92Ha10 - PNPI Home Page

92Ha01 Theoretical Study of 4 He(e,e’) 4 He(*)
D. Halderson, Phys. Rev. C45, 42 (1992).
Nuclear Reactions: 4 He(e,e’), E=60.6-200 MeV; analyzed data. Recoil-corrected continuum shell model.

92Ha02 Decay Scheme Data for 154 Eu, 198 Au and 239 Np
M. A. Hammed, I. M. Lowles, T. D. Mac Mahon, Nucl. Instrum. Methods Phys. Res. A312, 308 (1992)
Radioactivity: 154 Eu, 198 Au(β - ), 239 Np; measured relative, absolute γ-emission probabilities. 154 Gd levels deduced β-branching
ratios. Other data input. Comparison with other measurements.

92Ha03 Possibility of Observing Massive Neutrino Admixtures in Nuclear Orbital Electron Capture Rates
F. X. Hartmann, Phys. Rev. C45, R900 (1992).
Radioactivity: 157 Tb, 163 Ho, 179 Ta, 193 Pt, 205 Pb; analyzed decay data; deduced 157 Tb suitability for ν-admixtures search.

92Ha04 Reaction (p-bar)p → (Lambda-bar)Lambda in the Meson-Exchange Picture
J. Haidenbauer, T. Hippchen, K. Holinde, B. Holzenkamp, V. Mull, J. Speth, Phys. Rev. C45, 931 (1992).
Nuclear Reactions: 1 H(p-bar,X), (p-bar,p-bar), E at 1.4-1.71 GeV/ c; analyzed σ(θ), analyzing power vs θ; calculated σ vs
momentum for strangness production processes. Meson-exchange.

92Ha05 Investigation of Pion Exchange in the NN and N(N-bar) Systems
J. Haidenbauer, K. Holinde, A. W. Thomas, Phys. Rev. C45, 952 (1992).
Nuclear Reactions: 1 n(p,p), E ≤ 350 MeV; calculated phase shifts. 1 H(polarized p,p), E ≤ 25.68 MeV; calculated analyzing
powers vs θ. 1 H(p-bar,X), E < 650 MeV/c; calculated σ(θ), polarization vs θ. One-boson-exchange model.

92Ha06 Nuclear Masses in the Fermion Dynamical Symmetry Model
X. -L. Han, C. -L. Wu, D. H. Feng, M. W. Guidry, Phys. Rev. C45, 1127 (1992).
Nuclear Structure: Z ≥ 82; N ≥ 126; calculated neutron, proton separation pairing gap energies. Z=98, 114; calculated mass
shell corrections components. Fermion dynamical symmetry model.

92Ha07 Fusion-Fission of Aligned 23 Na with 138 Ba
S. J. Hall, G. Tungate, C. O. Blyth, H. D. Choi, K. A. Connell, N. J. Davis, B. R. Fulton, O. Karban, G. Kuburas, J. M. Nelson,
S. Roman, P. J. Woods, J. Phys. (London) G18, 181 (1992).
Nuclear Reactions: 138 Ba(polarized 23 Na, 23 Na), (polarized 23 Na,F), (polarized 23 Na,X), E=143-174 MeV; measured fusion,
fission, quasielastic σ(θ), T 20 (θ); deduced model parameters. Statistical model.

92Ha08 Studies of High-Spin States in Rare-Earth Nuclei using the Angular-Momentum Projection Method (III). Signature Splitting in
Odd Mass Nuclei
K. Hara, Y. Sun, Nucl. Phys. A537, 77 (1992).
Nuclear Structure: 165 , 167 Lu, 165 , 167 Yb, 161 , 163 Er; calculated levels, band structure; deduced signature splitting features.

92Ha09 Multifragmentation of 40 Ca + 40 Ca
K. Hagel, M. Gonin, R. Wada, J. B. Natowitz, B. H. Sa, Y. Lou, M. Gui, D. Utley, G. Nebbia, D. Fabris, G. Prete, J. Ruiz, D.
Drain, B. Chambon, B. Cheynis, D. Guinet, X. C. Hu, A. Demeyer, C. Pastor, A. Giorni, A. Lleres, P. Stassi, J. B. Viano, P.
Gonthier, Phys. Rev. Lett. 68, 2141 (1992).
Nuclear Reactions: 40 Ca( 40 Ca,X), E=35 MeV/nucleon; measured fragment emission probability vs charge for different number of
fragments; deduced multi-fragmentation mechanism. Different models.

92Ha10 Decays and Masses of 162 , 163 Ta and Some Neighboring Nuclides
E. Hagberg, X. J. Sun, V. T. Koslowsky, H. Schmeing, J. C. Hardy, Phys. Rev. C45, 1609 (1992).
Nuclear Reactions: 40 Ca( 127 I,X), ( 127 I,4n), ( 127 I, 5n), ( 127 I,6n), E=711 MeV; measured Eα, Iα, Eγ, Iγ; deduced σ(E) for residual
production σ, yields.
Radioactivity: 160 , 161 , 162 , 164 Ta, 159 , 160 , 161 , 162 , 164 Hf, 156 , 157 , 159 Lu, 158 Yb, 155 Tm [from 40 Ca( 127 I,X), E=711 MeV]; measured
Eα, Iα, Eγ, Iγ, T 1/2 . 150 , 151 Ho, 154 , 155 Tm, 158 , 159 Lu, 162 , 163 Ta, 166 , 167 Re, 170 , 171 Ir, 174 , 175 Au, 179 , 179m Tl deduced mass excess.
Other data input.

92Ha11 Algebraic Expression of the IBM3 Hamiltonian in Terms of Various Quantum Numbers (II). Numerical Test
M. Hasegawa, S. Tazaki, Nucl. Phys. A539, 381 (1992).
Nuclear Structure: 44 , 46 Ti, 48 Cr; calculated levels. Interacting boson model.

92Ha12 A Comparison of 3 H and 3 He Scattering from Light Deformed Nuclei
P. R. Hayes, N. M. Clarke, K. I. Pearce, M. B. Becha, R. S. Mackintosh, J. B. A. England, L. Zybert, G. M. Field, S. Roman,
Nucl. Phys. A540, 171 (1992).
Nuclear Reactions: 22 , 20 Ne(t,t’), ( 3 He, 3 He’), E=33.4 MeV; measured σ(θ); 26 , 24 Mg(t, t’), ( 3 He, 3 He’), E 34 MeV; analyzed data;
deduced potential parameters. 20 , 22 Ne, 26 , 24 Mg deduced deformation lengths, multipole moments. Coupled channel analysis.

92Ha13 Folded-Diagram Nucleon-Nucleon Potential for Application to the Many-Body Problem
J. Haidenbauer, K. Holinde, M. B. Johnson, Phys. Rev. C45, 2055 (1992).
Nuclear Reactions: 1 H(n,n), E ≤ 300 MeV; calculated phase shifts vs E. Energy independent nucleon-nucleon potential, foldeddiagram
expansion.
Nuclear Structure: 2 H; calculated electric, magnetic form factors. Impulse approximation, folded diagram potential.

92Ha14 Nuclear Excitation and Prompt Fission in Muonic 238 U
H. Hanscheid, P. David, H. Folger, J. Konijn, C. T. A. M. de Laat, C. Petitjean, H. W. Reist, F. Risse, Ch. Rosel, L. A. Schaller,
L. Schellenberg, W. Schrieder, L. M. Simons, A. Taal, Z. Phys. A342, 111 (1992).
Nuclear Reactions: 238 U(μ - ,F), E at 43 MeV/c; measured fission (fragment)γ-, γγ-, muonic (X-ray)(fragment)-coin, (Xray)(fragment)(t);
deduced fission barrier augmentation, nonradiative transitions role, fission probabilities.
Atomic Physics: esic-Atoms 238 U(μ - ,F), E at 42 MeV/ c; measured fission (fragment)γ-, γγ-, muonic (X-ray)(fragment)-coin, (Xray)(fragment)(t);
deduced fission barrier augmentation, nonradiative transtions role, fission probabilities.

92Ha15 High Temperature Gas Proportional Detector Techniques and Application to the Neutrino Mass Limit using 163 Ho
F. X. Hartmann, R. A. Naumann, Nucl. Instrum. Methods Phys. Res. A313, 237 (1992)
Radioactivity: 163 Ho, 55 Fe(EC); measured X-ray spectra; deduced electron neutrino mass limit. High temperature gas proportional
detector, calorimetric technique, gaseous organometallic 163 Ho sources.

92Ha16 Microscopic and Phenomenological Analysis of the Alaga Rule for Dipole States
E. Hammaren, P. Heikkinen, K. W. Schmid, A. Faessler, Nucl. Phys. A541, 226 (1992).
Nuclear Structure: 156 Gd, 164 Dy; calculated B(M1), γ-branching ratio for dipole excitations. Microscopic approach. Alaga rule
phenomenological analysis.

92Ha17 Microscopic Approach to the Generator Coordinate Method with Pairing Correlations and Density-Dependent Forces
Q. Haider, D. Gogny, J. Phys. (London) G18, 993 (1992).
Nuclear Structure: 16 O; calculated Skyrme, kinetic, spin-orbit, total energy. Generator coordinate method, Hill-Wheeler integral
equations, density-dependent forces.

92Ha18 Coupled-Channel Description of Rotational and Vibrational States in 20 Ne and 22 Ne
P. R. Hayes, N. M. Clarke, J. Phys. (London) G18, 1119 (1992).
Nuclear Reactions: 20 , 22 Ne(t,t’), ( 3 He, 3 He’), E=33.4 MeV; analyzed σ(θ). 20 , 22 Ne levels deduced J, π, band assignment. Vibrational
states, coupled-channels method.

92Ha19 Parity-Violating Asymmetry in Quasielastic e-d Scattering
E. Hadjimichael, G. I. Poulis, T. W. Donnelly, Phys. Rev. C45, 2666 (1992).
Nuclear Reactions: 2 H(polarized e,e’X), E not given; calculated parity violating asymmetry. Standard electroweak interaction
model, final state interactions.

92Ha20 On the Symmetric Fragmentation Barrier at Finite Temperature
F. Haddad, G. Royer, J. Phys. (London) G18, L153 (1992).
Nuclear Structure: 139 La; calculated potential energy, fragmentation barriers vs fragment number, temperature. Liquid-drop
model, nuclear proximity effects.

92Ha21 Double Neutron Capture in 62 Ni
A. Harder, S. Michaelsen, A. Jungclaus, K. P. Lieb, A. P. Williams, H. G. Borner, M. Trautmannsheimer, Z. Phys. A343, 7
(1992).
Nuclear Reactions: 62 Ni(n,γ), E=thermal; measured Eγ, Iγ. 63 , 64 Ni deduced levels, J, π, transition Iγ. Double neutron capture on
62 Ni leads to 63 Ni(n,γ) reaction.

92Ha22 Spontaneous Fission Properties of 259 Lr 103
T. M. Hamilton, K. E. Gregorich, D. M. Lee, K. R. Czerwinski, N. J. Hannink, C. D. Kacher, B. Kadkhodayan, S. A. Kreek, M. J.
Nurmia, M. R. Lane, M. P. Neu, A. Turler, D. C. Hoffman, Phys. Rev. C46, 1873 (1992).
Nuclear Reactions: 248 Cm( 15 N,4n), E=81 MeV; measured Eα, Iα.
Radioactivity: 259 Lr(α), (SF) [from 248 Cm( 15 N, 4n), E=81 MeV]; measured Eα, Iα, T 1/2 , fission fragment mass, kinetic energy distribution,
SF- to α-decay ratio.

