The following g-factors have been derived from time integral measurements of 7-7 angular correlations in the static magnetic hyperfine field of magnetized gadolinium metal probes:= +0.310(19) g(6 +) = + 0.25(21) 4 + g~ 3,1511 keV)= +0.809(27) 158Gd: g(4 +) = +0.409(15).The 5.35 d 156Tb sources were produced by the reaction t 56Gd(d ' 2 n) 156Tb in our cyclotron. A carrier-free 150 y 15STb source was obtained from ISOLDE/CERN. In comparison with the precisely known g-factors of the 2+ states, g(2+, 156Gd)= +0.386(4) and g(21 +, 158Gd)=0.381(4), we observe a large reduction for the 156Gd 4~-state whereas g increases slightly for 15SGd. The half-life of the 4+ state of t58Gd was remeasured as 158Gd: T1/2(4+)= 148(2)ps. A measurement of the rotation in the 4~ state of lS6Gd in external magnetic fields of various strengths up to B~xt=9.5 T did not confirm the anomalous dependence of the magnetic hyperfine field in gadolinium metal on the external field, which has been reported by Persson et al. [29].

The nuclear Larmor precession has been observed for the 2 +, 4 + and 6 + rotational states of ls4W in the hyperfine field of WFge by application of the TDPAC and the IPAC techniques. A carrier free radioactive source of lS4mRe alloyed with high purity iron was used for all three measurements. (5) with the sign convention of Krane and Steffen.

The static hyperfine field of B472K(ErHo)=739 (18) The results are discussed and compared with theoretical predictions.

The IPAC-method has been used with the external magnetic field of 9.0T of a split coil superconducting magnet and with the internal field of PdF__~e for a measurement of The half-life of the 645 keV state has been redetermined by use of cooled thallium free NaI detectors as T1/2 (645 keY)= 126(2) ps. >7 directional correlations were measured with a system of three large Ge planar diodes for the cascades 443-645 keV, 332-319keV, 393-280keV, and 64-280keV and analyzed in terms of dipole quadrupole mixing ratios of the ?,-lines involved. The spin of the 673 keV state was derived as 1/2 +.

The ~-factor of the 589 keV state of l~TIn has been determined by a measurement of the rotation of the 1,303-273 keV 7-7 directional correlation in an external magnetic field of 9.55(1)T. The result, g3/2(589 keV)= +0.068 (39), contradicts the usual interpretation of the state as the 2p3/2 single proton hole configuration for which the Schmidt value is ga/2-(Schmidt)= +2.53. It favours the interpretation as the first rotational state built up on the single proton [301] 1/2-Nilsson orbit in a strongly deformed core of prolate shape.