Time dependent anisotropy observed for 181Hf in Wurtzite GaN after implantation and RTA annealing for 120 s at temperatures indicated in the frames. The <0001> axis was aligned with the angle bisector between two detectors under 90°. The solid lines represent least squares fits to the data.
Figure 2
(a) Fraction of 181Hf probes in GaN showing the unique quadrupole interaction of Q1 = 338 MHz (open squares) after various steps of isochronal annealing programmes and the fraction associated with a defect (open triangles). (b) Width of the frequency distribution around Q1 (open squares) and Q2 (open triangles).
Figure 3
Time dependent anisotropy observed for 181Hf in Wurtzite GaN after annealing for different orientations of the <0001> axis. a) aligned with the angle bisector between two detectors under 90°, b) perpendicular to the detector plane, c) aligned with one detector axis. The solid lines represent least squares fits to the data.
Figure 4
Time dependent anisotropy observed for 181Hf in Wurtzite InN (for details see figure 1)
Figure 5
(a) Fraction fD of 181Hf probes in InN showing the unique quadrupole interaction of Q = 666 MHz after various steps of an isochronal annealing programme, (b) Width of the frequency distribution around Q.
Figure 6
Time dependent anisotropy observed for 181Hf in Wurtzite AlN (for details see figure 1)
Figure 7
(a) Fraction fD of 181Hf probes in AlN showing the unique quadrupole interaction of Q = 323 MHz after various steps of an isochronal annealing programme, (b) Width of the frequency distribution around Q.