92Ha23 Interaction Strength of Two Crossing Bands
G. B. Hagemann, I. Hamamoto, Phys. Rev. C46, 838 (1992).
Nuclear Structure: 156 Dy, 158 , 160 , 164 Er, 160 , 162 , 164 , 166 Yb, 164 , 166 Hf; analyzed level data; deduced crossing band interaction
strength. 155 , 157 , 159 , 161 Dy, 157 , 159 , 161 , 163 , 165 Er, 161 , 163 , 165 , 167 Yb, 167 , 169 , 171 Hf; analyzed level energy difference data.
157 Ho deduced band interaction strength dependence on n-p interaction details.

92Ha24 Spin-Dependent np Total Cross Section
P. Haffter, C. Brogli-Gysin, J. Campbell, D. Fritschi, J. Gotz, M. Hammans, R. Henneck, J. Jourdan, G. Masson, L. M. Qin, S.
Robinson, I. Sick, M. Tuccillo, J. A. Konter, S. Mango, B. van den Brandt, Nucl. Phys. A548, 29 (1992).
Nuclear Reactions: 1 H(polarized n,n), E=66 MeV; measured spin dependent σ difference. Comparison with phase shift analyses.
Polarized target.

92Ha25 Exchange Effects in β Decays of Many-Electron Atoms
M. R. Harston, N. C. Pyper, Phys. Rev. A45, 6282 (1992).
Radioactivity: 106 Ru, 241 Pu(β - ); calculated exchange effects role in β-decay, β-spectrum enhancement. Many-electron systems,
screened hydrogenic, Hartree-Fock approximations.

92Ha26 Can One Discriminate between Meson-Exchange and Quark-Gluon Transition Mechanisms in the (p-bar)p → (Lambdapar)Lambda
Process ( Question )
J. Haidenbauer, K. Holinde, V. Mull, J. Speth, Phys. Lett. 291B, 223 (1992).
Nuclear Reactions: 1 H(p-bar,X), E=1.546 GeV/c; analyzed polarization, depolarization data, (lambda)(lambda-bar) production;
deduced model discrimination possibility.

92Ha27 Determination of Technetium-99 in Environmental Material with Rhenium as a Yield Monitor
B. R. Harvey, K. J. Williams, M. B. Lovett, R. D. Ibbett, J. Radioanal. Nucl. Chem. 158, 417 (1992).

92Ha28 Gamow-Teller Strength in β-Decay of 25 Si
S. Hatori, H. Miyatake, S. Morinobu, K. Katori, M. Fujiwara, I. Katayama, N. Ikeda, T. Fukuda, T. Shinozuka, K. Ogawa, Nucl.
Phys. A549, 327 (1992).
Radioactivity: 25Si(β + p) [from 24Mg( 3He, 2n) reaction]; measured T , β-delayed Ep, Ip, βp-coin. 1/2 25Si deduced proton branching
ratio, β strength function. 25Al deduced level. Natural Mg target, surface barrier Si detector, ΔE-ΔE-E plastic scintillation β- telescope,
recoil mass separation. Model comparison.

92Ha29 Meson-Exchange and Quark-Gluon Transitions in the (p-bar)p → (Lambda-bar)(Lambda) Process
J. Haidenbauer, K. Holinde, V. Mull, J. Speth, Phys. Rev. C46, 2158 (1992).
Nuclear Reactions: 1 H(p-bar,X), (polarized p-bar,X), E at 1.4-1.9 GeV/c; calculated σ(E), σ(θ), spin observables, for (Lambdabar)(Lambda)
production. Meson exchange, quark-gluon transitions.

92Ha30 Temperature-Dependent Relativistic Microscopic Optical Potential of a Nucleon
Y. -L. Han, Q. -B. Shen, Y. -Z. Zhuo, Phys. Rev. C46, 2396 (1992).
Nuclear Reactions: 208 Pb(p,p), E=relativistic; calculated optical, Schrodinger-equivalent potentials, nucleon mean free paths.
Walecka meson-nucleon model, thermofield dynamics models.

92Ha31 Antihyperon-Hyperon Production in the Meson Exchange Framework
J. Haidenbauer, K. Holinde, J. Speth, Phys. Rev. C46, 2516 (1992).
Nuclear Reactions: 1 H(p-bar,X), E at 1.695-1.922 GeV/c; calculated strangeness production σ(θ), polarization vs θ.
Antihyperon-hyperon production, meson exchange framework.

92Ha32 Magnetic Dipole Strength in Superdeformed Nuclei
I. Hamamoto, W. Nazarewicz, Phys. Lett. 297B, 25 (1992).
Nuclear Structure: 192 Hg, 152 Dy; calculated B(M1), superdeformed nuclei; deduced isovector GQR, scissors mode overlap.

92Ha33 Simple, Fast Algorithm for Gamma-Ray Absorbed Dose Rate Calculations by Computer
P. L. Hargittai, Appl. Radiat. Isot. 43, 1412 (1992).

92Ha34 New Developments and Trends in NMR-ON
E. Hagn, Hyperfine Interactions 75, 229 (1992).
Compilation: 186 , 198 Au, 191 Pt, 171 , 173 Lu, 87m , 89m , 91m Y, 90m Zr, 184 Ir; compiled, reviewed data on NMR on oriented nuclei.

92Ha35 Nuclear Superdeformation Data Tables
X. -L. Han, C. -L. Wu, At. Data Nucl. Data Tables 52, 43 (1992).
Compilation: A=130, 150, 190; compiled Iγ for transitions in superdeformed bands.

92Ha36 Differential Cross Sections and Analysing Powers for (P-bar)P → π - π + and K - K + from 360 to 1550 MeV/c
A. Hasan, D. V. Bugg, J. R. Hall, R. L. Shypit, F. Tessarotto, R. Birsa, F. Bradamante, S. Dalla Torre-Colautti, A. Martin, A.
Penzo, P. Schiavon, A. Villari, S. Degli-Agosti, E. Heer, C. Lechanoine-Leluc, Y. Onel, D. Rapin, R. Kunne, K. Bos, J. C.
Kluyver, L. Linssen, A. S. Clough, Nucl. Phys. B378, 3 (1992).
Nuclear Reactions: 1 H(p-bar,π + π - ), (p-bar,K + K - ), E at 360-1550 MeV/c; measured analyzing power, σ(θ).

92Ha37 Improvement of RBS Detection Limits by Channeling
V. Havranek, V. Hnatowicz, J. Kvitek, V. Perina, Nucl. Instrum. Methods Phys. Res. B72, 224 (1992)
Nuclear Reactions: Si, S, Zn, Pb, Cl, K, Fe, Mo, Sb(α,α), E=1.3 MeV; measured yield vs E, backscattering; deduced detection
limits improvement. Aligned geometry.

92Ha38 What is the Spin of the 17-keV Neutrino ( Question )
A. Halprin, Phys. Rev. D46, R1903 (1992).

92Ha39 4 He(K - ,π±) Experiments at KEK and BNL
R. S. Hayano, Nucl. Phys. A547, 151c (1992).
Nuclear Reactions: 3 , 4 He(K - ,π - ), (K - , π + ), E at 600 MeV/c; measured spectra; deduced structure in 4 He(K - ,π - ) spectrum.

92Ha40 Production and Structure of Light Σ-Hypernuclei
T. Harada, Nucl. Phys. A547, 165c (1992).
Nuclear Reactions: 4 He(K - ,π - ), (K - ,π + ), E at 600 MeV/c; calculated Σ-hypernucleus production spectra, σ(θ(π,E(π))). DWBA
framework, complex nucleus-Σ potential.

92Ha41 Proton NMR Study of the Spin Structure of Mixed Antiferromagnets CO(1-x)Ni(x)Cl 2 .6H 2 O
T. Hamasaki, H. Kubo, J. Phys. Soc. Jpn. 61, 3287 (1992).
Nuclear Moments: +1}H; measured NMR; deduced mixed antiferromagnets CO(1-x)Ni(x)Cl 2 .6H 2 O spin structure.

92Ha42 New Production Systems at ISOLDE
E. Hagebo, P. Hoff, O. C. Jonsson, E. Kugler, J. P. Omtvedt, H. L. Ravn, K. Steffensen, Nucl. Instrum. Methods Phys. Res.
B70, 165 (1992)
Nuclear Reactions: Pt( 3 He,xnyp), E not given; Sn( 3 He,xnyp), E=910 MeV; measured production yields for Au, Hg, Cd isotopes.
Pt/graphite, Sn/graphite targets. U(p, X), E=600 MeV; measured production yields for Ne, Na, Mg, Al, Mn, Cu, Zn, Ga, Ge, As,
Ag, Cd, In, Sn, Sb, Te, Hg, Tl, Pb, Bi, Po isotopes. Uranium carbide with hot plasma ion source, data on Ta, Nb foil targets with W
surface ionizer and CF 4 leak also discussed.

92Ha43 Indirect Measurements of Beam-Energy Differences for Various Species of Ions Extracted from a FEBIAD Source
E. Hagberg, K. S. Sharma, G. R. Dyck, V. T. Koslowsky, P. P. Unger, J. C. Hardy, H. Schmeing, R. C. Barber, Nucl. Instrum.
Methods Phys. Res. B70, 546 (1992)
Nuclear Reactions: 92 Mo( 19 F,X), E=98 MeV; 92 Mo( 16 O, X), E=92 MeV; 92 Mo( 14 N,X), E=70 MeV; compiled, reviewed mass 106,
107, 108 radioactive beam production data; deduced beam energy differences for various ion species.

92HaZI Production and Structure of Light Σ-Hypernuclei
T. Harada, Y. Akaishi, RIKEN-91, p. 26 (1992).
Nuclear Reactions: 4 He(K - ,π - ), (K - ,π + ), E at 600 MeV/c; calculated σ(θ,E) for Σ-hypernucleus production; deduced hypernuclear
structure.

92HaZJ Final State Interaction in the 2 H(d(pol),pp)nn Reaction
T. Hayashi, K. Fukunaga, S. Kakigi, A. Okihana, T. Sekioka, T. Konishi, RCNP (Osaka), Ann. Rept., 1991, p. 29 (1992).
Nuclear Reactions: 2 H(polarized d,2p), E=59 MeV; measured σ(θ, E). Final state interaction.

92HaZK Study of the Superdeformed Bands in 194 Pb with EUROGAM
F. Hannachi, M. G. Porquet, G. Bastin, I. Deloncle, B. Gall, C. Schuck, A. G. Smith, F. Azaiez, C. Bourgeois, J. Duprat, A.
Korichi, N. Perrin, N. Poffe, H. Sergolle, A. Astier, Y. Le Coz, M. Meyer, N. Redon, M. Bentley, J. Simpson, J. F. Sharpey-
Schafer, M. J. Joyce, C. W. Beausang, P. Fallon, E. S. Paul, P. J. Dagnall, S. A. Forbes, S. Gale, P. M. Jones, R. Wadsworth,
R. M. Clark, M. M. Aleonard, D. Curien, Proc. Int. Conf. Nuclear Structure at High Angular Momentum, Ottawa, p. 384 (1992);
AECL-10613 (1992)
Nuclear Reactions: 162 Dy( 36 S,4n), E=162 MeV; measured Eγ, Iγ, γγ-coin, DSA. 194 Pb deduced levels, J, π, quadrupole moment,
superdeformed band, normally deformed band transitions.

