  Using an interaction extracted from the local hidden gauge Lagrangians, which
brings together vector and pseudoscalar mesons, and the coupled channels $\rho
N$ (s-wave), $\pi N$ (d-wave), $\pi \Delta$ (s-wave) and $\pi \Delta$ (d-wave),
we look in the region of $\sqrt s =1400-1850$ MeV and we find two resonances
dynamically generated by the interaction of these channels, which are naturally
associated to the $N^*(1520) (3/2^-)$ and $N^*(1700) (3/2^-)$. The $N^*(1700)
(3/2^-)$ appears neatly as a pole in the complex plane. The free parameters of
the theory are chosen to fit the $\pi N$ (d-wave) data. Both the real and
imaginary parts of the $\pi N$ amplitude vanish in our approach in the vicinity
of this resonance, similarly to what happens in experimental determinations,
what makes this signal very weak in this channel. This feature could explain
why this resonance does not show up in some experimental analyses, but the
situation is analogous to that of the $f_0(980)$ resonance, the second scalar
meson after the $\sigma (f_0(500))$ in the $\pi \pi$(d-wave) amplitude. The
unitary coupled channel approach followed here, in connection with the
experimental data, leads automatically to a pole in the 1700 MeV region and
makes this second $3/2^-$ resonance unavoidable.
