1975
DOI: 10.1007/bf01440863
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Determination of spin, magnetic moment and isotopic shift of neutron rich205Hg by optical pumping

Abstract: Abstract. Neutron rich 2~(T1/2 =5.2 min) was produced and on-line mass separated at the ISOLDE facility at CERN. The polarization achieved by optical pumping via the atomic line (6s 2 ~S 0,--,6s 6p 3P t, 2 = 2 537 A) was monitored by the/~ decay asymmetry. Hyperfine structure and isotopic shift of the 2~ absorption line was determined by Zeeman scanning. In addition a magnetic resonance was performed on the polarized

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Cited by 23 publications
(8 citation statements)
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“…1 was constructed from the coincidence relations. From optical pumping experiments the 2~ groundstate-spin is known to be 1/2- [4]. The two excited states at 379 and 467 keV are known from the reactions 2~ and 2~ d) [5-73. We estimated the 2~ grund-state to ground-state /?-decay from the calibrated 31 s-/~--singles component after subtraction of the /%rays to the excited states.…”
Section: Resultsmentioning
confidence: 99%
“…1 was constructed from the coincidence relations. From optical pumping experiments the 2~ groundstate-spin is known to be 1/2- [4]. The two excited states at 379 and 467 keV are known from the reactions 2~ and 2~ d) [5-73. We estimated the 2~ grund-state to ground-state /?-decay from the calibrated 31 s-/~--singles component after subtraction of the /%rays to the excited states.…”
Section: Resultsmentioning
confidence: 99%
“…In the case of fi-RADOP the asymmetry is calculated and corrected for background according to (23). This information serves to trace the resonance position, to determine the necessary statistics, and to obtain a preliminary A factor in order to narrow the region where the NMR resonance is to be found.…”
Section: Remarks On the Course Of The Experimentsmentioning
confidence: 99%
“…The complex 7 spectra, observed farer off stability ask for Ge(Li) detectors and multichannel analysis as described above. Since the two detectors differ in resdlution, spectral response etc., the calculation of signals in analogy to (22), (23) would require a careful peak analysis beforehand. In order to have a quick survey over the results during the experiment, we calculate the signal from the count rates of one detector only according to the following procedure: (i) The integral number of counts taken in both OP modes "a" and "b" is chosen equal.…”
Section: Remarks On the Course Of The Experimentsmentioning
confidence: 99%
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