92HaZL Low-Energy E1 Transitions and Octupole Softness in Odd-A Deformed Nuclei
G. B. Hagemann, I. Hamamoto, J. Kownacki, W. Satula, Proc. Int. Conf. Nuclear Structure at High Angular Momentum, Ottawa,
p. 327 (1992); AECL-10613 (1992)
Nuclear Structure: 169 Lu; calculated B(λ). One-quasiparticle coupled to a rotor.

92HaZM Shape Coexistence, Lanczos Techniques, and Large-Basis Shell-Model Calculations
W. C. Haxton, Proc. Int. Conf. Nuclear Structure at High Angular Momentum, Ottawa, p. 294 (1992); AECL-10613 (1992)
Nuclear Structure: 16 O; calculated levels, Gamow-Teller transition strength, B(λ), 4p-4h probabilities. 68 , 70 , 72 , 74 , 76 , 78 Ge, 70 ,
72 , 74 , 76 , 78 , 80 Se; calculated levels, occupation numbers. Lanczos algorithm based many-body techniques.

92HaZN A Superdeformed Band in 142 Sm
G. Hackman, S. M. Mullins, J. A. Kuehner, D. Prevost, J. C. Waddington, A. Galindo-Uribarri, V. P. Janzen, D. C. Radford, N.
Schmeing, D. Ward, Proc. Int. Conf. Nuclear Structure at High Angular Momentum, Ottawa, p. 203 (1992); AECL-10613 (1992)
Nuclear Reactions: 124 Sn( 24 Mg,6n), E=145 MeV; measured γγ-coin. 142 Sm deduced levels, J, π, superdeformed band, dynamic
moment of inertia.

92HaZO Test of the Nucleus-Σ Potential by 4 He(Stopped K - ,π + ) Spectrum
T. Harada, Contrib. 13th Int. Conf. on Few-Body Problems in Physics, Adelaide, Australia, January 5-11, 1992, I. R. Afnan, R.
T. Cahill, Eds., p. 392 (1992)
Nuclear Reactions: 4 He(K - ,π + ), E at rest; calculated spectra; deduced triton+Σ - -interaction role.

92HaZP Determination of the Semi-Leptonic Weak Interaction Pseudoscalar Coupling Constant, gp, Using the Reaction μ - p → ν(μ)nγ
M. D. Hasinoff, D. S. Armstrong, G. Azuelos, W. Bertl, M. Blecher, C. Q. Chen, P. Depommier, B. Doyle, T. von Egidy, T. P.
Gorringe, P. Gumplinger, R. Henderson, G. Jonkmans, A. J. Larabee, J. A. Macdonald, S. C. McDonald, M. Munro, J. -M.
Poutissou, R. Poutissou, B. C. Robertson, D. G. Sample, W. Schott, G. N. Taylor, S. Veillette, D. H. Wright, and the RMC Collaboration,
Contrib. 13th Int. Conf. on Few-Body Problems in Physics, Adelaide, Australia, January 5-11, 1992, I. R. Afnan, R.
T. Cahill, Eds., p. 252 (1992)
Nuclear Reactions: 1 H(μ - ,n), E at rest; compiled, reviewed status; discussed new data measurement efforts.

92HaZQ Meson Exchange Model for the (p-bar)p → (Lambda-bar)(Lambda) Reaction
J. Haidenbauer, T. Hippchen, K. Holinde, B. Holzenkamp, V. Mull, J. Speth, Contrib. 13th Int. Conf. on Few-Body Problems in
Physics, Adelaide, Australia, January 5-11, 1992, I. R. Afnan, R. T. Cahill, Eds., p. 164 (1992)
Nuclear Reactions: 1 H(p-bar,X), E at 1450-1900 MeV/c; calculated σ(θ), σ(E), polarization vs θ for (lambda)(lambda-bar) production;
deduced strangeness production model dependence.

92HaZR Studies of Superdeformation in the A = 150 Region
B. Haas, V. P. Janzen, D. Ward, H. R. Andrews, D. C. Radford, D. Prevost, J. A. Kuehner, A. Omar, J. C. Waddington, T. E.
Drake, A. Galindo-Uribarri, G. Zwartz, S. Flibotte, P. Taras, I. Ragnarsson, TASCC-P-92-11 (1992).
Nuclear Reactions: 124 , 122 , 120 Sn( 30 Si,xn), ( 29 Si,xn), ( 28 Si,xn), E=155 MeV; measured Eγ, Iγ, γγ-coin, DCO ratios. 149 , 148 , 147 ,
146 , 145 Gd deduced levels, J, π, superdeformed bands, γ-ray multiplicities, total γ-ray sum energy. Compton-suppressed hyperpure
Ge detector array, 4π-bismuth germanate ball. Cranked shell-model-Strutinski calculations.

92HaZS Gamow-Teller Strength in β-Decay of sd-Shell Proton Rich Nuclei with Tz = -(3/2)
S. Hatori, H. Miyatake, T. Shimoda, N. Takahashi, Y. Fujita, S. Morinobu, Contrib. 6th Intern. Conf. on Nuclei Far from Stability
+ 9th Intern. Conf. on Atomic Masses and Fundamental Constants, Bernkastel-Kues, Germany, PF3 (1992)
Radioactivity: 21 Mg, 25 Si, 29 S, 37 Ca(β + p); measured β-spectra. 25 Al, 29 P deduced Gamow-Teller transition strength distribution.

92HaZT Recent Results and Future Prospects Along the N = Z Line with Radioactive Nuclear Beams and RMS
J. H. Hamilton, A. V. Ramayya, Contrib. 6th Intern. Conf. on Nuclei Far from Stability + 9th Intern. Conf. on Atomic Masses and
Fundamental Constants, Bernkastel-Kues, Germany, PE10 (1992)
Nuclear Structure: 72 , 74 , 76 Kr; reviewed, analyzed data. 88 Ru; analyzed band structure; deduced low spin superdeformation.
Nuclei along N=Z line.

92HaZU β Transitions to Non-Analogue 0 + States and the Impact on Superallowed Decay Rates
E. Hagberg, V. T. Koslowsky, T. Shinozuka, J. G. Hykawy, J. C. Hardy, G. Savard, P. P. Unger, H. Schmeing, I. S. Towner,
Contrib. 6th Intern. Conf. on Nuclei Far from Stability + 9th Intern. Conf. on Atomic Masses and Fundamental Constant,
Bernkastel-Kues, Germany, F3 (1992).
Radioactivity: 46 V(β + ); 50 Mn(β + ); 54 Co(β + ); measured γ-spectra. 50 Mn deduced superallowed β-branch log ft, allowed Gamow-
Teller β branches. 54 Fe deduced 0 + state population evidence. Set-up sensitive to low intensity branches.

92HaZV Precision Neutron Binding Energies of 59 , 63 , 64 Ni and 90 Y Obtained from Thermal Neutron Capture Reactions
A. Harder, S. Michaelsen, A. Jungclaus, K. P. Lieb, A. P. Williams, H. G. Borner, Contrib. 6th Intern. Conf. on Nuclei Far from
Stability + 9th Intern. Conf. on Atomic Masses and Fundamental Constant, Bernkastel-Kues, Germany, PA4 (1992)
Nuclear Reactions: 89 Y, 58 , 62 Ni(n,γ), E=thermal; measured γ-spectra following capture. 90 Y, 64 , 63 , 59 Ni deduced binding energy,
Iγ, intermediate states.

92HaZW Low-Energy E1 Transitions and Octupole Softness in Odd-A Deformed Nuclei
G. B. Hagemann, I. Hamamoto, J. Kownacki, W. Satula, Contrib. Int. Conf. Nuclear Structure at High Angular Momentum,
Ottawa, p. 114 (1992); AECL-10613 (1992)
Nuclear Structure: 169 Lu; analyzed B(E1) data; deduced octupole softness role. Particle-rotor model.

92HaZX A Superdeformed Rotational Band in 142 Sm
G. S. Hackman, A. Galindo-Uribarri, V. P. Janzen, S. M. Mullins, D. Prevost, D. C. Radford, J. C. Waddington, D. Ward, Contrib.
Int. Conf. Nuclear Structure at High Angular Momentum, Ottawa, p. 81 (1992); AECL-10613 (1992)
Nuclear Reactions: 124 Sn( 24 Mg,6n), E=145 MeV; measured γ-multiplicity, total sum energy. 142 Sm deduced levels, J, π, dynamical
moment of inertia, superdeformed rotational band.

92HaZY Study of the Superdeformed Band in 194 Pb with Eurogam
F. Hannachi, Contrib. Int. Conf. Nuclear Structure at High Angular Momentum, Ottawa, p. 67 (1992); AECL-10613 (1992)
Nuclear Reactions: 164 , 162 Dy( 32 S,X), ( 36 S,X), E=157-162 MeV; measured γγγ-coin, DSA. 194 Pb deduced superdeformed band
states T 1/2 , decay features.

92HaZZ A Heavy-Ion Study of the Structure of 18 Ne and the Breakout from the Hot CNO Cycle
K. I. Hahn, N. Bateman, B. J. Lund, S. Utku, A. J. Howard, P. D. Parker, Bull. Am. Phys. Soc. 37, No. 2, 868, A7 7 (1992)
Nuclear Reactions: 12 C( 12 C, 6 He), E not given; meaured σ(E( 6 He)). 18 Ne deduced levels.

92He01 Nuclear Data Sheets Update for A=156
R. G. Helmer, Nucl. Data Sheets 65, 65 (1992).
Compilation: 156 Nd, 156 Pm, 156 Sm, 156 Eu, 156 Gd, 156 Tb, 156 Dy, 156 Ho, 156 Er, 156 Tm, 156 Yb, 156 Lu, 156 Hf, 156 Ta; compiled,
evaluated structure data.

92He02 Multistep-Compound Contribution to Precompound Reaction Cross Section
M. Herman, G. Reffo, H. A. Weidenmuller, Nucl. Phys. A536, 124 (1992).
Nuclear Reactions: 93 Nb(n,n’), E=14.6 MeV; 93 Nb(n,xn), E=13.47 MeV; calculated nucleon spectra, angle integrated σ. Multistep
compound reactions.

92He03 Rotational Band Structures in 129 La
Y. He, M. J. Godfrey, I. Jenkins, A. J. Kirwan, S. M. Mullins, P. J. Nolan, E. S. Paul, R. Wadsworth, J. Phys. (London) G18, 99
(1992).
Nuclear Reactions: 51 V( 82 Se,4n), E=290 MeV; measured γγ-coin, Iγ, DCO ratios. 129 La deduced levels, J, π, B(λ) ratios, band
structure, configurations. Cranked shell model.

92He04 Comment on the Trinucleon Electromagnetic Form Factors
H. Henning, P. U. Sauer, W. Theis, Nucl. Phys. A537, 367 (1992).
Nuclear Reactions: 3 H, 3 H(e,e), E not given; calculated form factors. Paris, Bonn potentials.

