Abstract
The magnetic moment of the 1142-keV state of was deduced from the known hyperfine splitting of the isomeric state in () and the hyperfine field in this compound. This field kOe was obtained from Mössbauer experiments with the 93.3-keV rays of . The deduced result identifies the state as a virtually pure two-proton configuration.
- Received 11 October 1971
DOI:https://doi.org/10.1103/PhysRevLett.27.1593
©1971 American Physical Society