1979
DOI: 10.1088/0034-4885/42/1/001
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The measurement of the lifetimes of excited nuclear states

Abstract: The experimental techniques of measuring the mean lifetimes T of excited nuclear states is reviewed. Emphasis is put on direct measurements of T in the region 10-18-10-6 s, especially on techniques involving the observation of Doppler energy shifts of y-rays. Indirect methods of obtaining T by measuring the widths or partial widths are discussed. Comparisons are made of the applicability, accuracy and reliability of the different experimental techniques.

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Cited by 113 publications
(44 citation statements)
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References 243 publications
(101 reference statements)
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“…The fast timing method is a well-established tool for measuring lifetimes of excited nuclear states [1,2]. Especially since γ-γ fast timing in the sub-nanosecond region has become feasible using LaBr 3 (Ce) scintillators, many studies in different mass regions have employed this method, more and more also in studies of very exotic nuclei using radioactive beams (e.g.…”
Section: Introductionmentioning
confidence: 99%
“…The fast timing method is a well-established tool for measuring lifetimes of excited nuclear states [1,2]. Especially since γ-γ fast timing in the sub-nanosecond region has become feasible using LaBr 3 (Ce) scintillators, many studies in different mass regions have employed this method, more and more also in studies of very exotic nuclei using radioactive beams (e.g.…”
Section: Introductionmentioning
confidence: 99%
“…to extract the Doppler-shift attenuation factor F(τ) [6]. Here, E 0 γ denotes the unshifted γ-ray energy, Θ is the angle between the direction of motion of the reaction product and the direction of γ-ray emission, and v 0 denotes the initial recoil velocity.…”
Section: Introductionmentioning
confidence: 99%
“…It was verified that both 1018-and 1246-keV lines do not show any broadening, i.e., lifetimes longer than 2 ps are expected for the 0 þ 2 and 0 þ 3 states. In contrast, the 1546-keV peak (shown in the inset), is more complex: besides the broadening, which was used to extract a lifetime of 1.4(2) ps for the 3 þ state at 2971.0 keV (with the Doppler shift attenuation method [38]), a weak satellite line is observed on the right-hand side shoulder. We hypothesized that this satellite line, at approximate energy of 1549 keV, may be a transition from the 0 þ 4 state of 66 Ni to the first excited 2 þ state, which would then place this 0 þ excitation at 2974 keV.…”
mentioning
confidence: 99%