92He05 Three-Dimensional γ-Ray Correlations and the Study of Rotational Damping in 167 , 168 Yb
B. Herskind, T. Dossing, D. Jerrestam, K. Schiffer, S. Leoni, J. Lisle, R. Chapman, F. Khazaie, J. N. Mo, Phys. Lett. 276B, 4
(1992).
Nuclear Reactions: 124 Sn( 48 Ca,X), E=208 MeV; measured γγγ-energy correlations. 167 , 168 Yb deduced rotational damping width.

92He06 Comparison of Nucleon-Nucleon Potential Models in Proton-Proton Bremsstrahlung
V. Herrmann, K. Nakayama, Phys. Rev. C45, 1450 (1992).
Nuclear Reactions: 1 H(polarized p,γ), E=280 MeV; calculated σ(θ 1 ,θ 2 ,θ), analyzing power. Relativistic approach, ppbremsstrahlung.

92He07 Fluctuation Analysis of Rotating Decay from Excited Nuclei
B. Herskind, A. Bracco, R. A. Broglia, T. Dossing, A. Ikeda, S. Leoni, J. Lisle, M. Matsuo, E. Vigezzi, Phys. Rev. Lett. 68,
3008 (1992).
Nuclear Structure: 167 , 168 Yb; analyzed transition energy data. Fluctuation analysis, high-spin quasicontinuum.

92He08 Study of Decay and Absorption of the Δ Resonance in Nuclei with a 4π Detector
T. Hennino, B. Ramstein, D. Bachelier, H. G. Bohlen, J. L. Boyard, C. Ellegaard, C. Gaarde, J. Gosset, J. C. Jourdain, J. S.
Larsen, M. C. Lemaire, D. L’Hote, H. P. Morsch, M. Osterlund, J. Poitou, P. Radvanyi, M. Roy-Stephan, T. Sams, K. Sneppen,
O. Valette, P. Zupranski, Phys. Lett. 283B, 42 (1992).
Nuclear Reactions: 1 , 2 H, 12 C( 3 He,t), E=2 GeV; measured energy transfer spectra, (π + p)(t)-coin; deduced Δ-resonance decay,
absorption mechanism.

92He09 Many Body Modes of Antiproton Annihilation Tested with Antiproton Production
E. Hernandez, E. Oset, Z. Phys. A341, 201 (1992).
Nuclear Reactions: 12 C, 40 Ca(γ,p-bar), E > 3.8 GeV; 12 C, 40 Ca(p,p-bar), E=8 GeV; calculated reaction σ; deduced p-bar annihilation
mechanism role.

92He10 Precision Measurement of Antiprotonic Hydrogen and Deuterium X-Rays
K. Heitlinger, R. Bacher, A. Badertscher, P. Blum, J. Eades, J. Egger, K. Elsener, D. Gotta, E. Morenzoni, L. M. Simons, Z.
Phys. A342, 359 (1992).
Atomic Physics: +1}, 2 H(p-bar,X), E at 105 MeV/c; measured X-ray spectra; deduced Lyman α transition shift, width.

92He11 Intruder Analog States: New classification of particle-hole excitations near closed shells
K. Heyde, C. De Coster, J. Jolie, J. L. Wood, Phys. Rev. C46, 541 (1992).
Nuclear Structure: 110 Ru, 114 Cd, 118 Te, 122 Ba; calculated levels, B(λ); deduced intruder spin, analog states role. Interacting
boson approximation model.

92He12 First Forbidden β-Decays as a Probe of T-Odd Nuclear Forces
E. M. Henley, I. B. Khriplovich, Phys. Lett. 289B, 223 (1992).
Radioactivity: 11Be, 17N(β- ); 18Ne(β + ); 19Ne(β + ), (EC); 36K(β + ); 39Cl(β- ); 107Cd(β + )(EC); 154Eu(β- ), (EC); 169Hf(EC), (β + ); 231Th(β- );
235 - Pa(β ); calculated square root of branching ratio for decay to final levels; deduced enhancements due to level mixing caused by
T-odd forces.

92He13 Band Structure in the Neutron-Rich Lanthanide Nucleus 152 Nd. I. Anomalous Properties of the K(π) =0 + Bands
M. Hellstrom, B. Fogelberg, H. Mach, D. Jerrestam, L. Spanier, Phys. Rev. C46, 860 (1992).
Radioactivity: 152 Pr(β - ); measured Eγ, Iγ, γγ-coin, γγ(θ); deduced log ft, orbital, pairing dependent structure effects. 152 Nd
deduced levels J, π, δ, band structure.

92He14 Proton 2p-2h Intruder Excitations and the Modified Vibrational Intensity and Selection Rules
K. Heyde, C. De Coster, J. L. Wood, J. Jolie, Phys. Rev. C46, 2113 (1992).
Nuclear Structure: 114 Cd; calculated intruder states, quadrupole phonon vibrational states; deduced modified vibrational intensity,
selection rules.

92He15 Evaporation Residues from Heavy (Z = 90-93) Compound Nuclei at Excitation Energies of E(X) (75-110) MeV
F. P. Hessberger, V. Ninov, D. Ackermann, Z. Phys. A343, 301 (1992).
Nuclear Reactions: 180 Hf, 181 Ta, 182 , 184 W, Re( 40 Ar, X), E=6.3 MeV/nucleon; measured evaporation residue σ(E). 232 Th( 40 Ar,X),
E=5.5-6.3 MeV/ nucleon; measured evaporation residue σ; deduced no evidence for transfermium isotope production.

92He16 High-Spin States in 66 , 68 Ge
U. Hermkens, F. Becker, J. Eberth, S. Freund, T. Mylaeus, S. Skoda, W. Teichert, A. von der Werth, Z. Phys. A343, 371
(1992).
Nuclear Reactions: 40 Ca( 32 S,2pα), ( 32 S,4p), E=100 MeV; 58 Ni( 16 O,2pα), E=65 MeV; measured γγ-coin, Iγ(θ). 66 , 68 Ge deduced
levels, J, π.

92He17 Manifestation of Quadrupole Collectivity in the Magnetc Dipole Strength
K. Heyde, C. De Coster, A. Richter, H. -J. Wortche, Nucl. Phys. A549, 103 (1992).
Nuclear Structure: 168 Er, 160 , 162 , 164 Dy, 154 , 156 , 158 , 160 Gd, 144 , 148 , 150 , 152 , 154 Sm, 142 , 146 , 148 , 150 Nd; analyzed B(λ) data;
deduced quadrupole collectivity features. Quasiparticle TDA, interacting boson model, sum rule approach.

92He18 Relativistic Effects in Proton-Proton Bremsstrahlung
V. Herrmann, K. Nakayama, Phys. Rev. C46, 2199 (1992).
Nuclear Reactions: 1 H(p,γ), (polarized p,γ), E=100, 280 MeV; calculated bremsstrahlung σ(θ 1 ,θ 2 , θ), analyzing power; deduced
rescattering role. Proton-proton bremsstrahlung, relativistic effects.

92He19 Gamma Emission in Precompound Reactions. II. Numerical Application
M. Herman, A. Horing, G. Reffo, Phys. Rev. C46, 2493 (1992).
Nuclear Reactions: 93 Nb, 59 Co, 181 Ta(n,γ), E=14.1 MeV; analyzed total γ-spectra. Precompound reactions, parameter free
interpretation.

92He20 A New High Flow 81 Rb/ 81m Kr Generator
J. D. M. Herscheid, L. F. Van Rooji, P. J. Van Leuffen, J. A. J. Camps, Appl. Radiat. Isot. 43, 1203 (1992).
Nuclear Reactions: 82 Kr(p,2n), E not given; measured 81m Kr yield following 81 Rb decay. Ion-exchange membrane, 81m Kr generator.

92He21 Nuclear Moments as a Test of Shell-Model and Collective Model Descriptions of the Nucleus
K. Heyde, Hyperfine Interactions 75, 69 (1992).
Nuclear Structure: 123 , 127 , 129 , 131 , 133 Sb, 141 , 143 , 145 , 147 , 149 , 151 , 153 Eu; calculated μ. 208 , 209 Po, 209 , 210 At, 210 , 211 Rn, 211 ,
212 Fr, 212 , 213 Ra; analyzed quadrupole moment systematics. 104 , 108 , 112 , 116 , 120 , 124 , 128 , 132 Sn; analyzed proton rms radii,
charge radii isotonic shifts. 4 He, 6 , 7 Li, 9 Be, 10 , 11 B, 12 , 13 , 14 C, 14 , 15 N, 16 O; analyzed charge rms radius systematics. Shell model
with collective effects.

92He22 Some Studies of Molecular Ions Obtained from a U + C Target at > 2100 0 C
M. Hellstrom, B. Fogelberg, L. Jacobsson, L. Spanier, G. Rudstam, Nucl. Instrum. Methods Phys. Res. B70, 142 (1992)

92HeZK Spectrum Fluctuations from Regular- and Damped Rotational Structures in 168 Yb and 163 Tm Nuclei
B. Herskind, T. Dossing, S. Leoni, M. Matsuo, N. Ninel, E. Vigezzi, A. Atac, P. Bosetti, M. Bergstrom, A. Bracco, A. Brockstedt,
R. A. Broglia, H. Carlsson, P. Ekstrom, H. J. Jensen, J. Jongman, G. B. Hagemann, F. Ingebretsen, R. M. Lieder, T.
Lonnroth, A. Maj, B. Million, A. Nordlund, J. Nyberg, M. Piiparinen, H. Ryde, M. Sugawara, P. O. Tjom, A. Virtanen, Proc. Int.
Conf. Nuclear Structure at High Angular Momentum, Ottawa, p. 470 (1992); AECL-10613 (1992)
Nuclear Reactions: 130 Te( 37 Cl,xn), E=160 MeV; analyzed γ sum coincidence spectra, multiplicity. 163 Tm deduced level decay
paths.
Nuclear Structure: 167 , 168 Yb, 163 Tm; analyzed data; deduced level decay paths.

92HeZL A New Recoil Filter for γ-Detector Arrays
J. Heese, W. Lahmer, K. H. Maier, M. Janicki, W. Meczynski, J. Styczen, Proc. Int. Conf. Nuclear Structure at High Angular
Momentum, Ottawa, p. 439 (1992); AECL-10613 (1992)
Nuclear Reactions: 154 , 156 Gd( 36 Ar,4n), E=175 MeV; measured γ(X-ray)-coin, γ-multiplicity, γγ(particle)-coin. 188 , 186 Pb deduced
transitions. Recoil filter detector.

92HeZM Superdeformation in the A = 190 Region: The lead nuclei
E. A. Henry, J. A. Becker, M. J. Brinkman, A. Kuhnert, M. A. Stoyer, T. F. Wang, S. W. Yates, F. A. Azaiez, C. W. Beausang,
J. Burde, M. A. Deleplanque, R. M. Diamond, J. E. Draper, W. H. Kelly, W. Korten, A. O. Macchiavelli, J. Oliveira, E. Rubel, F.
S. Stephens, J. A. Cizewski, Proc. Int. Conf. Nuclear Structure at High Angular Momentum, Ottawa, p. 15 (1992); AECL-10613
(1992)
Nuclear Reactions: 176 Yb( 26 Mg,6n), E=138 MeV; measured γγ-coin. 196 Pb deduced new levels in superdeformed band.
154 Sm( 48 Ca,X), E=205, 210 MeV; 176 Yb( 24 Mg, xn), E=129-134 MeV; 176 Yb( 26 Mg,xn), E=130, 135 MeV; measured not given. 197 ,
195 , 193 Pb deduced no superdeformed bands.
Nuclear Structure: 192 , 194 , 196 Pb; analyzed superdeformed band data.

