  Among the light baryons, the $J^\pi = \frac{1}{2}^-$ $\Lambda(1405)$ hyperon
is an important special case as it sits just below the $N\bar{K}$ threshold and
decays almost exclusively to $\Sigma\pi$. Some long-standing hypotheses for
$\Lambda(1405)$ are that it could be a $N\bar{K}$ bound state or a $\Sigma\pi$
continuum resonance. It may also be considered as a simple quark-model
resonance, the $P$-wave companion of the $\Lambda(1520)$. In recent years
chiral unitary models have suggested that there are two isospin zero poles
present in this mass region, and that the "line shape" of the $\Lambda(1405)$
depends to what extent each of the two poles are stimulated in a given
reaction. Below the $N\bar{K}$ threshold, the $\Lambda(1405)$ decays to the
three $\Sigma\pi$ charge combinations. The $\Sigma^{0}\pi^{0}$ mode is purely
$I=0$ and it is uncontaminated by complications arising from $I=1$ scattering
processes contributing to the reaction mechanism in the $\Sigma^{+}\pi^{-}$ and
$\Sigma^{-}\pi^{+}$ decays. It is also not affected from production and decay
of the nearby $\Sigma^{0}(1385)$ hyperon. The GlueX experiment at Jefferson Lab
has been used to study the $\Lambda(1405) \to \Sigma^{0}\pi^{0}$ decay mode. We
focus on the preliminary results of $d\sigma/dM_{\Sigma^{0}\pi^{0}}$ and fits
to the line shape of the $\Lambda(1405)$ region in the $-(t-t_{min})$ range 0 -
1.5 GeV$^2$ from analyzing the reaction $\gamma p \to K^{+}\Lambda^*$ using the
data collected during the first phase of the GlueX program.
