T.-F. Wang
Lawrence Livermore National Laboratory
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Physical Review C | 1992
A. Kuhnert; M. A. Stoyer; J. A. Becker; E. A. Henry; M. J. Brinkman; S. W. Yates; T.-F. Wang; J. A. Cizewski; F. S. Stephens; M.-A. Deleplanque; R. M. Diamond; A. O. Macchiavelli; J. E. Draper; F. Azaiez; W. H. Kelly; W. Korten
Evidence for collective behavior in the high-spin region of lead nuclei is provided by the observation of two collective structures in {sup 197}Pb. One of these bands is interpreted as an oblate collective structure built on oblate proton and possibly neutron states. A second more irregular band is suggested to be most likely a triaxial rotational band. Neutron and proton configurations for these bands are suggested from the results of quasiparticle Routhians and total Routhians surface calculations. A partial level scheme up to {ital I}{approx}69/2 and {ital E}{sub {ital x}}{approx}8 MeV is presented.
Physical Review C | 1995
L. A. Bernstein; Ja Cizewski; H.-Q. Jin; W. Younes; R. G. Henry; L. P. Farris; A Charos; M. P. Carpenter; Rvf Janssens; T. L. Khoo; T. Lauritsen; I. G. Bearden; D. Ye; J. A. Becker; Ea Henry; M. J. Brinkman; Hughes; A. Kuhnert; T.-F. Wang; Ma Stoyer; R. M. Diamond; F. S. Stephens; M.-A. Deleplanque; A. O. Macchiavelli; I. Y. Lee; B. Cederwall; J. R. B. Oliveira; J. Burde; P. Fallon; C Duyar
We have studied via in-beam gamma-ray spectroscopy Po-196 and Po-198, which are the first neutron-deficient Po isotopes to exhibit a collective low-lying structure. The ratios of yrast state energi ...
Physical Review Letters | 1993
M. J. Balbes; M. M. Farrell; Richard N. Boyd; X. Gu; M. Hencheck; J. D. Kalen; C. A. Mitchell; J. J. Kolata; K. L. Lamkin; R. Smith; R. Tighe; K. Ashktorab; F. D. Becchetti; J. Brown; D. A. Roberts; T.-F. Wang; D. Humphreys; G. Vourvopoulos; M. S. Islam
Cross sections for the [sup 8]Li([ital d],[ital n])[sup 9]Be (ground state) and [sup 8]Li([ital d],[ital t])[sup 7]Li reactions, both important to primordial nucleosynthesis in the inhomogeneous models, have been measured using a radioactive beam technique. The cross section for the former reaction is found to be small, so it is important only for synthesis of [sup 9]Be. The cross section for the latter reaction, however, is found to be large enough to destroy significant quantities of [sup 8]Li, and thus could affect predictions of primordial nucleosynthesis yields.
Physical Review C | 1994
J. R. B. Oliveira; S. Frauendorf; M.-A. Deleplanque; B. Cederwall; R. M. Diamond; A. O. Macchiavelli; F. S. Stephens; J. Burde; J. E. Draper; C. Duyar; E. Rubel; J. A. Becker; E. A. Henry; M. J. Brinkman; A. Kuhnert; M. A. Stoyer; T.-F. Wang
High-[ital K] bands have been observed in the [sup 166,167,168]Yb isotopes following the [sup 124]Sn([sup 48]Ca,[ital xn][gamma]) reaction. The [nu][ital h][sub 11/2] band in [sup 167]Yb has been extended to higher spins. The high-[ital K] bands in the even-even isotopes were observed for the first time and show very high [ital B]([ital M]1)/[ital B]([ital E]2) ratios. Configuration assignments for the new bands are proposed. The results are interpreted within the Tilted Cranking model.
Nuclear Physics | 1995
M.J. Balbes; M.M. Farrell; Richard N. Boyd; X. Gu; M. Hencheck; J.D. Kalen; C.A. Mitchell; J. J. Kolata; K. Lamkin; R. Smith; R. Tighe; K. Ashktorab; F. D. Becchetti; Jane Brown; D. A. Roberts; T.-F. Wang; D. Humphrey; G. Vourvopoulos; Mohammad S. Islam
Abstract We have measured angular distributions of the 2 H( 8 Li, 7 Li) 3 H and 2 H( 8 Li, 9 Be)n reactions at E c.m. = 1.5 to 2.8 MeV using an 8 Li- radioactive-beam technique. Astrophysical S -factors and reaction rates were calculated form the measured cross sections. Although the 2 H( 8 Li, 9 Be)n cross section is small, it can contribute to 9 Be synthesis. The 2 H( 8 Li, 7 Li) 3 H reaction has a sufficiently large cross section to destroy 8 Li, which may decrease the synthesis of heavier elements. No products from the 2 H( 8 Li, 9 Li)p reaction were detected. We also present the results of calculations using the inhomogeneous model of primordial nucleosynthesis in several regions of parameter space.