92HeZN On the Relativistic Spin Correction in Proton-Proton Bremsstrahlung
V. Herrmann, K. Nakayama, KFA-IKP Ann. Rept., 1991, p. 186 (1992).
Nuclear Reactions: 1 H(polarized p,γ), E=280 MeV; calculated bremsstrahlung σ(θ 1 ,θ 2 )vsθγ; deduced relativistic spin correction.

92HeZO Spin Observables in pp Bremsstrahlung and Off-Shell Effects of the NN Interaction
V. Herrmann, K. Nakayama, KFA-IKP Ann. Rept., 1991, p. 183 (1992).
Nuclear Reactions: 1 H(polarized p,γ), E=280 MeV; calculated bremsstrahlung analyzing power, spin polarization observables vs
θ; deduced off-shell effects role.

92HeZP Rescattering Contribution to Proton-Proton Bremsstrahlung in a Relativistic Approach
V. Herrmann, K. Nakayama, KFA-IKP Ann. Rept., 1991, p. 180 (1992).
Nuclear Reactions: 1 H(p,γ), E=280 MeV; calculated bremsstrahlung σ(θ 1 ,θ 2 )vsθγ; deduced rescattering effects. Relativistic
approach.

92HeZQ Elastic Transfer in 11 B+ 12 C System at 344.5 MeV(Lab)
J. Hebenstreit, L. Jarczyk, B. Kamys, A. Magiera, W. Oelert, P. von Rossen, Z. Rudy, H. Seyfarth, A. Strzalkowski, B.
Styczen, KFA-IKP Ann. Rept., 1991, p. 118 (1992).
Nuclear Reactions: 11 B( 12 C, 12 C), E=344.5 MeV; measured σ(θ). 12 C level deduced spectroscopic factor.

92HeZR Transition Rates from Negative-Parity Bands in 152 Nd
M. Hellstrom, H. Mach, B. Fogelberg, D. Jerrestam, L. Spanier, Contrib. 6th Intern. Conf. on Nuclei Far from Stability + 9th
Intern. Conf. on Atomic Masses and Fundamental Constants, Bernkastel-Kues, Germany, PE39 (1992)
Radioactivity: 152 Pr(β - ); measured γγ(θ), βγγ(t). 152 Nd deduced levels, J, π, K, band structure, configuration.

92HeZS Anomalous Properties of the K(π) =0 + Bands of 152 Nd
M. Hellstrom, B. Fogelberg, H. Mach, D. Jerrestam, L. Spanier, Contrib. 6th Intern. Conf. on Nuclei Far from Stability + 9th
Intern. Conf. on Atomic Masses and Fundamental Constants, Bernkastel-Kues, Germany, PE38 (1992)
Nuclear Structure: 152 Nd; measured not given; deduced levels, J, π, K, band structure, γ-branching.

92HeZT Intruder Analog States: A new classification of coexisting particle-hole excitations near closed shells
K. Heyde, C. De Coster, J. Jolie, J. L. Wood, Contrib. 6th Intern. Conf. on Nuclei Far from Stability + 9th Intern. Conf. on Atomic
Masses and Fundamental Constant, Bernkastel-Kues, Germany, E8 (1992).
Nuclear Structure: 110 Ru, 114 Cd, 118 Te, 122 Ba; calculated levels, B(λ), band structure. 116 Sn, 112 Pd, 120 Xe analyzed band structure;
deduced intruder analog states, configuration. Interacting boson model.

92HeZU Proton and Alpha Radioactivity in the Vicinity of 100 Sn
F. Heine, T. Faestermann, A. Gillitzer, Contrib. 6th Intern. Conf. on Nuclei Far from Stability + 9th Intern. Conf. on Atomic
Masses and Fundamental Constant, Bernkastel-Kues, Germany, C14 (1992)
Radioactivity: 107 , 108 , 109 Te, 110 , 111 I, 110 , 111 , 112 Xe(α); measured Eα, Iα, αα(θ), pα(θ). 112 Cs deduced proton decay Q-value.

92HeZV Half-Lives of Short-Lived W-, Ta- and Hf-Isotopes as Determined in Model Experiments for the Chemical Separation of Element
106
W. Heller, R. Binder, H. Bruchertseifer, U. Becker, F. Haberberger, G. Herrmann, J. V. Kratz, M. Mendel, A. Nahler, M.
Pense-Maskow, N. Trautmann, N. Wiehl, W. Bruchle, E. Jager, M. Schadel, B. Schausten, J. Alstad, G. Skarnemark, R.
Dressler, S. Fischer, A. Ross, B. Eichler, S. Hubener, Univ. Mainz, 1991 Ann. Rept., p. 28 (1992).
Radioactivity: 166 , 167 , 168 , 169 , 170 , 171 W(α) [from Gd( 20 Ne,xn), E=170, 207 MeV]; 164 , 166 , 167 , 170 , 171 Ta(β + ), (EC). 162 , 163 , 164 ,
165 Hf [from 166 , 167 , 168 , 169 W(α-decay)]; measured Eγ, Iγ, T1/2 .

92HeZW A New Recoil Filter for γ-Detector Arrays
J. Heese, M. Janicki, W. Lahmer, K. H. Maier, W. Meczynski, J. Styczen, Contrib. Int. Conf. Nuclear Structure at High Angular
Momentum, Ottawa, p. 137 (1992); AECL-10613 (1992)
Nuclear Reactions: 124 Sn, 152 Sm( 40 Ar,X), E=185 MeV; 154 , 156 Gd( 36 Ar,X), E=175 MeV; measured Eγ, Iγ, γ(recoil)-coin. Detector
array, recoil filter.

92HeZX A Trace of Motional Narrowing ( Question )
B. Herskind, T. Dossing, S. Leoni, M. Matsuo, E. Vigezzi, A. Atac, M. Bergstrom, A. Bracco, A. Brockstedt, H. Carlsson, P.
Ekstrom, H. J. Jensen, J. Jongman, G. B. Hagemann, F. Ingebretsen, R. M. Lieder, T. Lonnroth, A. Maj, B. Million, A.
Nordlund, J. Nyberg, M. Piiparinen, H. Ryde, M. Sugawara, P. O. Tjom, A. Virtanen, Contrib. Int. Conf. Nuclear Structure at
High Angular Momentum, Ottawa, p. 103 (1992); AECL-10613 (1992)
Nuclear Reactions: 130 Te( 37 Cl,xn), E=166 MeV; measured γ-spectra, γ-multiplicity, sum energy gating. 163 Tm deduced effective
path number, rotational Γ. Fluctuation analysis, rotational plane mapping methods.

92HeZY Superdeformation in the A = 190 Region: The lead nuclei
E. A. Henry, J. A. Becker, M. J. Brinkman, A. Kuhnert, M. A. Stoyer, T. F. Wang, S. W. Yates, F. A. Azaiez, C. W. Beausang,
J. Burde, M. A. Deleplanque, R. M. Diamond, J. E. Draper, W. H. Kelly, W. Korten, A. O. Macchiavelli, E. Rubel, F. S.
Stephens, J. A. Cizewski, Contrib. Int. Conf. Nuclear Structure at High Angular Momentum, Ottawa, p. 73 (1992); AECL-10613
(1992)
Nuclear Structure: 192 , 194 , 196 , 198 Pb; analyzed data systematics; deduced superdeformed band states dynamic moment of inertia.
193 , 195 , 197 Pb; analyzed preliminary data.

92HeZZ Search for Berry’s Phase Effects in Deformed Nuclei
K. G. Helmer, C. Wu, D. Cline, A. E. Kavka, W. J. Kernan, E. G. Vogt, M. W. Guidry, X. L. Han, R. W. Kincaid, X. T. Liu, H.
Schecter, J. O. Rasmussen, A. Shihab-Eldin, M. A. Stoyer, M. L. Halbert, I. Y. Lee, Bull. Am. Phys. Soc. 37, No. 2, 871, A8
11 (1992)
Nuclear Reactions: 156 Gd( 206 Pb, 204 Pb), ( 206 Pb, 208 Pb), E=888 MeV; measured γ(particle)-coin, γ-multiplicity. 154 , 158 Gd deduced
levels, J, π.

92Hi01 Determination of Neutron and Proton Multipole Matrix Elements in 208 Pb from π - and π + Scattering at 180 MeV
N. M. Hintz, X. H. Yang, M. Gazzaly, S. J. Seestrom-Morris, C. L. Morris, D. C. Cook, A. M. Mack, J. W. McDonald, S. Mordechai,
D. S. Oakley, C. F. Moore, M. Lynker, J. D. Zumbro, Phys. Rev. C45, 601 (1992).
Nuclear Reactions: 208 Pb(π + ,π + ), (π + , π + ’), (π - ,π - ’), (π - , π - ), E=180 MeV; measured σ(θ). 208 Pb levels deduced neutron, proton
multipole matrix elements.

92Hi02 Coupled-Channels Study of Polarized 6 Li Scattering at 44 MeV
Y. Hirabayashi, Y. Sakuragi, Nucl. Phys. A536, 375 (1992).
Nuclear Reactions: 26 Mg, 120 Sn(polarized 6 Li, 6 Li), E=44 MeV; analyzed σ(θ), vector, tensor analyzing power vs θ. Coupledchannels
theory.

92Hi03 Double K-Shell Vacancy Production in the Electron Capture Decay of 125 I
M. M. Hindi, R. L. Kozub, Phys. Rev. C45, 1070 (1992).
Radioactivity: 125 I(EC); measured (γ)X-, X-ray triple-coin; deduced double K-shell vacancy production. Hyperpure Ge detectors.

92Hi04 Modifications of the Tensor and Spin-orbit Interactions and the Stretched States in 208 Pb
N. M. Hintz, A. M. Lallena, A. Sethi, Phys. Rev. C45, 1098 (1992).
Nuclear Reactions: 208 Pb(p,p’), E=318 MeV; analyzed σ(θ). 208 Pb(e,e’), E=335.4 MeV; analyzed σ(θ); deduced quenching factors,
effective masses.

92Hi05 Neutron Emission as a Probe of Fusion-Fission and Quasifission Dynamics
D. J. Hinde, D. Hilscher, H. Rossner, B. Gebauer, M. Lehmann, M. Wilpert, Phys. Rev. C45, 1229 (1992).
Nuclear Reactions: U, 197 Au, 169 Tm, 154 , 144 Sm, 124 Sn( 18 O,nF), E=158.8 MeV; U, 208 Pb, 197 Au, 184 W, 154 Sm, 109 Ag( 16 O, nF),
E=288 MeV; U, 208 Pb, 197 Au, 181 Ta, 165 Ho, 169 Tm, 141 Pr( 40 Ar,nF), E=249 MeV; U, 208 Pb, 197 Au, 175 Lu, 154 Sm( 64 Ni,nF), E=417.7
MeV; measured fission (fragment)n(θ), σ(fragment mass,total kinetic energy); deduced pre-, post-scission neutron multiplicities,
pre-scission time-scales.

92Hi06 Search for Light Neutral Boson Associated with Beta Decay
K. H. Hicks, D. E. Alburger, Phys. Lett. 276B, 423 (1992).
Radioactivity: 35 S(β - ); measured γγ-coin; deduced no evidence for light neutral boson. High parity Ge low energy photon detectors.

