NO and CO Adsorption on Nonhomogeneous Pt(100)
Surfaces
D. Y. Zemlyanov,* M. Yu. Smirnov, and E. I. Vovk
Boreskov Institute of Catalysis, Pr. Akademika Lavrentieva 5, 630090 Novosibirsk, Russia
Received July 1, 1998. In Final Form: October 1, 1998
The adsorption of NO and CO on a nonhomogeneous Pt(100) surface made up of both the (hex) and
(1 × 1) structural phases was studied at 300 K by means of high-resolution electron energy-loss spectroscopy
(HREELS). The nonhomogeneous surface was prepared by titrating NOads/(1 × 1) islands formed on the
original (hex) surface with deuterium and subsequent heating to desorb residual Dads. The as-prepared
surface was assumed to consist of patches of the (1 × 1) structure surrounded by the (hex) surface. The
ratio between the (1 × 1) patches and the (hex) area was controlled by the initial coverage of NOads before
titration. The exposure of the nonhomogeneous surface to NO or CO at 300 K led to saturation of the (1
× 1) patches first. It was supposed that the NO and CO molecules adsorbing on the (hex) areas quickly
diffuse along the surface, meet the (1 × 1) patches, and are “trapped” by them. NOads (COads) spreads on
the surface of the (1 × 1) patches. As soon as the (1 × 1) patches are saturated, the adsorption-induced
(hex) f (1 × 1) back-reconstruction takes place. The details of the NO and CO adsorption on the
nonhomogeneous surface were compared with the process on the reconstructed and unreconstructed Pt-
(100) surfaces.
1. Introduction
The Pt(100) surface shows two surface structures, which
exhibit dramatically different adsorption and catalytic
properties,
1
making it an attractive subject for model
studies. The clean Pt(100) surface undergoes a recon-
struction under ultrahigh vacuum (UHV) conditions and
exhibits a hexagonal (hex) surface structure, characterized
by a (5 × 20) low-energy electron diffraction (LEED)
pattern.
2-5
The unreconstructed (1 × 1) surface can be
prepared by the procedure described by Bonzel et al.
5
This
procedure includes NO adsorption on the reconstructed
Pt(100) surface up to saturation at 300 K, subsequent
heating of the NO
ads
layer, reduction with hydrogen of the
O
ads
species formed by NO dissociation, and heating to
remove residual H
ads
. The clean (1 × 1) surface is
metastable, converting back to the (hex) structure at
temperatures above 400 K.
The adsorption of both CO and NO on the Pt(100) surface
has been studied in detail by a number of surface science
techniques. The following scheme of NO and CO adsorption
on the Pt(100)-(hex) surface at 300 K could be formulated
on the basis of data from the literature. Adsorption of NO
and CO induces locally the transition of the (hex) phase
to the (1 × 1) one, leading to the formation of NO
ads
/
(1 × 1) or CO
ads
/(1 × 1) islands.
6-12
The local coverage on
the (1 × 1) islands is approximately 0.5 ML,
13
whereas
the (hex) phase surrounding the islands is nearly free of
adsorbates.
6,9
According to LEED and scanning tunneling microscopy
(STM) data,
14-17
the formation of the CO
ads
/(1 × 1) and
NO
ads
/(1 × 1) islands proceeds through a nucleation and
trapping mechanism that includes two stages. The first
stage is assumed to be the generation of the centers of
nucleation presumably on the (hex) phase on the basis of
surface structural defects.
17
During the second stage the
growth of the adsorption islands proceeds without the
appearance of new centers of nucleation.
The atomic density of the (1 × 1) surface is 1.28 × 10
15
cm
-2
.
4
This value is approximately 20% lower than the
one of the (hex) surface (1.61 × 10
15
cm
-2
).
15
This difference
results in a significant mass-transport of platinum atoms
during the NO
ads
/(1 × 1) and CO
ads
/(1 × 1) island formation.
STM data demonstrate
15-17
that platinum atoms expelled
during the (hex) f (1 × 1) transition form clusters with
a size of ∼15-25 Å. The clusters are distributed randomly
within the (1 × 1) patches. Two molecular adsorption states
of NO were detected in the NO
ads
/(1 × 1) islands by means
of infrared absorption spectroscopy (IRAS)
6
and high-
resolution electron energy-loss spectroscopy (HREELS),
18-20
namely on the surface of the (1 × 1) patches and on
structural defects lifted by the (hex) f (1 × 1) reconstruc-
* Corresponding author. Fax: +7 (3832* 343056. E-mail: dzem@
catalysis.nsk.su.
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135 Langmuir 1999, 15, 135-140
10.1021/la980793r CCC: $18.00 © 1999 American Chemical Society
Published on Web 01/05/1999