  We derive a simple system of equations to describe the magnetization
relaxation of a molecular spin in weak interaction with a thermal bath for the
whole temperature domain. Using this for the intermediate temperature domain
where the transition from coherent to incoherent relaxation occurs, we find
that the slowest relaxation mode shows a first-order phase transition.
Associated with this transition, an unusual non-monotonic
temperature-dependence of the relaxation rate of this mode is also
demonstrated. Contrary to the popular belief, this non-monotony gives rise to a
peculiar but observable behavior where increasing temperature will not only
result in a smaller rate of the slowest relaxation mode but also may lead to a
slower decaying of the magnetization after some relaxing time. Additionally, it
is also shown that magnetization relaxation in this intermediate temperature
domain can only be accurately described by a bi- or tri-exponential form. The
physical reason underlying these features can be attributed to the role of the
quantum tunneling effect and different but comparative relaxation modes. A
simple experiment to confirm our findings on the first-order phase transition
and the non-monotony of the relaxation rate is accordingly proposed.