92Hi07 Ground-State Properties of Neutron-Deficient Platinum Isotopes
Th. Hilberath, St. Becker, G. Bollen, H. -J. Kluge, U. Kronert, G. Passler, J. Rikovska, R. Wyss, and the ISOLDE Colloration,
Z. Phys. A342, 1 (1992).
Nuclear Moments: +198}, 196 , 195 , 194 , 193 , 192 , 190 Pt; measured hfs, isotope shift; deduced μ, quadrupole moments, rms charge
radii, quadrupole moments. Particle-triaxial rotor model, mean field calculations. Other isotopes studied. Resonance ionization
mass spectroscopy, pulser-laser induced desorption techniques, Pt isotopes produced as daughters of Hg-isotopes obtained from
on-line isotope separator.
Radioactivity: 183 , 184 , 185 , 185m , 186 , 187 , 188 , 189 , 190 , 191 Pt; measured hfs, isotope shift; deduced μ, quadrupole moments, rms
charge radii, quadrupole moments. Particle-triaxial rotor model, mean field calculations. Other isotopes studied. Resonance ionization
mass spectroscopy, pulser-laser induced desorption techniques, Pt isotopes produced as daughters of Hg-isotopes
obtained from on-line isotope separator.

92Hi08 Lambda Polarization in 12 C(π - ,Lambda) Reactions at p(π) = 4 GeV/c
S. Hirenzaki, F. Iseki, K. -I. Kubo, Z. Phys. A343, 471 (1992).
Nuclear Reactions: 12 C(π - ,X), E at 4 GeV/c; calculated inclusive lambda production σ vs E(lambda). Regge pole amplitudes
approach.

92Hi09 High-Spin Phenomena in 174 Os
L. Hildingsson, W. Klamra, Th. Lindblad, C. G. Linden, B. Cederwall, W. Satula, R. Wyss, C. Kalfas, S. Kossionides, C. T.
Papadopoulos, R. Vlastou, J. Gizon, D. Clarke, F. Khazaie, J. C. Lisle, J. N. Mo, Nucl. Phys. A545, 871 (1992).
Nuclear Reactions: 146 Nd( 32 S,4n), E=166 MeV; measured γγ-coin. 174 Os deduced levels, J, π, band structure, configuration.

92Hi10 Prediction of Average β and γ Energies and Probabilities of β-Delayed Neutron Emission in the Region of Fission Products
M. Hirsch, A. Staudt, H. V. Klapdor-Kleingrothaus, At. Data Nucl. Data Tables 51, 243 (1992).
Nuclear Structure: A=62-172; calculated mean Eβ, Eγ, β-delayed neutron probabilities for 1n, 2n. A=62-168; calculated T 1/2 .
Proton-neutron quasiparticle RPA.

92Hi11 Evidence for Strong Nuclear-Breakup Contribution to 6 Li → α + d Breakup by 208 Pb at Forward Angles
Y. Hirabayashi, Y. Sakuragi, Phys. Rev. Lett. 69, 1892 (1992).
Nuclear Reactions: 208 Pb( 6 Li, 6 Li’), E=156 MeV; analyzed σ(θ); deduced strong breakup contribution. Continuum discretized
coupled-channels method.

92Hi12 Preparation of Thin Counting Samples by Volatilization-Condensation
U. Hickmann, N. Greulich, N. Trautmann, G. Herrmann, Nucl. Instrum. Methods Phys. Res. A321, 216 (1992)
Radioactivity: 210 Po(α); measured α-spectra; deduced detector resolution. Thin counting samples preparation.
Nuclear Reactions: 248 Cm( 238 U,F), E not given; analyzed fission product metallic element yields, γ-decay data. Volatilizationcondensation
thin counting samples preparation.

92Hi13 Intermediate Energy pp Phase Shifts to 1000 MeV
Y. Higuchi, N. Hoshizaki, S. Jinushi, H. Masuda, H. Nakao, Prog. Theor. Phys. (Kyoto) 88, 1019 (1992).
Nuclear Reactions: 1 H(p,p), E=0.8-1 GeV; analyzed data; deduced 3 F 3 amplitude features. Phase shift analysis.

92HiZY Continuum-Discretized Coupled-Channels Study of 6 Li → α + d Breakup in Nuclear and Coulomb Fields of Heavy Nucleus: (II)
Coulomb-breakup contribution
Y. Hirabayashi, Y. Sakuragi, Contrib. 13th Int. Conf. on Few-Body Problems in Physics, Adelaide, Australia, January 5-11,
1992, I. R. Afnan, R. T. Cahill, Eds., p. 70 (1992).
Nuclear Reactions: 208 Pb( 6 Li, 6 Li’), E=156 MeV; calculated σ(θ). Continuum-discretized coupled-channels method, cluster model
for 6 Li, Coulomb breakup contribution.

92HiZZ Quasifree Charge-Exchange at Intermediate Energies
K. Hicks, R. Henderson, K. P. Jackson, C. A. Miller, M. C. Vetterli, S. Yen, P. Alford, A. Celler, Bull. Am. Phys. Soc. 37, No.
2, 963, I7 8 (1992)
Nuclear Reactions: 54 Fe, 12 C(polarized p,n), E=290, 420 MeV; measured σ(θ), analyzing power vs θ. Relativistic, nonrelativistic
model comparison.

92Hj01 Folded-Diagram Effective Interactions with the Bonn Meson-Exchange Potential Model
M. Hjorth-Jensen, E. Osnes, H. Muther, Ann. Phys. (New York) 213, 102 (1992).
Nuclear Structure: 18 O, 20 Ne; calculated levels. Bonn meson-exchange potential model, folded-diagram effective interactions,
Brueckner-Hartree-Fock basis.

92Hj02 Effective Interactions for Valence-Hole Nuclei with Modern Meson-Exchange Potential Models
M. Hjorth-Jensen, E. Osnes, T. T. S. Kuo, Nucl. Phys. A540, 145 (1992).
Nuclear Structure: 16 O, 40 Ca; calculated single particle energies. A=14, 38; calculated degenerate, nondegenerate unperturbed
single particle energies. Folded diagram theory, effective interaction.

92Hj03 On the Role of Third- and Higher-Order Contributions to the Effective Interaction for pf Shell Nuclei
M. Hjorth-Jensen, T. Engeland, A. Holt, E. Osnes, Nucl. Phys. A541, 105 (1992).
Nuclear Structure: 44 Ca, 44 Sc, 44 Ti; calculated level relative to 40 Ca. Effective interaction, third-, higher-order contributions in
perturbation theory, Bonn, Paris potentials based meson-exchange interaction.

92Ho01 Electromagnetic Static Moments of Deuteron in the Bethe-Salpeter Formalism
N. Honzawa, S. Ishida, Phys. Rev. C45, 47 (1992).
Nuclear Structure: 2 H; calculated μ, quadrupole moment. Bethe-Salpeter formalism.

92Ho02 High-Spin States in 166 Lu
D. Hojman, A. J. Kreiner, M. Davidson, J. Davidson, M. Debray, E. W. Cybulska, P. Pascholati, W. A. Seale, Phys. Rev. C45,
90 (1992).
Nuclear Reactions: 159 Tb( 12 C,5n), E=75-90 MeV; measured Eγ, Iγ, γγ(t). 166 Lu deduced levels, J, π, γ-multipolarity, B(λ) ratios,
band structure.

92Ho03 Measurement of the 12 C(p,π 0 ) 13 N Reaction by Recoil Detection
J. Homolka, W. Schott, W. Wagner, W. Wilhelm, M. Saber, R. E. Segel, R. D. Bent, M. Fatyga, R. E. Pollock, P. Kienle, K. E.
Rehm, Phys. Rev. C45, 1276 (1992).
Nuclear Reactions: 12 C(p,π 0 ), (p,π + ), E=153.5-204 MeV; measured σ(θ); deduced σ ratio. Phase space, Coulomb barrier penetration
analyses, isospin conservation.

92Ho04 Radiative Proton Capture to Individual States in 12 C
B. Hoistad, E. Nilsson, J. Thun, S. Dahlgren, S. Isaksson, G. S. Adams, C. Landberg, T. B. Bright, S. R. Cotanch, Phys. Lett.
276B, 294 (1992).
Nuclear Reactions: 11 B(p,γ), E=98 MeV; measured σ(θ), radiative capture. Microscopic continuum shell model, realistic finite
range effective interaction, tensor components.

92Ho05 S-Matrix Poles and Phase Shifts for NΔ Scattering
N. Hoshizaki, Phys. Rev. C45, R1424 (1992).
Nuclear Reactions: 1 H(p,pπ + ), E ≤ 0.8 GeV; analyzed NΔ-phase shifts data, S-matrix poles.

92Ho06 Energy Dependence of the Isotopic Effect in the (n, p) Reaction on the Germanium Isotopes
H. M. Hoang, U. Garuska, D. Kielan, A. Marcinkowski, B. Zwieglinski, Z. Phys. A342, 283 (1992).
Nuclear Reactions: 70 , 72 , 73 , 74 Ge(n,p), 70 Ge(n, 2n), 72 , 74 Ge(n,α), E=13-16.6 MeV; measured σ. Activation technique. Preequilibrium,
equilibrium mechanisms included in model analysis.

92Ho07 Strength Distribution of Isoscalar Vibrations Around Thermal Equilibrium
H. Hofmann, S. Yamaji, A. S. Jensen, Phys. Lett. 286B, 1 (1992).
Nuclear Structure: 208 Pb; calculated isoscalar mode strength distribution near thermal equilibrum. Quasi-static picture, temperature
dependent effective coupling constant.

92Ho08 Isospin Character of the Transition to the 0.803-MeV State in 206 Pb from π± Scattering at 180 MeV
D. J. Horen, C. L. Morris, S. J. Seestrom, F. W. Hersman, J. R. Calarco, M. Holtrop, M. Leuschner, M. Rawool-Sullivan, R. W.
Garnett, S. J. Greene, M. A. Plum, J. D. Zumbro, Phys. Rev. C46, 499 (1992).
Nuclear Reactions: 206 Pb(π + ,π + ), (π + , π + ’), (π - ,π - ), (π - , π - ’), E=180 MeV; measured missing mass spectra, σ(θ). 206 Pb deduced
neutron, proton matrix elements ratio for quadrupole, octupole transitions. Deformed optical model, DWIA analyses.

92Ho09 Measurement of the Electron Neutrino Mass from Tritium β-Decay
E. Holzschuh, M. Fritschi, W. Kundig, Phys. Lett. 287B, 381 (1992).
Radioactivity: 3 H(β - ); measured β-spectra; deduced ν-mass upper limit.

92Ho10 Rotational Structures in 174 Ta and ’ Identical Bands ’ in the Normal Deformation Regime
D. Hojman, A. J. Kreiner, M. Davidson, Phys. Rev. C46, 1203 (1992).
Nuclear Reactions: 169 Tm( 9 Be,4n), E=40-65 MeV; measured Eγ, Iγ, γγ(t), γ(θ). 174 Ta deduced levels, J, π, band structure.

92Ho11 Intermediate-Energy Proton Direct Capture Populating Continuum States
Y. -K. Ho, Z. -S. Yuan, Phys. Rev. C46, 1425 (1992).
Nuclear Reactions: 11 B(p,γ), E=10-70 MeV; calculated σ(θ) vs E. Direct capture continuum states population.

