  Composite Higgs loop effects in the top mode standard model are discussed by
using the Miransky-Tanabashi-Yamawaki (MTY) approach based on the
Schwinger-Dyson equation. The top mass is obtained as 179 GeV for the Planck
scale cutoff (\Lambda \simeq 10^{19} GeV). This result is different from that
of the Bardeen-Hill-Lindner (BHL) approach based on the renormalization group
equation (RGE), with QCD plus Higgs loop effects included (m_t \simeq 205 GeV).
Detailed comparison of the MTY approach with the BHL approach is made. We
derive ``RGE'' from the Pagels-Stokar formula by considering the infrared mass
as the ``renormalization point''. Then, it is found that the MTY approach
including the composite Higgs loop effects is only partially equivalent to the
BHL approach with QCD plus Higgs loop effects. The difference essentially
results from the treatment of the composite Higgs propagator, or more
precisely, of Z_H^{-1}. Our results can be summarized as m_t (Ours) \simeq
1/\sqrt{2} m_t (MTY), in contrast to m_t (BHL) \simeq \sqrt{2/3} m_t (MTY),
where m_t (MTY) \simeq 250 GeV is the original MTY prediction without Higgs
loop effects.
