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achieve the saturated adsorption of CO (m/z = 28) and H2
(m/z = 2) more quickly than Pt–Fe/M. After reaching the sat-
urated adsorption, O2 (m/z = 32) pulses are injected in the He
carrier stream. Neither CO2 (m/z = 44) nor H2O (m/z = 18)
is formed with no consumption of injected O2 at Pt/M; how-
ever, CO2 is immediately formed at Pt–Fe/M by the oxidation
of adsorbed CO with pulse-injected O2. Nevertheless no H2O
is detected. The results of CO/H2-TPD in Fig. 5 show the pres-
ence of two kinds of H2. The weakly adsorbed H2, desorbed
completely up to 150 ◦C, may react with O2 and formed H2O.
The H2O is presumably trapped in the mordenite cages and can-
not be detected in the present experiment shown in Fig. 7b. We
may consider that using strongly adsorbed H2, starting the des-
orption at >200 ◦C, or continuing the desorption at even 400 ◦C
has probably less reactivity to adsorbed O2 than that of CO,
which desorbs completely up to 300 ◦C. This reasoning can be
supported by the result in Figs. 1 and 2 indicating that almost all
O2 was used for the oxidation of CO at 50 ◦C. The CO adsorbed
on Pt sites reacts with O2 adsorbed on Fe sites, forming CO2. In
the PROX reaction under the steady-state condition, where re-
actant gases are supplied continuously, such Pt sites as weakly
adsorbed H2 may be occupied with CO preferentially, resulting
in the preferential oxidation of CO by the O2 adsorbed con-
tinuously on the neighboring Fe sites. This is the reason why
Pt–Fe/M exhibits superior selectivity at such a low operating
temperature, despite the presence of a large excess of H2 com-
pared with CO as well as the added O2 in reforming gases.
by our XANES analysis [18]. As the result, no PROX activity
appeared (as seen in Fig. 1), because of the lack of essential
requisites for the Langmuir–Hinshelwood mechanism. At Pt–
Fe/M, the foregoing results and discussion clearly indicate that
Pt sites are available for the adsorption of CO as well as H2
,
and that Fe sites act as O2 adsorption sites. CO adsorbed on a
Pt site and O adsorbed on an Fe site react immediately even at
50 ◦C once both reactants sit on such neighboring sites. This
is the mechanism that Watanabe and Motoo proposed as the
so-called “bifunctional mechanism” for the electrocatalytic ox-
idation of “C-containing reactants” on binary alloys such as
Pt–Ru [24,25]. A PROX reaction on Au catalysts supported
on TiO2, Al2O3, and ZrO2, an oxidation of CO by H–O–O
species, generated via the reaction between dissociatively ad-
sorbed H2 on the gold particles and O2 molecule from the gas
phase, was suggested [26]. In this mechanism, both CO2 and
H2 generation must be observed as the result of the reaction
between CO and H–O–O species. But when an O2 pulse was
introduced to the Pt–Fe/M catalyst saturated with CO and H2,
CO2 was formed but H2 was not detected, as seen Fig. 7b. This
experimental result strongly suggests that the PROX reaction
on Pt–Fe/M catalyst proceeds not via the pathway proposed for
Au-supported catalyst, but via the bifunctional mechanism that
we have proposed. Perfect dispersion (or neighborhood) of two
types of sites may not be required for the mechanism as long as
they are close enough for the surface diffusions of both types
to adsorbed reactants. In addition to the components for the bi-
functions, the special reaction spaces of zeolite cages are also
essential to achieving the desired reactivity and selectivity, as
indicated by a performance different than that of the conven-
tional PROX catalysts. A reason why H2 on Pt sites of Pt/M or
Pt–Fe/M is less active than CO at the PROX reaction has not yet
been clearly explained, but it does happen and leads to superior
selectivity.
3.2.4. Mechanisms of the PROX reaction
Based on the foregoing observations and discussions, we can
summarize schematically the adsorption of CO, O2, and/or H2
and the reaction processes at the different catalysts, as shown
in Fig. 8. As seen in Figs. 6 and 7, no PROX reaction occurs
because the reaction sites are fully covered with CO and/or
H2 strongly adsorbed on Pt/M due to blocked access of O2
to the reaction sites. This strongly indicates that a dissocia-
tive adsorption of O2 and the following surface reaction with
preadsorbed CO are essential for the PROX reaction, that is,
a Langmuir–Hinshelwood mechanism. The reaction can occur
only at Pt/M as the reaction temperature is elevated (>120 ◦C),
maybe because both the CO coverage and the bonding strength
are lowered and the resulting CO-free sites are available for the
dissociative adsorption of O2 (see Figs. 1 and 4). But Fe/M
has no affinity for CO adsorption, as seen in Fig. 4, presum-
ably because Fe sites are dominantly in FeO phase as indicated
4. Conclusion
The PROX activity of Pt/M, Fe/M, and Pt–Fe/M was ex-
amined. Pt/M and Fe/M did not show any activity at 50 ◦C.
However, Pt–Fe/M showed distinctive PROX reactivity and se-
lectivity at the same temperature—for example, it achieved the
ideal performance of 100% at even λ (2 × O2/CO) = 1.0 and
SV = 12,500 h−1, with no noticeable decline in selectivity even
at SV = 100,000 h−1. CO, H2, and O2 chemisorption measure-
ments demonstrated that Fe/M cannot adsorb CO and H2, but
can absorb O2, whereas both Pt/M and Pt–Fe/M show a high
affinity to both CO and H2 adsorption. It was also found that
adding Fe to Pt/M can preserve O2 adsorption sites for the
PROX reaction even in CO/excess H2 mixed gas. Regarding
the PROX mechanism at low temperatures on Pt/M, Fe/M, and
Pt–Fe/M, the poor reactivity of Pt/M and Fe/M can be ascribed
to the lack of CO and/or O2 adsorption as the essential requi-
site for Langmuir–Hinshelwood mechanism. We proposed the
so-called “bifunctional mechanism” for the distinctive perfor-
mance at Pt–Fe/M, where Pt site acts as CO adsorption site and
Fe site acts as an O2 dissociative-adsorption site and enhances
Fig. 8. PROX mechanism, schematically shown, at (a) Pt/M, (b) Fe/M and
(c) Pt–Fe/M catalysts.