92Ho12 Different Effects of Valence Neutrons on the Isospin Character of Transitions to the First 2 + and 3 - States of 90 , 92 , 94 , 96 Zr
D. J. Horen, R. L. Auble, J. Gomez del Campo, R. L. Varner, J. R. Beene, G. R. Satchler, B. Lund, V. R. Brown, P. L. Anthony,
V. A. Madsen, Phys. Lett. 296B, 18 (1992).
Nuclear Reactions: 90 , 92 , 94 , 96 Zr( 6 Li, 6 Li’), E=70 MeV; measured σ(θ). 90 , 92 , 94 , 96 Zr levels deduced neutron, proton matrix element
ratio.

92Ho13 Influence of Core-Polarized States in the Inhibition of Analogue-Antianalogue M1 Transitions in 59 , 61 Cu
M. D. Hossain, Nuovo Cim. 105A, 1141 (1992).
Nuclear Reactions: 58 , 60 Ni(p,γ), E resonance; measured γ-spectra. 59 , 61 Cu deduced M1 transition widths for IAR.

92Ho14 Rotational Spectra of Deformed Nuclei and the Quantum Group SU(q)(2)
M. Honusek, M. Vinduska, V. Wagner, Czech. J. Phys. B42, 1337 (1992).
Nuclear Structure: A=146-248; analyzed levels, B(λ). Comparison between SU(q)(2) and other models.

92Ho15 Nuclear Matter Distributions
P. E. Hodgson, Hyperfine Interactions 74, 75 (1992).
Nuclear Structure: 40 , 48 Ca, 39 K, 90 , 92 , 94 Zr, 206 , 208 Pb, 205 Tl; compiled, reviewed charge density distribution fits. 40 , 48 Ca, 64 Ni,
116 , 124 Sn, 208 Pb; compiled, reviewed neutron density distribution fits. 198 , 200 , 202 , 204 , 206 , 208 , 210 , 212 , 214 Pb; N ≤ 160; compiled,
reviewed rms charge radii fits. A=169-230; compiled, reviewed α-decay Geiger-Nuttall plots.

92Ho16 Studies of Weak Interaction Effects by Laser Spectroscopy of Short-Lived Atoms
C. H. Holbrow, D. Murnick, R. R. Dasari, M. S. Feld, Hyperfine Interactions 74, 119 (1992).
Radioactivity: 85m Rb(IT); measured γ-anisotropy; deduced weak interaction implications. Sub-Doppler resolution, laser-induced
nuclear orientation.

92Ho17 K-Shell Ionization of Intermediate-Z Elements by 30-MeV/ amu H, N, Ne, and Ar Ions
V. Horvat, G. Sampoll, K. Wohrer, M. Chabot, R. L. Watson, Phys. Rev. A46, 2572 (1992).
Nuclear Reactions: 27 Al, Ti, Fe, Cu, Ge, Zr, Mo, Pd, Sn(p,X), (N, X), (Ne,X), (Ar,X), E=30 MeV/nucleon; measured K (X-ray) production
σ, double K-shell ionization I X-ray.
Atomic Physics: +27}Al, Ti, Fe, Cu, Ge, Zr, Mo, Pd, Sn(p,X), (N,X), (Ne,X), (Ar,X), E=30 MeV/nucleon; measured K (X-ray) production
σ, double K-shell ionization I X-ray.

92Ho18 Microscopic Study on Band Structures of 76 , 78 Se and 82 Kr
T. Horibata, J. Phys. Soc. Jpn. 61, 2712 (1992).
Nuclear Structure: 76 , 78 Se, 82 Kr; calculated levels, nucleon pickup spectroscopic factors.

92Ho19 Flavor Singlet Axial Current and Chiral Hyperbag
S. -T. Hong, B. -Y. Park, Int. J. Mod. Phys. E1, 131 (1992).

92HoZS Proton Particle States in 69 , 71 Ga Studied through (d,n) Reactions on 68 , 70 Zn
M. Hosaka, S. Miyamoto, T. Inomata, G. Zhong, K. Ishii, H. Orihara, Cyclotron Rad. Center, Tohoku Univ., Ann. Rept., 1991,
p. 30 (1992).
Nuclear Reactions: 68 , 70 Zn(d,n), E=25 MeV; measured En, σ(θ). 69 , 71 Ga levels deduced spectroscopic factors. Tof. Adiabatic
deuteron breakup approximation.

92HoZT The 16 O( 3 He,n) Reaction at E=45MeV
K. Hosomi, T. Tohei, T. Nakagawa, J. Takamatsu, A. Terakawa, A. Narita, T. Inomata, H. Orihara, K. Ishii, M. Ohura, M.
Hosaka, G. C. Jon, S. Miyamoto, K. Abe, T. Suehiro, K. Miura, H. Ohnuma, Cyclotron Rad. Center, Tohoku Univ., Ann. Rept.,
1991, p. 5 (1992).
Nuclear Reactions: 16 O( 3 He,n), E=45 MeV; measured En, σ(θ). Tof, DWBA.

92HoZU Resolution of Discrepancy Between Backward-Angle Cross-Section Data for n-d Elastic Scattering
C. R. Howell, N. Al-Niemi, R. T. Braun, C. E. Brient, D. E. Gonzalez, S. M. Grimes, G. Mertens, R. S. Pedroni, C. D. Roper, H.
R. Setze, W. Tornow, Contrib. 13th Int. Conf. on Few-Body Problems in Physics, Adelaide, Australia, January 5-11, 1992, I. R.
Afnan, R. T. Cahill, Eds., p. 298 (1992)
Nuclear Reactions: 2 H(n,n), E=8, 14 MeV; measured σ(θ), large angles. Mixed CD 2 -CH 2 foil scatterer.

92HoZV Electromagnetic Static Moments of Deuteron in the Bethe - Salpeter Formalism
N. Honzawa, Contrib. 13th Int. Conf. on Few-Body Problems in Physics, Adelaide, Australia, January 5-11, 1992, I. R. Afnan,
R. T. Cahill, Eds., p. 250 (1992)
Nuclear Structure: 2 H; calculated μ, quadrupole moment. Bethe-Salpeter formalism.

92HoZW Deformation Studies of 79 Rb
J. W. Holcomb, T. D. Johnson, T. Glasmacher, P. C. Womble, M. A. Riley, S. L. Tabor, Bull. Am. Phys. Soc. 37, No. 2, 936,
F10 2 (1992)
Nuclear Reactions: 63 Cu( 19 F,2np), E=65 MeV; measured γγ-coin, DSA. 79 Rb deduced levels, J, π, T 1/2 , transition quadrupole
moments, deformation parameters. Model comparison.

92HoZX Isospin Character of Transitions to Bound States of 206 Pb from π± Scattering at 180 MeV
D. J. Horen, C. L. Morris, S. J. Seestrom-Morris, F. W. Hersman, J. R. Calarco, M. Holtrop, M. Leuschner, M. Rawool, R. Garnett,
S. Greene, M. Plum, J. Zumbro, Bull. Am. Phys. Soc. 37, No. 2, 916, E7 10 (1992)
Nuclear Reactions: 206 Pb(π + ,π + ), (π + , π + ’)E=180 MeV; measured not given. 206 Pb levels deduced neutron, proton matrix element
ratio, isospin character.

92HoZY A(nn) for 500 MeV p(pol) + p(pol) Elastic Scattering
G. Hoffmann, M. Barlett, W. Kielhorn, G. Pauletta, M. Purcell, L. Ray, J. Amann, J. Jarmer, K. Jones, S. Penttila, N. Tanaka,
G. Burleson, J. Faucett, M. Gilaini, G. Kyle, L. Stevens, A. Mack, D. Mihailidis, T. Averett, J. Comfort, J. Gorgen, J. Tinsley,
Bull. Am. Phys. Soc. 37, No. 2, 903, C8 10 (1992)
Nuclear Reactions: 1 H(polarized p,p), E=500 MeV; measured A(nn), θ=23 0 -65 0 . Polarized proton target.

92HoZZ Determination of Asymptotic S-Wave Normalization of the Deuteron by Low-Energy n-d Scattering
C. R. Howell, W. Tornow, H. R. Setze, R. S. Pedroni, S. M. Grimes, C. E. Brient, G. Mertens, H. Witala, Bull. Am. Phys. Soc.
37, No. 2, 887, B8 4 (1992)
Nuclear Reactions: 2 H(n,n), E=8, 10, 14 MeV; measured σ(θ=140 0 -178 0 (cm)). 2 H deduced S-wave asymptotic normalization.
Self-normalizing CD 2 -CH 2 foil, charged particle spectrometer.

92Hs01 Study of Even-Odd N = 90 Isotones in the IBA-Plus-Three-Fermion Model
S. T. Hsieh, H. C. Chiang, M. M. King Yen, J. Phys. (London) G18, 859 (1992).
Nuclear Structure: 157 Ho, 159 Tm, 161 Lu; calculated levels, B(λ), backbending plots. 162 Hf, 160 Yb, 168 Er; calculated backbending
plots. Interacting boson approximation plus three-fermion model.

92Hs02 Structure of Even Ge Isotopes by Means of Interacting Boson Model with a Fermion Pair Model
S. T. Hsieh, H. C. Chiang, D. -S. Chuu, Phys. Rev. C46, 195 (1992).
Nuclear Structure: 64 , 66 , 70 , 72 , 74 , 76 , 78 Ge; calculated levels, B(λ). Interacting boson model.

92Hs03 Spectral Anomalies of Even-Mass Hg Isotopes
S. T. Hsieh, H. C. Chiang, M. M. King Yen, Phys. Rev. C46, 1682 (1992).
Nuclear Structure: 184 , 186 , 188 , 190 , 192 , 194 , 196 , 198 , 200 Hg; calculated levels, B(λ) ratios. Interacting boson approximation plus
fermion pair model.

92Hu01 Search for Low-Lying Magnetic Dipole Strength in the Heavy Odd-Mass Nucleus 165 Ho
N. Huxel, W. Ahner, H. Diesener, P. von Neumann-Cosel, C. Rangacharyulu, A. Richter, C. Spieler, W. Ziegler, C. De Coster,
K. Heyde, Nucl. Phys. A539, 478 (1992).
Nuclear Reactions: 165 Ho(γ,γ’), E=2.8 MeV bremsstrahlung; 165 Ho(e,e’), E=35.1 MeV; measured spectra. 165 Ho levels deduced
M1 transition strengths. Unified rotational model, interacting boson-fermion model calculations comparison.

92Hu02 Spectroscopy of 123 Cs: Configuration dependent crossing frequencies
J. R. Hughes, D. B. Fossan, D. R. LaFosse, Y. Liang, P. Vaska, M. P. Waring, J. -Y. Zhang, Phys. Rev. C45, 2177 (1992).
Nuclear Reactions: 108 Pd( 19 F,4n), E=76 MeV; measured γγ-coin, Eγ, Iγ(θ). 123 Cs deduced levels, band structure, J, π, δ. Potential
energy surface, cranked shell model calculations.

92Hu03 Near-Barrier Fusion of 11 Li with Heavy Spherical and Deformed Targets
M. S. Hussein, M. P. Pato, L. F. Canto, R. Donangelo, Phys. Rev. C46, 377 (1992).
Nuclear Reactions: ICPND 208 Pb( 11 Li,X), E(cm)=10-40 MeV; 238 U( 11 Li,X), E(cm)=10-45 MeV; calculated fusion σ(E); deduced
structure near barrier. Coupled-channels description.

