Electric monopole transitions between <span class="aps-inline-formula"><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mrow><msup><mrow><mi mathvariant="normal">O</mi></mrow><mrow><mo>+</mo></mrow></msup></mrow></math></span> states in <span class="aps-inline-formula"><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mrow><mmultiscripts><mrow><mi mathvariant="normal">Ru</mi></mrow><mprescripts></mprescripts><mrow></mrow><mrow><mn>102</mn></mrow><mrow></mrow><mrow></mrow></mmultiscripts></mrow></math></span>

M. Koike; K. Komura; H. Kawakami; M. Kanbe; H. Yamada; G. Madiueme; S. Shibata; T. Fujisawa; T. Wada

doi:10.1103/PhysRevC.24.1611

Electric monopole transitions between $O^{+}$ states in ${}^{102}{Ru}$

M. Koike, K. Komura, H. Kawakami, M. Kanbe, H. Yamada, G. Madiueme, S. Shibata, T. Fujisawa, and T. Wada

Phys. Rev. C 24, 1611 – Published 1 October 1981

Abstract

The electric monople ( $E 0$ ) transition from the first excited $0^{+}$ state at 943.67 keV in ${}^{102}{Ru}$ is observed from the internal conversion electron studies. The dimensionless ratio of the $E 0$ to $E 2$ transition probabilities, $X (\frac{E 0}{E 2})$ , is deduced to be 0.013±0.002. The monopole moment $ρ (E 0)$ is estimated as 0.092.

RADIOACTIVITY ${}^{102}{Rh}$ [from ${}^{102}{Ru}$ ( $p$ , $n$ )]; measured $E_{ce}$ , $I_{ce}$ , $E_{γ}$ , $I_{γ}$ . ${}^{102}{Rh}$ deduced branching ratio $\frac{B (E 0)}{B (E 2)}$ , monopole moment $ρ (E 0)$ .

Received 6 May 1981

DOI:https://doi.org/10.1103/PhysRevC.24.1611

Authors & Affiliations

M. Koike, K. Komura^*, H. Kawakami, M. Kanbe^†, H. Yamada^‡, G. Madiueme^§, and S. Shibata^∥

Institute for Nuclear Study, University of Tokyo, Tanashi, Tokyo 188, Japan

T. Fujisawa and T. Wada

Institute of Physical and Chemical Research, Wako-shi, Saitama-ken 351, Japan

^*Permanent address: Low Level Radioactivity Laboratory Faculty of Science, Kanazawa University, Tatsunokuchi, Ishikawaken 923-12, Japan.
^†Present address: Department of Applied Physics, Tokyo Institute of Technology, Ohokayama, Meguro-ku, Tokyo 152, Japan.
^‡Present address: Oak Ridge National Laboratory, Oak Ridge Tennessee 37830.
^§Permanent address: Department of Physics, University of Ife, Ile-Ife, Nigeria.
^∥Present address: Department of Chemistry, Carnegie-Mellon University, Pittsburgh, Pennsylvania 15213.

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Vol. 24, Iss. 4 — October 1981

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Physical Review C

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