R. Klapisch
CERN
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Featured researches published by R. Klapisch.
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
Physics Letters B | 1982
F. Touchard; P. Guimbal; S. Büttgenbach; R. Klapisch; M. De Saint Simon; J.M. Serre; C. Thibault; H.T. Duong; P. Juncar; S. Liberman; J. Pinard; J.L. Vialle
Abstract Laser optical spectroscopy on a thermal atomic beam has been performed on the 4 2 S sol1 2 −4 2 P 1 2 D 2 line of 38,39,41–47K. Hyperfine structure constants and isotope shifts have been measured. Magnetic moments and changes in the mean square charge radii are deduced.
Nuclear Physics | 1981
M. Langevin; C. Détraz; D. Guillemaud; F. Naulin; M. Epherre; R. Klapisch; S.K.T. Mark; M. de Saint Simon; C. Thibault; F. Touchard
Abstract β-delayed emission of α-particles from 9Li and of both α and 6He particles from 11Li is observed. Singles energy spectra and two-dimensional energy spectra of coincident particles are measured. A time-of-flight versus energy measurement is used to identify the mass of the particle. New β-branches are observed which populate high-energy levels in the daughter nuclei. The branching ratios are measured and the β-delayed neutron emission probabilities P n for 9 Li and P 3n for 11 Li are deduced.
Nuclear Physics | 1980
M. Epherre; G. Audi; C. Thibault; R. Klapisch; G. Huber; F. Touchard; H. Wollnik
Abstract The masses of 204–210, 212 Fr and 224–228 Fr have been determined with direct on-line mass spectrometry. From previously known Q a values, the masses of 28 isotopes of Pa, Ac, At, Bi and Tl are deduced. All these experimental masses are compared with the current mass predictions.
Nuclear Instruments and Methods in Physics Research | 1981
M. de Saint Simon; Roger Fergeau; M. Jacotin; J.F. Kepinski; R. Klapisch; C. Thibault; F. Touchard; M. Langevin; D. Guillemaud
Abstract The experiments performed with the PS on-line mass spectrometer: atomic hyperfine structure determinations and nuclear spectroscopy of Li, Na and K isotopes require high efficiency and as low as possible radioactive background in the area of the detectors. A view of the lay-out will be given concerning in particular the very thick iron and concrete shielding and the mass separated ion beam line going through the shielding from the mass spectrometer to the detector room. This device is an L-shaped pipe with electrostatic focusing elements. The background correlated with the proton beam pulse is lower than the sensitivity of the γ detector and the neutron flux is less than 1 n/cm2s. Slow rate events, corresponding to nuclei far from the stability, such as 34Na, are recorded with a good signal-to-noise ratio.
Nuclear Instruments and Methods in Physics Research | 1981
C. Thibault; P. Guimbal; R. Klapisch; M. de Saint Simon; J.M. Serre; F. Touchard; S. Büttgenbach; H.T. Duong; P. Jacquinot; P. Juncar; S. Liberman; P. Pillet; J. Pinard; J.L. Vialle; G. Huber; A. Pesnelle
Abstract On-line high resolution laser spectroscopy experiments have been performed in which the light from a cw tunable dye laser interacts at right angles with a thermal atomic beam. 76–98Rb, 118–145Cs and 208–213Fr have been studied using the ionic beam delivered by the ISOLDE on-line mass separator at CERN while 20–31Na and 38–47K have been studied by setting the apparatus directly on-line with the PS 20 GeV proton beam. The principle of the method is briefly explained and some results concerning nuclear structure are given.
Nuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms | 1992
M. de Saint Simon; A. Coc; M. Jacotin; J.-F. Képinski; R. Le Gac; G. Le Scornet; C. Thibault; F. Touchard; H. Haebel; H. Herr; R. Klapisch; G. Lebée; G. Petrucci; G. Stefanini; H. Deitinghoff; A. Schempp; F. Botlo-Pilat
Abstract The experiment aims at the reduction of the upper limit on a hypothetical CPT violation in the antiproton-proton system. A radio-frequency mass spectrometer (RFMS) has been designed and built to make the comparison of the charge to mass ratios of p and p by measuring the ratios of the cyclotron frequencies of p and H− ions. At present, the RFMS is installed on-line to the LEAR facility at CERN. The resolving power has been found to be close to 3 × 105 and it still could be improved. A decelerating system (RFQ) has been installed in order to decelerate antiprotons from 2 MeV to 200 keV and to match as well as possible the acceptance of the spectrometer. It is presently under test and data taking should take place in 1992.
European Symposium on Antiproton-Proton Interactions and Fundamental Symmetries 9 | 1989
C. Thibault; A. Coc; Roger Fergeau; Renaud Le Gac; Michel de Saint Simon; F. Touchard; Ernst Haebel; H. Herr; R. Klapisch; G. Lebée; G. Petrucci; Giorgio Stefanini
The radiofrequency mass spectrometer has been prepared in Orsay, and moved to CERN to be installed on-line with LEAR (PS189). The present and finally expected performances are given.
Nuclear Physics | 1993
C. Thibault; A. Coc; H. Deitinghof; Ernst Haebel; H. Herr; R. Klapisch; G. Lebée; R. Le Gac; G. Petrucci; M. de Saint Simon; A. Schempp; G. Stefanini; F. Touchard
Abstract In order to test CPT invariance theorem, PS189 aims at checking the equality of proton and antiproton masses via the measurement of the ratio of H − and p masses using a radio-frequency mass spectrometer. Recent progress, including a resolving power of 6 × 10 5 , is presented.
Archive | 1987
A. Coc; Roger Fergeau; Ernst Haebel; H. Herr; R. Klapisch; G. Lebée; Renaud Le Gac; G. Petrucci; Michel de Saint Simon; Giorgio Stefanini; C. Thibault; F. Touchard
The principle and the main parameters of the radiofrequency mass spectrometer for the experiment PS 189 (Fig. 1) have already been discussed and described in detail1,2,3. We shall here only recall them very briefly and give the present status of the preparation of the experiment.