  Using the renormalization approach proposed by Millis for the itinerant
electron systems we calculated the specific heat coefficient $\gamma(T)$ for
the magnetic fluctuations with susceptibility $\chi^{-1}\sim
|\delta+\omega|^\alpha+f(q)$ near the Lifshitz point. The constant value
obtained for $\alpha=4/5$ and the logarithmic temperature dependence, specific
for the non-Fermi behavior, have been obtained in agreement with the
experimental dat.
