1188 J. Phys. Chem. B, Vol. 101, No. 7, 1997
Sasahara et al.
The as-deposited surface of ca. 1.5 monolayers of Pt ions on
Rh(110) gave a XPS peak ratio of Rh 3d5/2/Pt 4d3/2 ) 1.1, but
this surface showed no LEED pattern. No appreciable con-
tamination was detected on this surface by XPS. This reveals
that the deposition of Pt on Rh(110) surface is not pseudomor-
phic.
It was shown that the XPS peak for the Pt of a Pt-deposited
Rh(100) surface changes little by heating to 1050 K in UHV8,9
but is drastically changed by heating in O2, and a p(3×1) LEED
pattern is established at 600 K with increasing Rh atoms by
reacting with oxygen.8,9 Recently, our STM image shows that
the p(3×1) surface is reflected by an ordered arrangement of
Pt and Rh-O rows on the surface.18 Therefore, hereafter the
reconstructed surface is described by a (Pt-Rh-O-Pt). If we
compare the catalytic activity of Rh(100), Pt/Rh(100), and (Pt-
Rh-O-Pt)/Rh(100) for the reaction of NO + H2, it is clear
that the (Pt-Rh-O-Pt)/Rh(100) is extremely active for the NO
+ H2 reaction.13 From these results, it was deduced that the
reconstruction is responsible for the prominent catalytic activity
of the Pt-Rh catalyst for the NO + H2 reaction.
Figure 3. Change of the Rh 3d5/2/Pt 4d3/2 ratio of the XPS spectrum
and LEED pattern of Pt/Rh(110) surfaces.
As mentioned above, the Pt layer on the Pt/Rh(100) surface
is stable at ca. 1000 K in vacuum,8 but the XPS ratio of Rh
3d5/2/Pt 4d3/2 for the Pt/Rh(110) surface was increased by
annealing at 1000 K for 30 min. This fact indicates that the Pt
atoms on the Rh(110) surface are less stable than those on the
Rh(100) surface so that the Pt atoms are diffused into the Rh
crystal. In other words, thermal stability of the Pt layer on the
Rh surface depends on the crystallographic planes. A Pt/Rh-
(110) surface annealed at 1000 K, which gave a p(1×1) LEED
pattern, did not show a very high activity for the reduction of
NO with H2, as shown in Figure 2 with solid circles. It is
interesting that a characteristic N2 peak observed on the Rh-
(110) surface also appeared at ca. 440 K, as shown in Figure 2
with open circles, which may suggest that the Pt/Rh(110)
annealed at 1000 K is almost covered with Rh atoms instead of
Pt.
structure is established. To compare the catalytic activity of
the Pt/Rh(110) surface, the reaction of NO with H2 was
performed on a p(1×n) Pt/Rh(110) surface having a ratio of
Rh 3d5/2/Pt 4d3/2 ) 2.7, where the p(1×n) surface was previously
prepared by heating the c(2×2) surface in 1 × 10-7 Torr of H2
at 760 K. As mentioned above, the Rh/Pt ratio of the p(1×n)
Pt/Rh(110) surface was changed little by treating with H2 at
760 K, and it is the same on the c(2×2) surface obtained by
heating in O2. However, as shown in Figure 2 with triangles,
the p(1×n) Pt/Rh(110) surface showed a remarkable catalytic
activity for the reaction and N2 evolution occurred at ca. 400
K, which is almost the same temperature for the NO + H2
reaction on the p(3×1) (Rh-O-Pt)/Rh(100) surface.12 This
fact may reveal that similar active sites are formed on both (Rh-
O-Pt)/Rh(100) and c(2×2) or p(1×n) Pt/Rh(110) surfaces.
When an as-deposited Pt/Rh(110) surface was heated in 1 ×
10-7 Torr of H2 at 760 K for 10 min, the LEED pattern changed
to a p(1×n) but the Rh 3d5/2/Pt 4d3/2 ratio of the XPS peaks
changed little. This p(1×n) LEED pattern was stable at 760 K
in UHV and no O 1s XPS peak was detected. When the p(1×n)
surface was annealed at 760 K in 1 × 10-7 Torr of O2 for 60
min, the LEED pattern sequentially changed from the p(1×n)
to a p(1×3) pattern and finally to a c(2×2) pattern as shown in
Figure 3. In accordance with the LEED pattern change, the
Rh 3d5/2/Pt 4d3/2 ratio and the O 1s peak of the XPS spectrum
increased concomitantly as shown in Figures 3 and 4. Taking
account of the fact that the Pt and Rh atoms cannot diffuse very
rapidly at temperatures lower than 900 K,19 the rapid increase
of the Rh 3d5/2/Pt 4d3/2 ratio at 760 K is caused by the reaction
of Rh with O2. The p(1×n) and the p(1×3) patterns were stable
even at 760 K in H2, but the c(2×2) surface changed to a (1×n)
structure in 1 × 10-7 Torr of H2 at 760 K. It should be pointed
out that the c(2×2) is not influenced at room temperature by
exposure to H2. Contrary to the Pt/Rh(110) surface, the Pt/
Rh(100) surface gives the p(3×1) + p4g p(2×2) LEED pattern
by heating in O2 at 600 K and this surface readily changes to
the p(1×1) structure at room temperature by exposure to H2.
By reaction of Rh atoms with O, Rh atoms were segregated
on the Pt0.25Rh0.75(100) alloy surface by exposure to O2 or NO,20
and it is the same on the Pt/Rh(110) surface. The extraction of
Rh atoms on the Pt/Rh(110) surface by reacting with O2 can be
diagnosed by the cyclic voltammogram for the Pt/Rh(110)
2-
surface. To avoid the influence of Cl- ions from PtCl6 on
the voltammogram,11 the Pt/Rh(110) disk was washed with
superpure water and then the cyclic voltammogram was obtained
in 0.05 M H2SO4 solution. It is known that the peak at -0.21
V(SCE) attributable to the Rh(110) surface (Figure 1a) is
suppressed as the deposition of Pt atoms increases and a shoulder
appears at around -0.15 V(SCE), as shown in Figure 1b. After
the washing of this surface with superpure water, the Pt/Rh-
(110) disk was transferred to the main UHV chamber and was
characterized by LEED and XPS. The amount of Pt deposited
on the Rh(110) surface was estimated to be 0.9 monolayer by
the XPS, where no clear LEED pattern was observed.
Although this Pt/Rh(110) surface was heated at a rate of 1
K/s to 760 K in UHV, no clear LEED pattern was observed.
The Rh 3d5/2/Pt 4d3/2 ratio is not very sensitive to the
compositional change of the topmost layer,21 but the cyclic
voltammogram may be sensitive to the topmost layer. In fact,
the cyclic voltammogram for the surface annealed at 760 K in
UHV gave a new peak at ca. -0.15 V(SCE) as shown in Figure
5a, although the ratio of Rh/Pt changed little. By comparison
of the cyclic voltammogram of the annealed surface to that of
Rh(110) surface, the new peak at -0.15 V(SCE) is responsible
for the characteristic peak of the Pt layer. Therefore, the Pt
As mentioned above, Pt layer formed on the Rh surface has
different stability depending on the crystallographic planes of
Rh crystal in vacuum. However, the extraction of Rh by O2
was commonly observed on both the Pt/Rh(110) and Pt/Rh-
(100) surfaces. The Pt/Rh(100) surface gave high catalytic
activity for the NO reduction when Rh atoms are extracted by
reacting with O2; that is, the p(3×1) (Pt-Rh-O-Pt)/Rh(100)