Physical Review C | 1994
J. R. B. Oliveira; S. Frauendorf; Deleplanque; B. Cederwall; R. M. Diamond; A. O. Macchiavelli; F. S. Stephens; J. Burde; J. E. Draper; C. Duyar; E. Rubel; J. A. Becker; E. A. Henry; M. J. Brinkman; A. Kuhnert; Stoyer; T.-F. Wang
High-[ital K] bands have been observed in the [sup 166,167,168]Yb isotopes following the [sup 124]Sn([sup 48]Ca,[ital xn][gamma]) reaction. The [nu][ital h][sub 11/2] band in [sup 167]Yb has been extended to higher spins. The high-[ital K] bands in the even-even isotopes were observed for the first time and show very high [ital B]([ital M]1)/[ital B]([ital E]2) ratios. Configuration assignments for the new bands are proposed. The results are interpreted within the Tilted Cranking model.
Progress in Particle and Nuclear Physics | 1992
P. Willsau; H. Hübel; F. Azaiez; M.-A. Deleplanque; R. M. Diamond; W. Korten; A. O. Macchiavelli; F. S. Stephens; H. Kluge; F. Hannachi; J.C. Bacelar; J. A. Becker; M. J. Brinkman; E. A. Henry; A. Kuhnert; T.-F. Wang; J.A. Draper; E. Rubel
Lifetimes of members of the superdeformed band in 194Pb were measured by the Doppler-shift attenuation method. Quadrupole moments around 20 eb that are constant over the whole frequency range were derived. The results rule out large centrifugal stretching effects.
European Physical Journal A | 1992
P. Willsau; H. Hübel; W. Korten; F. Azaiez; M.-A. Deleplanque; R. M. Diamond; A. O. Macchiavelli; F. S. Stephens; H. Kluge; F. Hannachi; J. C. Bacelar; J. A. Becker; M. J. Brinkman; E. A. Henry; A. Kuhnert; T.-F. Wang; J.A. Draper; E. Rubel
Lifetimes of superdeformed states in194Pb were measured by the Doppler-shift attenuation method. Quadrupole moments around 20 eb, that are constant over the observed frequency range, are derived. The results rule out large centrifugal stretching effects.
Physical Review C | 1993
B. Cederwall; M.-A. Deleplanque; F. Azaiez; R. M. Diamond; P. Fallon; W. Korten; I. Y. Lee; A. O. Macchiavelli; J. R. B. Oliveira; F. S. Stephens; W. H. Kelly; Vo Dt; J. A. Becker; M. J. Brinkman; E. A. Henry; J.R. Hughes; A. Kuhnert; Stoyer; T.-F. Wang; J. E. Draper; C. Duyar; E. Rubel; J. DeBoer
High-spin states in the nucleus [sup 196]Hg were populated in the reaction [sup 192]Os([sup 9]Be,5[ital n]) at a beam energy of 65 MeV. A regular rotational-like [Delta][ital I]=1 band has been observed up to an excitation energy of [ital E][sup *][approx]8.7 MeV and spin [ital I][approx]30[h bar]. This is the second observation of a band of this character in a mercury isotope. The experimental results are compared with mean field calculations and semiclassical estimates based on the Doenau-Frauendorf formalism. The mercury bands show significantly lower [ital B]([ital M]1)/[ital B]([ital E]2) branching ratios as compared with similar bands in light lead nuclei. This difference may be more readily explained by a difference in single-particle structure rather than by large differences in deformation between the lead and mercury configurations.
Nuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms | 1993
J. A. Becker; E. A. Henry; A. Kuhnert; M. A. Stoyer; M. J. Brinkman; T.-F. Wang; N. Roy; J. A. Cizewski; F. S. Stephens; M.-A. Deleplanque; R. M. Diamond; J.R.B. Oliveira; J. E. Draper; F. Azaiez; A. O. Macchiavelli; W. Korten; E. Rubel; C. Duyar; W.H. Kelly; Vo Dt
Abstract Reports of recent experiments have included observations of regular and irregular bands in neutron deficient Pb isotopes with A =194, 196–201. The bands are populated strongly in (HI, xn ) reactions. The shared characteristics of the bands include: 1) bandhead energies of a few MeV; 2) high bandhead spin; 3) large alignments; 4) small dynamic moments of inertia, and 5) strong L =1 transitions and weaker L =2 crossover transitions, with B( M 1) B( E 2) ≈ 20 μ 2 e 2 b 2 . Lifetimes of band members in the 198 Pb regular band are B (M1) ≈ 1 W.u. and B (E2) ≈ 12 W.u. (with large errors). These observations are consistent with an interpretation of the regular structures as collective oblate bands with both proton and neutron excitations involved; the closed proton shell at Z =82 is broken, and coupled to v( i 13 2 ) −n excitations. The irregular structures may correspond to triaxial shapes, with similar orbits involved. A similar structure has been also found in 193 Hg.