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- W2055148908 abstract "The electric monopole ($E0$) transitions from the first and second excited ${0}^{+}$ states at 1130.3 and 1740.7 keV, respectively, in $^{100}mathrm{Ru}$ have been observed from the internal-conversion-electron studies of the decay of $^{100}mathrm{Rh}$. The monopole strength for the first excited ${0}^{+}$ state $ensuremath{rho}(E0;{0}_{1}^{+}ensuremath{-}{0}_{g}^{+})<0.11$ is deduced as an upper limit. The dimensionless ratios of the reduced $E0$- to $E2$-transition probabilities $X$ are deduced: $Xleft(frac{E0;{0}_{1}^{+}ensuremath{-}{0}_{g}^{+}}{E2;{0}_{1}^{+}ensuremath{-}{2}_{1}^{+}}right)=0.011ifmmodepmelsetextpmfi{}0.001,$ $Xleft(frac{E0;{0}_{2}^{+}ensuremath{-}{0}_{g}^{+}}{E2;{0}_{2}^{+}ensuremath{-}{2}_{1}^{+}}right)=0.6ifmmodepmelsetextpmfi{}0.3$. The observed branching ratio of the monopole strength for the second excited ${0}^{+}$ state is $frac{ensuremath{rho}({0}_{2}^{+}ensuremath{-}{0}_{g}^{+})}{ensuremath{rho}({0}_{2}^{+}ensuremath{-}{0}_{1}^{+})}=0.73ifmmodepmelsetextpmfi{}0.07$. The experimental results are compared with the theory on the basis of the collective vibrations of an axially and nonaxially deformed nucleus.RADIOACTIVITY $^{100}mathrm{Pd}$ [from $^{103}mathrm{Rh}(p,4n)$]; measured ${E}_{mathrm{ce}}$, ${I}_{mathrm{ce}}$, ${E}_{ensuremath{gamma}}$, ${I}_{ensuremath{gamma}}$, $ensuremath{gamma}ensuremath{-}ensuremath{gamma}$ coin $^{100}mathrm{Ru}$ deduced ICC, $B(E0)$, branching ratio $frac{B(E0)}{B(E2)}$." @default.
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- W2055148908 title "Electric monopole transitions between<mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML display=inline><mml:mrow><mml:msup><mml:mrow><mml:mn>0</mml:mn></mml:mrow><mml:mrow><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math>states in<mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML display=inline><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant=normal>Ru</mml:mi></mml:mrow><mml:mprescripts /><mml:mrow /><mml:mrow><mml:mn>100</mml:mn></mml:mrow><mml:mrow…" @default.
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