1978
DOI: 10.1016/0375-9474(78)90322-6
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Lifetimes of bound states in 22Na

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Cited by 15 publications
(3 citation statements)
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“…The two experimental observables that went into determining Γ M1 (and therefore b) in the above were the lifetime of the E x = 1952 keV analog state [26] and the 1952 → 0 keV branch, whose value has so far only been published in a laboratory report [23] to be 0.61(24)%. It is thus evident that a remeasurement of this branch is an essential step in examining the origin of the large tensor term reported in Ref.…”
Section: Form Factormentioning
confidence: 99%
“…The two experimental observables that went into determining Γ M1 (and therefore b) in the above were the lifetime of the E x = 1952 keV analog state [26] and the 1952 → 0 keV branch, whose value has so far only been published in a laboratory report [23] to be 0.61(24)%. It is thus evident that a remeasurement of this branch is an essential step in examining the origin of the large tensor term reported in Ref.…”
Section: Form Factormentioning
confidence: 99%
“…where Γ M1 and E γ are the isovector M 1 width and photon energy of the analog γ transition, M is the average of the parent and daughter nuclear masses, κ is a constant [25] and α is the fine-structure constant. The two experimental observables that went into determining Γ M1 (and therefore b) in the above were the lifetime of the E x = 1952 keV analog state [26] and the 1952 → 0 keV branch, whose value has so far only been published in a laboratory report [23] to be 0.61(24)%.…”
Section: Form Factormentioning
confidence: 99%
“…Theoretical F(.r)-curves, based on the LSS theory [29], were calculated using a Monte-Carlo program [30]. The correction factors to the electronic and nuclear stopping functions used in the calculations were adopted to be f, = 1.0 k 0.…”
Section: Lifetimes In "Comentioning
confidence: 99%