Abstract
The perturbed angular correlation (PAC) technique was used to study the hyperfine interactions in the antiferromagnetic and paramagnetic regions of the distorted perovskites ${\mathrm{LaCrO}}_{3}$ and ${\mathrm{LaFeO}}_{3}.$ The dilute ${}^{111}{\stackrel{\ensuremath{\rightarrow}}{\mathrm{In}}}^{111}\mathrm{Cd}$ nuclear probes were introduced into the samples through a chemical process. The present measurements cover the temperature ranges from 15 to 848 K for ${\mathrm{LaCrO}}_{3}$ and 77 to 1324 K for ${\mathrm{LaFeO}}_{3}.$ Two distinct electric-quadrupole interactions were observed in each compound. The lower quadrupole frequency was assigned to the transition-metal atom site while the higher frequency was attributed to the lanthanum site in both cases. Temperature dependence of the electric-quadrupole interaction parameters indicated structural phase transitions at around 512 and 1223 K, respectively, in ${\mathrm{LaCrO}}_{3}$ and ${\mathrm{LaFeO}}_{3}.$ The phase transitions were associated with the change from an orthorhombic to rhombohedral structure and characterized by a sudden increase in the electric field gradient ${V}_{\mathrm{zz}}$ and a decrease in the asymmetry parameter $\ensuremath{\eta}$ for both sites. PAC spectra measured below the N\'eel temperature revealed that at 0 K the supertransferred magnetic hyperfine field on ${}^{111}\mathrm{Cd}$ at the Cr site in ${\mathrm{LaCrO}}_{3}$ (2.4 T) is much smaller than at the Fe site in ${\mathrm{LaFeO}}_{3}$ (19.4 T). The magnetic field on ${}^{111}\mathrm{Cd}$ at La sites in both compounds is of the order of 0.3 T. Additional measurements were made to determine the magnetic hyperfine field using the probe nucleus ${}^{140}{\stackrel{\ensuremath{\rightarrow}}{\mathrm{La}}}^{140}\mathrm{Ce}.$ The result reconfirmed that a relatively weak hyperfine field is supertransferred to the probe atoms at La sites.
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