At. Motta et al., Defects and magnetic hyperfine fields in ZrFe2 investigated using perturbed-angular-correlation spectroscopy, PHYS REV B, 60(2), 1999, pp. 1188-1196
We have measured the temperature dependence of the electric and magnetic hy
perfine interactions at Ta-181 nuclei substituted into the Zr site in the L
aves-phase compound ZrFe2, using tie perturbed angular correlation of gamma
rays emitted after the beta(-) decays of Hf-181 probe nuclei. Although the
overall crystal structure is cubic, a weak strongly damped electric-quadru
pole interaction is observed, which shows no significant temperature depend
ence over the investigated temperature range from 290-1300 K. Thus below th
e magnetic ordering temperature Te of 631(2) K we observe combined magnetic
-dipole and electric-quadrupole hyperfine interactions. Two separate magnet
ic components characterize the magnetic-dipole interactions. For the intera
ction at the primary site, which is occupied by 70-80% of the probes, the L
armor frequency measured at temperature has a value of omega(L) = 407(1) Mr
ad sec(-1). The secondary site is populated by the remaining 20-30% of the
probes, for which the corresponding Larmor-frequency has a room temperature
value of omega(t) = 579(3) Mrad sec(-1). We attribute the primary interact
ion to the "perfect-crystal" probe environment at the Zr site, whereas we a
scribe the secondary interaction to the enhancement of the transferred hype
rfine field by the presence of Fe antisite defects near the Zr site. At tem
peratures below but very close to T-C, those frequencies cannot be determin
ed for either interaction, because the magnetic-hyperfine and the electric-
quadrupole frequencies converge to comparable values.