The problem of the existence of bound states outside the continuum of
the bands due to the presence of a nonlinear impurity is studied withi
n a two-band tight-binding model in one dimension. The nonlinear impur
ity deviates from the ordinary sites by an on-site energy of the form
(chi)(\psi(0)\(2))(beta/2), where \psi(0)\(2) is the probability of fi
nding the particle at the impurity site, chi is referred to as the str
ength and beta is the nonlinearity of the impurity. For beta > 2, ther
e exist threshold values for chi below which there is no bound state.
For 0 < beta less than or equal to 2, there is always one bound state
above the upper band for chi > 0; and two bound states, one with energ
y inside the band gap and another below the lower band, for (chi) < 0.
For beta < 0, there is always a bound state above (below) the upper (
lower) band for chi > 0 (chi < 0). For \beta\ < 2/3 (beta < 0), there
is always a state inside the gap; while for \beta\ > 2/3, there exists
an upper bound for \chi\ above which no bound states are found inside
the gap.