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- W3034567533 endingPage "1617" @default.
- W3034567533 startingPage "1612" @default.
- W3034567533 abstract "Quadrupole coupling constants of the $^{43}mathrm{Sc}$(19/${2}^{ensuremath{-}}$) and the $^{43}mathrm{Ti}$(19/${2}^{ensuremath{-}}$) mirror isomers, implanted into hexagonal Ti, have been measured with the time differential perturbed angular distribution method. Values of $frac{{e}^{2}mathrm{qQ}}{h}=8.5(19)$ MHz and 8.0(16) MHz are found at room temperature, corresponding to $eQ=19.9(14)e{mathrm{fm}}^{2} mathrm{and} 30(7)e{mathrm{fm}}^{2}$ for the $^{43}mathrm{Sc}$(19/${2}^{ensuremath{-}}$) and the $^{43}mathrm{Ti}$(19/${2}^{ensuremath{-}}$) states, respectively. The isomeric lifetimes were remeasured as ${T}_{frac{1}{2}}=469(4)$ nsec and 553(21) nsec for the two states. These values, along with transition rates of high spin states in $A=42$ nuclei were analyzed in terms of effective charges, and were found to be consistent with ${e}_{n}=0.56(7)$ and ${e}_{p}=1.26(9)$ for the quadrupole moments, ${e}_{n}=0.65(3)$ and ${e}_{p}=1.35(5)$ for the $B(E2)$ values. The slight increase in the effective charges for the nondiagonal compared to the diagonal $E2$ matrix elements is understood as the effect of an increased core deformation in the lower spin partner of the transition.NUCLEAR REACTIONS $^{27}mathrm{Al}[^{19}mathrm{F},p2n]^{43}mathrm{Sc}({frac{19}{2}}^{ensuremath{-}})$, $E(^{19}mathrm{F})=45.5$ MeV; $^{40}mathrm{Ca}[ensuremath{alpha},p]^{43}mathrm{Sc}({frac{19}{2}}^{ensuremath{-}})$, $^{40}mathrm{Ca}[ensuremath{alpha},n]^{43}mathrm{Ti}({frac{19}{2}}^{ensuremath{-}})$, ${E}_{ensuremath{alpha}}=21$ MeV; pulsed beam, measured ${T}_{frac{1}{2}}$, deduced $B(E2)$, measured $ensuremath{gamma}(ensuremath{theta},t)$ in Ti metal, deduced $Q$." @default.
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- W3034567533 date "1981-04-01" @default.
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- W3034567533 title "E2moments of theSc43(19/2−) and theTi43(19/2−) states and theCa40core deformation" @default.
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- W3034567533 doi "https://doi.org/10.1103/physrevc.23.1612" @default.
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