Nuclear orientation ofAgm106

Nuclei of ${}_{}{}^{106}{}_{}{}^{}\mathrm{Ag}_{}^m{}_{}{}^{}$ embedded in an iron matrix have been oriented at low temperatures. The decay to ${}_{}{}^{106}{}_{}{}^{}\mathrm{Pd}$ allowed determination of the spin values for the levels at 2366 keV ($J=4\mathrm{}$), 2351 keV ($J=4\mathrm{}$), 2283 keV ($J=4\mathrm{}$), 2077 keV ($J=4\mathrm{}$), and 1932 keV ($J=4\mathrm{}$). The $E2\mathrm{}$ fractions $Q=\frac{{\delta }^2}{(1+{\delta }^2})$ could be deduced for 12 mixed $M1-E2\mathrm{}$ transitions (energies in keV): $Q\left(222\right)=0.017\mathrm{}\pm 0.005$, $\delta <0\mathrm{}$; $Q\left(391\right)={0.996}_{-0.006\mathrm{}}^{+0.004\mathrm{}}$, $\delta <0\mathrm{}$; $Q\left(406\right)=0.91\mathrm{}\pm 0.01$, $\delta <0\mathrm{}$; $Q\left(430\right)=0.982\mathrm{}\pm 0.003$, $\delta <0\mathrm{}$; $Q\left(474\right)=0.01\mathrm{}\pm 0.01$ or $Q\left(474\right)=0.94\mathrm{}\pm 0.02$, $\delta <0\mathrm{}$; $Q\left(601\right)=0.03\mathrm{}\pm 0.03$ or $Q\left(601\right)={0.90}_{-0.06\mathrm{}}^{+0.03\mathrm{}}$, $\delta <0\mathrm{}$; $Q\left(616\right)=0.990\mathrm{}\pm 0.005$, $\delta <0\mathrm{}$; $Q\left(703\right)=0.54\mathrm{}\pm 0.14$, $\delta <0\mathrm{}$ or $Q\left(703\right)=1.00-0.04\mathrm{}$, $\delta >0\mathrm{}$ or $\delta <0\mathrm{}$; $Q\left(793\right)=0.00+0.01\mathrm{}$, $\delta >0\mathrm{}$ or $Q\left(793\right)={0.980}_{-0.020\mathrm{}}^{+0.005\mathrm{}}$, $\delta <0\mathrm{}$; $Q\left(825\right)=0.002\mathrm{}\pm 0.002$ or $Q\left(825\right)=0.97\mathrm{}\pm 0.01$, $\delta <0\mathrm{}$; $Q\left(1046\right)=0.005\mathrm{}\pm 0.003$, $\delta <0\mathrm{}$; $Q\left(1528\right)=0.07\mathrm{}\pm 0.01$ or $Q\left(1528\right)=0.84\mathrm{}\pm 0.02$, $\delta <0\mathrm{}$. In addition, the magnetic moment of $6^{+}$ isomeric state of ${}_{}{}^{106}{}_{}{}^{}\mathrm{Ag}$ was determined to be $\left|\mu \right|=(2.8\mathrm{}\pm 0.2){\mu }_N$.