H.T. Duong
Centre national de la recherche scientifique
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Featured researches published by H.T. Duong.
Nuclear Physics | 1981
C. Thibault; F. Touchard; S. Büttgenbach; R. Klapisch; M. de Saint Simon; H.T. Duong; P. Jacquinot; P. Juncar; S. Liberman; P. Pillet; J. Pinard; J.L. Vialle; A. Pesnelle; G. Huber
Abstract High-resolution laser spectroscopy has been performed on 118–145 Cs and 119m, 121m, 122m, 130m, 134m, 135m, 136m, 138m, Cs.The Cs nuclei have been produced either by spallation of La or by fission of U by the 600 MeV proton beam, from the SC at CERN. The hyperfine structures, spins, and isotope shifts have been measured. The charge radii changes deduced from the isotope shifts exhibit shell effects at N = 82, isomeric staggering for N = 64,66,67 and a strong odd-even staggering for all isotopes with N
Hyperfine Interactions | 1988
B. Roussière; E. Le Blanc; G. Savard; H.T. Duong; J. Pinard; S. Liberman; J.K.P. Lee; J. E. Crawford; G. Thekkadath; P. Kilcher; J. Obert; J. Oms; J. C. Putaux; J. Sauvage
Isotope shift (IS) and hyperfine structure (HFS) measurements have been performed for185, 187, 189, 191, 195Pt using the PILIS (Post ISOCELE Laser Isobar Separator) apparatus installed at the ISOCELE facility. Magnetic and quadrupole moments have been deduced from the HFS results. The charge radius changes determined for these odd nuclei from the IS results, added to the σ values of the even-A nuclei are compared to the results of lattice Hartree-Fock+BCS calculations for asymmetric solutions:185Pt is confirmed to be prolate shaped whereas187, 189, 191Pt are likely triaxial in their ground states.
Hyperfine Interactions | 1992
S. Matsuki; K. Shimomura; I. Ogawa; Keiichiro Suzuki; S. Hamada; Takashi Nakamura; H. Okuno; M. Koizumi; N. Inabe; Y. Fukashiro; H. Sunaoshi; M. Wada; Toshiyuki Murayama; Masao Kitano; Toshiyuki Kubo; T. Shinozuka; K. Asahi; Y. Kido; T.T. Inamura; T. Nomura; M. Ishihara; M. Fujioka; H.T. Duong; H. Haas
Radiation-detected optical pumping in solids has been developed to investigate the structure of unstable nuclei. Appreciable nuclear polarization of implanted or doped unstable-nuclei in a host crystal is achieved with the optical pumping in solids. The nuclear polarization achieved is enhanced/reduced by applying a radio-frequency magnetic field together with the optical pumping, radiation-detected magnetic resonance being thus observed to get information on electromagnetic properties of unstable nuclei. Two schemes have been successfully developed for the optical pumping of unstable nuclei in solids. One is to directly pump the atoms by the excitation from the ground state to a broad absorption band in visible and UV regions which shows a large magnetic circular dichroism. This scheme is applicable to many rare-earth atoms in alkaline-earth fluoride host. The other scheme is to pump the electrons in the conduction band of direct-type semiconductor and thus indirectly polarize the nuclei in the host material via a hyperfine interaction between the nuclei and the polarized conduction electrons. This scheme can be especially applied to the III to VI families of atoms in direct-type semiconductors. Principle of the methods, on-line experimental system, and a few examples of the results obtained so far are presented and discussed.
Hyperfine Interactions | 1992
H.T. Duong; J. Pinard; C Ekstrom; M. Gustafsson; Ingvar Lindgren; T. Nilsson; J Persson; T.T. Inamura; P. Juncar; S. Matsuki; Toshiyuki Murayama; R. Neugart; J. L. Vilalle; M. Pellarin; S Penselin; I. Ragnarsson; O. Redi; H.H. Stroke
The hyperfine anomaly gives an insight into the coupling of spin and orbital magnetic moments in the nucleus. More precisely, the nuclear magnetization is expressible through the nuclear wave functions with which is tested not only the magnetic moment operator, but also the tensor product [s×C2]1. The experiment can then be expected to be of value in testing the nuclear structure theory. The greatest value of these measurements is gained when these are made systematically over a large number of isotopes. We propose to initiate a program at ISOLDE to measure the hyperfine anomaly systematically in the heavy alkali elements. The experimental setup to achieve, in particular, a precise measurement of the nuclearg-factor is presented and the results on atomic beams of39K are discussed.
Physical Review C | 1981
C. Thibault; F. Touchard; S. Buettgenbach; R. Klapisch; M. de Saint Simon; H.T. Duong; P. Jacquinot; P. Juncar; S. Liberman; P. Pillet; J. Pinard; J.L. Vialle; A. Pesnelle; G. Huber
Journal De Physique | 1982
H.T. Duong; P. Juncar; S. Liberman; J. Pinard; J.L. Vialle; S. Büttgenbach; P. Guimbal; M. de Saint Simon; J.M. Serre; C. Thibault; F. Touchard; R. Klapisch
Hyperfine Interactions | 1981
C. Thibault; S. Büttgenbach; H.T. Duong; P. Guimbal; G. Huber; P. Jacquinot; P. Juncar; R. Klapisch; S. Liberman; A. Pesnelle; P. Pillet; J. Pinard; J.M. Serre; M. de Saint Simon; F. Touchard; J.L. Vialle
Nuclear Physics | 2005
J. Pinard; H.T. Duong; D. Marescaux; H.H. Stroke; O. Redi; M. Gustafsson; T. Nilsson; S. Matsuki; Y. Kishimoto; K. Kominato; I. Ogawa; Masaru Shibata; M. Tada; J.R. Persson; Y. Nojiri; S. Momota; T.T. Inamura; M. Wakasugi; P. Juncar; Toshiyuki Murayama; T. Nomura; M. Koizumi
Nuclear Physics | 2005
J. Pinard; H.T. Duong; D. Marescaux; H.H. Stroke; O. Redi; M. Gustafsson; T. Nilsson; S. Matsuki; Y. Kishimoto; K. Kominato; I. Ogawa; Masaru Shibata; M. Tada; J.R. Persson; Y. Nojiri; S. Momota; T.T. Inamura; M. Wakasugi; P. Juncar; Toshiyuki Murayama; T. Nomura; M. Koizumi
Nuclear Physics | 2005
J. Pinard; H.T. Duong; D. Marescaux; H.H. Stroke; O. Redi; M. Gustafsson; T. Nilsson; S. Matsuki; Y. Kishimoto; K. Kominato; I. Ogawa; Masaru Shibata; M. Tada; J.R. Persson; Y. Nojiri; S. Momota; T.T. Inamura; M. Wakasugi; P. Juncar; Toshiyuki Murayama; T. Nomura; M. Koizumi