92Hu04 Isomers in Three Doubly Odd Fr-At-Bi α-Decay Chains
M. Huyse, P. Decrock, P. Dendooven, G. Reusen, P. Van Duppen, J. Wauters, Phys. Rev. C46, 1209 (1992).
Radioactivity: 206 , 204 , 202Fr(α), 202 , 200At(α), (β + ); 198At(α); measured Eα, Iα, T , γγ-coin, Eγ, Iγ, electron spectra. 1/2 206 , 204 , 202Fr, 202 200 198 198 196 194 , , At, , , Bi deduced levels, J, π, α-reduced widths, α-branching ratios, Q(α), B(E3), γ-multipolarity, configuration,
isomer transitions.

92Hu05 DWBA Calculation of Neutron Angular Distribution for 7 Li(n,n’) 7 Li (477.6 keV) Reaction
F. Huang, S. Bao, Z. Shi, Chin. J. Nucl. Phys. 14, No 1, 59 (1992).
Nuclear Reactions: 7 Li(n,n), (n,n’), E=8-11 MeV; calculated σ(θ); deduced model parameters. DWBA analysis.

92Hu06 Statistical Fragmentation of Au Projectiles at E/A = 600 MeV
J. Hubele, P. Kreutz, V. Lindenstruth, J. C. Adloff, M. Begemann-Blaich, P. Bouissou, G. Imme, I. Iori, G. J. Kunde, S. Leray,
Z. Liu, U. Lynen, R. J. Meijer, U. Milkau, A. Moroni, W. F. J. Muller, C. Ngo, C. A. Ogilvie, J. Pochodzalla, G. Raciti, G.
Rudolf, H. Sann, A. Schuttauf, W. Seidel, L. Stuttge, W. Trautmann, A. Tucholski, R. Heck, A. R. DeAngelis, D. H. E. Gross,
H. R. Jaqaman, H. W. Barz, H. Schulz, W. A. Friedman, R. J. Charity, Phys. Rev. C46, R1577 (1992).
Nuclear Reactions: C, 27 Al, Cu, Pb( 197 Au,X), E=600 MeV/nucleon; measured intermediate mass fragments mean multiplicity.

92Hu07 Nucler Data Sheets Update for A=56
J. Huo, Nucl. Data Sheets 67, 523 (1992).
Compilation: 56 Ti, 56 V, 56 Cr, 56 Mn, 56 Fe, 56 Co, 56 Ni, 56 Cu, 56 Zn; compiled, evaluated structure data.

92Hu08 Dielectron Yields in p + d and p + p Collisions at 4.9 GeV
H. Z. Huang, S. Bedoe, M. Bougteb, J. Cailiu, J. Carroll, T. Hallman, L. Heilbronn, G. Igo, P. Kirk, G. Krebs, A. Letessier-
Selvon, B. Luttrell, F. Manso, L. Madansky, H. S. Matis, D. Miller, J. Miller, C. Naudet, R. J. Porter, G. Roche, L. S.
Schroeder, P. A. Seidl, Z. F. Wang, R. Welsh, W. K. Wilson, A. Yegneswaran, and the DLS Collaboration, Phys. Lett. 297B,
233 (1992).
Nuclear Reactions: 1 , 2 H(d,X), E=4.9 GeV; measured dielectron yield; deduced dielectron origin features.

92Hu09 Nuclear Magnetic Resonance of Brute Force Oriented 110m Ag(Ag)
W. D. Hutchison, N. Yazidjoglou, D. H. Chaplin, Hyperfine Interactions 73, 247 (1992).
Radioactivity: 110m Ag(β - ); measured NMR, oriented nuclei; deduced μ. Brute force orientation in elemental Ag.

92Hu10 Production of 77 Br for TDPAC Studies
J. L. Hutter, T. J. Ruth, P. W. Martin, Appl. Radiat. Isot. 43, 1393 (1992).
Radioactivity: 77 Br(EC), (β + ) [from 78 Se(p,X), E=29 MeV]; measured Eγ, Iγ, γγ-coin, γγ(t); deduced suitability as probe for γγ(θ,H,t).

92Hu11 Transient NMRON of Brute Force Oriented 110m Ag(Ag)
W. D. Hutchison, N. Yazidjoglou, D. H. Chaplin, Hyperfine Interactions 75, 253 (1992).
Radioactivity: 110m Ag(IT); measured NMR, brute force orientation in Ag; deduced electric field gradient.

92Hu12 NMRON Studies of Ferromagnetic hcp and fcc Co
W. D. Hutchison, A. V. J. Edge, N. Yazidjoglou, D. H. Chaplin, Hyperfine Interactions 75, 291 (1992).
Radioactivity: 60 Co(β - ); measured NMR, oriented nuclei; deduced electric field gradient for 60 Co in Co. Ferromagnetic hcp and
fcc Co.

92Hu13 Status Report of the Leuven Isotope Separator On-Line (LISOL)
M. Huyse, P. Decrock, P. Dendooven, J. Gentens, G. Vancraeynest, P. Vandenberghe, P. Van Duppen, Nucl. Instrum.
Methods Phys. Res. B70, 50 (1992)
Nuclear Reactions: 230 , 232 Th(p,X), E=55 MeV; 233 U(p, X), E=40 MeV; 231 Pa(p,X), E=22 MeV; measured mass separated 227 ,
226 , 225 , 224 Pa, 225 Th yields. Ion guide operation.

92HuZT The Study of GDR in CIAE
Z. Huang, L. Zhu, L. Hou, D. Ding, Beijing National Tandem Accelerator Laboratory, 1990-1991, Ann. Rept., p. 92 (1992).
Nuclear Reactions: 12 C(n,γ), E 6-22 MeV; measured σ(θ) vsE; 2 H(d,γ), E=5.781 MeV; measured σ(θ). 56 Fe(n,γ), E=9 MeV;
measured Eγ, Iγ. 40 Ca(n,γ), E=9.3-14 MeV; measured Eγ, Iγ. 116 Sn( 16 O,γ), E=80 MeV; measured Eγ, Iγ. 132 Ce deduced GDR,
GQR, energy, Γ.

92HuZU Collective Oblate Bands in Pb Nuclei
H. Hubel, G. Baldsiefen, D. Mehta, B. V. Thirumala Rao, U. Birkental, G. Frohlingsdorf, M. Neffgen, N. Nenoff, S. C. Pancholi,
N. Singh, W. Schmitz, K. Theine, P. Willsau, H. Grawe, J. Heese, H. Kluge, K. H. Maier, M. Schramm, R. Schubart, F.
Azaiez, C. Bourgeois, D. Hojman, A. Korichi, N. Perrin, H. Sergolle, H. J. Maier, Proc. Int. Conf. Nuclear Structure at High Angular
Momentum, Ottawa, p. 99 (1992); AECL-10613 (1992)
Nuclear Reactions: 192Os( 12C,5n), E=82 MeV; 193Os( 13C, 6n), E=81 MeV; 186W( 18O,5n), E=94 MeV; 192Os( 13C,5n), E=76 MeV;
192 14 199 200 201 Os( C, 5n), E=70 MeV; measured γγ-coin. , , Pb deduced levels, J, π, band structure, dynamic moment of inertia,
shape features.

92HuZV Radioactive Ion Beams Post-Accelerated to Low and Medium Energies
M. Huyse, P. Van Duppen, Contrib. 6th Intern. Conf. on Nuclei Far from Stability + 9th Intern. Conf. on Atomic Masses and Fundamental
Constants, Bernkastel-Kues, Germany, H1 (1992)
Nuclear Reactions: 1 H( 13 N,γ), E=8.4 MeV; measured reaction σ(E).

92HuZW Hyperfinestructure- Anomaly, Its Determination Solely from A- Factors, and Nuclear Magnetic Moments of Europium Nuclei
H. Huhnermann, W. Moller, G. Alkhazov, V. Panteleev, Contrib. 6th Intern. Conf. on Nuclei Far from Stability + 9th Intern. Conf.
on Atomic Masses and Fundamental Constant, Bernkastel-Kues, Germany, PB5 (1992)
Nuclear Moments: +151}, 153 Eu; measured hfs; deduced μ. Collinear laser ion-beam spectroscopy.
Radioactivity: 145 , 146 , 147 , 152 Eu; measured hfs; deduced μ. Collinear laser ion-beam spectroscopy.

92HuZX Crossed-Second-Order Effects in Isomer Shift and Field and Mass Shift in Eu II
H. Huhnermann, W. Moller, G. Alkhazov, V. Panteleev, Contrib. 6th Intern. Conf. on Nuclei Far from Stability + 9th Intern. Conf.
on Atomic Masses and Fundamental Constant, Bernkastel-Kues, Germany, PB4 (1992)
Radioactivity: 152 Eu(β - ), (β + ), (EC); measured isomer shift relative to 151 Eu; deduced crossed second order effects. Collinear
laser ion beam spectroscopy.
Nuclear Moments: +151}, 152 Eu; measured isomer shift; deduced crossed second order effects. Collinear laser ion beam spectroscopy.

92HuZY Configuration-Dependent Crossing Frequencies in Neutron-Deficient Cs Isotopes
J. R. Hughes, P. Vaska, D. B. Fossan, D. R. LaFosse, Y. Liang, M. P. Waring, J. -Y. Zhang, Contrib. Int. Conf. Nuclear Structure
at High Angular Momentum, Ottawa, p. 108 (1992); AECL-10613 (1992)
Nuclear Reactions: 106 Cd( 16 O,2np), 108 Pd( 19 F, 4n), E not given; measured not given. 119 , 123 Cs deduced levels, J, π, band
structure. Standard γ-spectroscopy. Model comparison.

92HuZZ Collective Oblate Bands in Pb Nuclei
H. Hubel, Contrib. Int. Conf. Nuclear Structure at High Angular Momentum, Ottawa, p. 41 (1992); AECL-10613 (1992)
Nuclear Reactions: 192 Os( 12 C,xn), E=82 MeV; 192 Os( 13 C, xn), E=76 MeV; 192 Os( 14 C,xn), E=70 MeV; 186 W( 18 O,xn), E=94 MeV;
measured γγ-coin. 199 , 200 , 201 Pb deduced levels, J, π, γ-multipolarity, B(λ) ratios, band structure, shape features.

92Hy01 Partial-Wave Analysis of K + -Nucleon Scattering
J. S. Hyslop, R. A. Arndt, L. D. Roper, R. L. Workman, Phys. Rev. D46, 961 (1992).
Nuclear Reactions: 2 H(K + ,X), (K + ,K + ), E < 2.65 GeV; analyzed data; deduced scattering lengths.

92HyZZ Recent Neutrino-Physics Related Mass Measurements at the University of Manitoba
J. G. Hykawy, R. C. Barber, K. S. Sharma, J. N. Nxumalo, P. P. Unger, R. D. Peters, M. H. Sidky, H. E. Duckworth, G. R.
Dyck, C. A. Lander, Contrib. 6th Intern. Conf. on Nuclei Far from Stability + 9th Intern. Conf. on Atomic Masses and Fundamental
Constant, Bernkastel-Kues, Germany, PA5 (1992)
Radioactivity: 82 Se, 82 Kr(2β); measured Q-value; 205 Tl, 205 Pb; measured mass difference; deduced relevance to neutrino physics.
Second-order double focussing spectrometer.