Currently Gutzwiller projection technique and nested Bethe ansatz are two m
ain methods used to handle electronic systems in the U infinity limit. We d
emonstrate that these two approaches describe two distinct physical systems
. In the nested Bethe ansatz solutions, there is a decoupling between the s
pin and charge degrees of freedom. Such a decoupling is absent in the Gutzw
iller projection technique. Whereas in the Gutzwiller approach, the usual a
ntisymmetry of space and spin coordinates is maintained, we show that the B
ethe ansatz wave function is compatible with a form of quantum statistics,
viz., orthofermi statistics. In these statistics, the wave function is anti
symmetric in spatial coordinates alone. This feature ultimately leads to sp
in-charge decoupling.