Measurements of the magnetization as a function of temperature T, magn
etic field H, and time are performed in Nb-O solid solution having T-c
= 6.8 K. Two ''irreversibility lines'' are found in the H-T phase dia
gram: one of those lies well below the H-c2(T) boundary, while the oth
er is situated very close to H-c2(T). In both pinned vortex state regi
ons Kohlrausch magnetic relaxation is observed, implying the occurrenc
e of a strongly disordered vortex matter. The reentrant irreversible b
ehavior of the magnetization close to H-c2(T) could be understood in t
erms of a ''peak effect''. Similarity between vortex behavior in Nb-O
and heavy-fermion systems is pointed out.