In0.1Cu0.45Fe0.45Cr2S4 has been studied by Mossbauer spectroscopy, X-ray di
ffraction, and magnetic-susceptibility measurements. The crystal is found t
o have a cubic spinel structure with the lattice constant a(0) = 9.931 +/-
0.005 Angstrom. The iron ions are in ferric states. The temperature depende
nce of the magnetic hyperfine field is analyzed by the Neel theory of ferri
magnetism. The intersublattice superexchange interaction is antiferromagnet
ic with a strength of J(AB) = -4.90 k(B) while the intrasublattice superexc
hange interactions are ferromagnetic with strengths of J(AA) = 7.90 k(B) an
d J(BB) = 10.30 k(B). The ferrimagnetic-to-paramagnetic transition takes pl
ace at 231 K. There is a second transition from the ferrimagnetic state to
a spin-glass-like state below 78 K. A ten percent (10 %) replacement of the
Cu-Fe ion-pairs by In ions decreases the Neel temperature by 34 % and the
magnetic hyperfine field at liquid-helium temperature by 12 %.