Little is known about
the detailed structural information at the
interface of Pt
n
cluster and γ-Al
2
O
3
(001) surface, which plays an important role
in the dehydrogenation and cracking of hydrocarbons. Here, the nucleation
and growth of Pt
n
(
n
=
1–8, 13) clusters on a γ-Al
2
O
3
(001)
surface have been examined using density functional theory. For the
most stable configuration Pt
n
/γ-Al
2
O
3
(001) (
n
= 1–8, 13),
Pt
n
clusters bond to the γ-Al
2
O
3
(001) surface through Pt–O and Pt–Al
bonds at the expense of electron density of the Pt
n
cluster. With the increase in the Pt
n
cluster size, both the metal–support interaction and
the nucleation energies exhibit an odd–even oscillation pattern,
which are lower for an even Pt
n
cluster
size than those for its adjacent odd ones. Both the metal–surface
and metal–metal interactions are competitive, which control
the nanoparticle morphology transition from two-dimension (2D) to
three-dimension (3D). On the γ-Al
2
O
3
(001)
surface, when the metal–support interaction governs, smaller
clusters such as Pt
1
, Pt
2
, Pt
3
, and
Pt
4
prefer a planar 2D nature. Alternatively, when the
metal–metal interaction dominates, larger clusters such as
Pt
5
, Pt
6
, Pt
7
, Pt
8
, and
Pt
13
exhibit a two-layer structure with one or more Pt
atoms on the top layer not interacting directly with the support.
Herein, the Pt
4
cluster is the most stable 2D structure;
Pt
5
and Pt
6
clusters are the transition from
the 2D to the 3D structure; and the Pt
7
cluster is the
smallest 3D structure.