  We have investigated change in the electronic structures of
atomically-controlled La$_{1-x}$Sr$_x$MnO$_3$ (LSMO) thin films as a function
of hole-doping level ($x$) in terms of {\it in situ} photoemission spectroscopy
(PES) and x-ray absorption spectroscopy (XAS) measurements. The {\it in situ}
PES measurements on a well-ordered surface of high-quality epitaxial LSMO thin
films enable us to reveal their intrinsic electronic structures, especially the
structure near the Fermi level ($E_F$). We have found that overall features of
valence band as well as the core levels monotonically shifted toward lower
binding energy as $x$ was increased, indicating the rigid-band like behavior of
underlying electronic structure of LSMO thin films. The peak nearest to $E_F$
due to the $e_g$ orbital is also found to move toward $E_F$ in a rigid-band
manner, while the peak intensity decreases with increasing $x$. The loss of
spectral weight with $x$ in the occupied density of states was compensated by
simultaneous increment of the shoulder structure in O 1$s$ XAS spectra,
suggesting the existence of a pseudogap, that is depression in spectral weight
at $E_F$, for all metallic compositions. These results indicate that the simple
rigid-band model does not describe the electronic structure near $E_F$ of LSMO
and that the spectral weight transfer from below to above $E_F$ across the gap
dominates the spectral changes with $x$ in LSMO thin films.
