Figure 1

Spectrum of $\gamma$ rays observed at $+{65}^{°}$ to the beam axis in coincidence with backscattered ${}^{32}\mathrm{S}$ beam ions. This spectrum represents all of the data for the field-up direction in the detector at $+{65}^{°}$, obtained during the precession measurement on the Cd target.Reuse & Permissions

Figure 2

Experimental and calculated angular correlations for even-$A$ Cd isotopes following Coulomb excitation with 95-MeV ${}^{32}\mathrm{S}$ beams. (Data for the different isotopes have been offset for presentation.)Reuse & Permissions

Figure 3

Spectrum of $\gamma$ rays observed at $+{65}^{°}$ to the beam axis in coincidence with backscattered ${}^{32}\mathrm{S}$ beam ions. This spectrum represents the data for the field-up direction in the detector at $+{65}^{°}$, obtained during the precession measurement on the natural Ru target.Reuse & Permissions

Figure 4

Experimental and calculated angular correlations for even-$A$ Ru isotopes following Coulomb excitation with 95-MeV ${}^{32}\mathrm{S}$ beams. Different symbols represent the four $\gamma$-ray detectors.Reuse & Permissions

Figure 5

Examples of $\gamma$-ray spectra observed at $+{65}^{°}$ and $+{115}^{°}$ to the beam axis in coincidence with C ions forward scattered into the outer-particle counters. These spectra represent all of the data for the field-up direction, obtained during the precession measurements on ${}^{102}\mathrm{Ru}$, ${}^{108}\mathrm{Pd}$, and ${}^{108}\mathrm{Cd}$ using Target II.Reuse & Permissions

Figure 6

Measured and calculated angular correlations for ${}^{108}\mathrm{Pd}$ in inverse kinematics. The upper panel is for the center-particle detector (average ${}^{12}\mathrm{C}$ scattering angle 0${}^{°}$); the lower panel is for the top and bottom (outer-) particle detectors (average ${}^{12}\mathrm{C}$ scattering angle 20.7${}^{°}$).Reuse & Permissions

Figure 7

Measured transient-field strength for ${}^{108}\mathrm{Pd}$ ions traversing the gadolinium layer of Target I. Dotted horizontal lines indicate the velocity range over which the transient field is sampled. The average transient-field strength is plotted at the average ion velocity. Open symbols correspond to the detection of ${}^{12}\mathrm{C}$ ions in the central detector, while filled symbols indicate detection in the outer detectors with an average scattering angle of 20.7${}^{°}$. The solid line shows the $v^{0.45}$ velocity dependence of the Rutgers parametrization [19] scaled to best fit these data.Reuse & Permissions

Figure 8

Comparison of transient-field measurements on the Pd isotopes. The present measurements in inverse kinematics are compared with previous measurements in conventional kinematics [31, 32, 33, 34]. The data are shown relative to the present adopted $g(2^{+})$ value in ${}^{106}\mathrm{Pd}$.Reuse & Permissions

Figure 9

Comparison of $g$ factors from the three measurements on the Ru isotopes, calibration values from the literature, and the average values obtained from the global fit. See text.Reuse & Permissions

Figure 10

$g(2^{+})$ calculations compared with experiment. The green line shows $Z/A$.Reuse & Permissions

Figure 11

Comparison between calculated $g$ factors. Black squares show the full calculation as described in the text and shown in Fig. 10. Red dots show the approximation of Eq. (14), which takes into account only the magnetic moments generated by the $g_{9/2}$ protons and the $h_{11/2}$ neutrons.Reuse & Permissions

Figure 12

Composition of the angular momentum of the 2${}^{+}$ states of the Mo and Cd isotopes. The fraction of $J=2$ of each oscillator shell as obtained from the cranking model is shown. The distance between the lower frame and the circles (red curve) is the fraction of the protons in the $N=3$ oscillator shell, the distance between the circles and squares (red and black curves) the $N=4$ proton fraction, the distance between the squares and triangles (black and blue curves) the $N=4$ neutron fraction, and the distance between the triangles (blue curve) and the upper frame the $N=5$ neutron fraction. The contribution of the $N=5$ protons is negligible. The distance between the lower frame and orange curve with no symbols is the proton fraction according to the IBM-II boson counting rule calculated by means of Eq. (16). The neutron fraction is the distance between this curve and the upper frame. The straight green line shows $2Z/A$.Reuse & Permissions

Figure 13

Nilsson diagram of molybdenum neutrons close to the $N=50$ shell; the dashed lines represent negative parity and belong to $h_{11/2}$ levels. The neutron numbers of Mo isotopes are shown at the calculated equilibrium deformation, which illustrates the intrusion of the $h_{11/2}$ shell among the positive-parity orbits for $N<64$, and explains the impact of $h_{11/2}$ orbit on the calculated $g$ factors.Reuse & Permissions