaska, D. B. Fossan, G. Hackman, D. R. LaFosse, E. S. Paul, D. Prevost, H. Schnare, J. C.Waddington, R. Wadsworth, D. Ward, M. P. Waring, Phys. Lett. 318B, 592 (1993).

Nuclear Reactions: 96Zr(19F,4n), E=85, 72 MeV; measured γγ-coin, DSA. 111In deduced levels, J, π, intruder band features, qua-drupole moment, dynamic moments of inertia.

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93Mu20 Comparison of Two Versions of the Generalized Optical Model in Analysis of Neutron Data for Tellurium Isotopes’ Nuclei

R. M. Musaelyan, V. M. Skorkin, I. V. Surkova, T. M. Yakovenko, Bull. Rus. Acad. Sci. Phys. 57, 829 (1993).

Nuclear Reactions: 122, 124, 126, 128, 130Te(n, X), (n,n’), E ≤ 1.5 MeV; calculated σ(E); deduced suitable model, parameters. Twoversions of generalized optical model.

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93Mu21 Ion Exchange Behaviour of Cadmium and Indium on Organic Anion and Cation Exchangers: A 115Cd/115mIn Generator

A. Mushtaq, H. M. A. Karim, Radiochim. Acta 60, 189 (1993).

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93Mu22 Mathematical Analysis of Isobaric Decay Chain in Alpha Particle Induced Reactions

S. Mukherjee, N. L. Singh, J. Rama Rao, Pramana 41, 311 (1993).

Nuclear Reactions: ICPND 93Nb(α,3nα), (α,4npα), (α, n2α), (α,2n2α), E=threshold-120 MeV; analyzed σ vs E; deduced isobaricdecay chain feeding contribution to σ. Hybrid model, Batemann’s equations.

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93Mu23 Measurement and Analysis of the Excitation Functions for Alpha Particle Induced Reactions on Niobium

S. Mukherjee, M. H. Rashid, S. N. Chintalapudi, Pramana 41, 329 (1993).

Nuclear Reactions: ICPND 93Nb(α,n), (α,2n), (α,3n), (α, nα), (α,3np), E=threshold-45 MeV; measured σ vs E. Stacked foilactivation technique, Ge(Li) detector. Preequilibrium decay, hybrid model.

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93Mu24 Studies on K(α) X-Ray Satellite Energy Shifts

M. V. K. Murthy, K. S. Rao, V. Radhakrishna Murty, K. Parthasaradhi, T. Seshi Reddy, G. Ramesh Babu, B. Seetharami Reddy,Indian J. Pure Appl. Phys. 31, 137 (1993).

Atomic Physics: +27}Al, Si(γ,X), E=low; measured K(α) X-ray satellite energy shifts.

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93Mu25 Magnetic Ordering in DyNi2Si2 and DyNi2Ge2 Intermetallics Studied by 161Dy Mossbauer Spectroscopy

A. Murata, H. Onodera, M. Ohashi, Y. Yamaguchi, Hyperfine Interactions 78, 457 (1993).

Nuclear Reactions: 161Dy(γ,γ), E=74.6 keV; measured Mossbauer spectra; deduced magnetic hyperfine field vs temperature inDyNi2Si2, DyNi2Ge2.

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93Mu26 155Gd-Mossbauer Studies of the T(’)-, T(*)- and T-Phases of La(2-x-y)Gd(x)Sr(y)CuO4

M. Muther, G. Wortmann, I. Felner, I. Nowik, Physica C209, 428 (1993).

Nuclear Reactions: 155Gd(γ,γ), E=60 keV; measured Mossbauer spectra; deduced electric, magnetic hyperfine interactionsbased Gd ions location, magnetic properties in three possible phases.

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93Mu27 High-Resolution Spectroscopy and Optically Detected Nuclear Magnetic Resonance Studies of Ho3+ Ions in SrF2 Crystals Con-

taining Ba2+ and Ca2+ Impurities

M. Mujaji, T. Boonyarith, J. P. D. Martin, N. B. Manson, G. D. Jones, J. Phys. Condens. Matter 5, 3937 (1993).

Nuclear Moments: +165}Ho; measured NMR for Ho3+ ions in SrF2 crystals, Ba2+, Ca2+ impurities.

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93Mu28 Interactions of Protons with Nucleons and Neon Nuclei at an Energy of 300 GeV Accompanied by Neutron Generation

M. M. Muminov, I. Suvanov, B. S. Yuldashev, Bull. Rus. Acad. Sci. Phys. 57, 634 (1993).

Nuclear Reactions: 1H, Ne(p,X), E=300 GeV; measured fast neutron production, momentum distributions. Models testing.

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93MuZW High Spin States in the Odd-Odd Nucleus 82Y

J. Mukai, A. Odahara, H. Tomura, S. Suematsu, S. Mitarai, T. Kuroyanagi, D. Jerrestam, J. Nyberg, G. Sletten, A. Atac, S. E.Arnell, H. A. Roth, O. Skeppstedt, Kyushu Univ. Tandem Acc. Lab. Rept., 1991-1992, p. 78 (1993).

Nuclear Reactions: 58Ni(28Si,n3p), E=100, 102, 128 MeV; measured Eγ, Iγ, γγ-coin. 82Y deduced high-spin levels, J, π. NORD-BALL spectrometer.

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93MuZX Measurement of 12C(2+) Spin Alignment following 12C + 16O Collision I

T. Mukae, H. Fujita, M. Hijiya, T. Okamoto, S. Niiya, M. Matsuo, S. Mitsuoka, K. Utsunomiya, K. Nakamoto, Y. Sugiyama, Y.Tomita, K. Ideno, H. Ikezoe, Y. Yamanouchi, T. Sugimitsu, N. Kato, S. Morinobu, Kyushu Univ. Tandem Acc. Lab. Rept.,1991-1992, p. 40 (1993).

Nuclear Reactions: 12C(16O,16O’), E=64.3-78.2 MeV; measured σ(θ,E); deduced resonance structure.

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93MuZY Investigations of the Neutron Halo by Radioactive Beam Experiments

A. C. Mueller, IPNO-DRE-93-08 (1993).

Nuclear Reactions: 9Be, Ti, Ni, 197Au, 28Si(11Li, X), E=29 MeV/nucleon; compiled data, analyses; deduced 11Li halo features.

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93MuZZ Search for Nuclear Molecule Configurations in 48Cr

A. St. J. Murphy, N. M. Clarke, N. Curtis, B. R. Fulton, S. J. Hall, M. J. Leddy, J. S. Pople, G. Tungate, R. P. Ward, W. D. M.Rae, P. M. Simmonds, W. N. Catford, G. J. Gyapong, S. M. Singer, S. P. Chappell, S. P. Fox, C. D. Jones, D. L. Watson,Daresbury Lab., 1992-1993 Ann. Rept., Appendix, p. 70 (1993).

Nuclear Reactions: 24Mg(24Mg,X), E=150, 170 MeV; measured (16O,16O)-coin; deduced no three-body breakup evidence,σ(θ1,θ2).

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93My01 Transport of Polarized Ions Through a Tandem-Superconducting-Linac Heavy-Ion Accelerator

E. G. Myers, A. J. Mendez, K. W. Kemper, P. L. Kerr, E. L. Reber, B. G. Schmidt, Nucl. Instrum. Methods Phys. Res. A334,271 (1993)

Nuclear Reactions: 4He(polarized 6Li,6Li), E=20 MeV; measured on target beam polarization variation; deduced beam polariza-tion loss mechanisms.