The
intrinsic behavior of photogenerated charges and reactions
with chemicals are key for a photocatalytic process. To observe these
basic steps is of great importance. Here we present a reliable and
robust system to monitor these basic steps in powder photocatalysts,
and more importantly to elucidate the key issue in photocatalytic
methane conversion over the benchmark catalyst TiO
2
. Under
constant excitation, the absorption signal across the NIR region was
demonstrated to be dominated by photoexcited electrons, the absorption
of photoexcited holes increases toward shorter wavelengths in the
visible region, and the overall shapes of the photoinduced absorption
spectra obtained using the system demonstrated in the present work
are consistent with widely accepted transient absorption results.
Next,
in situ
measurements provide direct experimental
evidence that the initial step of methane activation over TiO
2
involves oxidation by photoexcited holes. It is calculated
that 90 ± 6% of photoexcited electrons are scavenged by O
2
(in dry air), 61 ± 9% of photoexcited holes are scavenged
by methane (10% in argon), and a similar amount of photoexcited electrons
can be scavenged by O
2
even when the O
2
concentration
is reduced by a factor of 10. The present results suggest that O
2
is much more easily activated in comparison to methane over
anatase TiO
2
, which rationalizes the much higher methane/O
2
ratio frequently used in practice in comparison to that required
stoichiometrically for photocatalytic production of value-added chemicals
via methane oxidation with oxygen. In addition, methanol (a preferable
product of methane oxidation) is much more readily oxidized than methane
over anatase TiO
2
.