ThMnAl and ThMnIn have the C-15, cubic Laves phase crystal structure. prono
unced thermomagnetic irreversibility is seen in the magnetisation of both c
ompounds. A cusp in the AC susceptibility of ThMnAl near 43 K which shows f
requency dependence establishes the spin glass freezing of the Mn moments i
n this compound. This is further corroborated by the heat capacity data whi
ch do not exhibit any anomaly near the cusp temperature. On the other hand,
the zero-field-cooled magnetisation of ThMnIn shows a sharp ferromagnetic-
like increase around 270 K, a broad peak around 180 K and then decreases mo
notonically with temperature. Various scenarios based on the sign change of
Mn-Mn exchange interaction between ThMnAl and ThMnIn due to the increased
Mn-Mn bond length in the latter are discussed. Electrical resistivity is la
rge in both compounds and shows a negative temperature coefficient indicati
ng the disordered nature of both alloys. (C) 2000 Elsevier Science B.V. All
rights reserved.