Surface structures of Au and Rh deposited on O-pre-adsorbed Cu(110)

Y Yi-Lin Li (Department of Physics, National Central University 1 , No. 300 Jhongda Road, Jhongli District, Taoyuan 320317,) T Tzu-Yu Liu G Guan-Chen Liu (Department of Physics, National Central University 1 , No. 300 Jhongda Road, Jhongli District, Taoyuan 320317,) Y Yu-Yao Hsia (Department of Physics, National Central University 1 , No. 300 Jhongda Road, Jhongli District, Taoyuan 320317,) Y Yu-Ling Lai (National Synchrotron Radiation Research Center 3 , 101 Hsin-Ann Road, Hsinchu Science Park, Hsinchu 300092,) H Hung-Wei Shiu (National Synchrotron Radiation Research Center 3 , 101 Hsin-Ann Road, Hsinchu Science Park, Hsinchu 300092,) Y Yao-Jane Hsu (National Synchrotron Radiation Research Center 3 , 101 Hsin-Ann Road, Hsinchu Science Park, Hsinchu 300092,) J Jeng-Han Wang (Department of Chemistry, National Taiwan Normal University 2 , No. 88, Sec. 4, Ting-Zhou Road, Taipei 116059,) M Meng-Fan Luo (Department of Physics, National Central University 1 , No. 300 Jhongda Road, Jhongli District, Taoyuan 320317,)

Abstract

We have studied the structures of Au and Rh deposited on (2 × 1)O–Cu(110) and c(6 × 2)O–Cu(110) surfaces with varied surface probe techniques and modeling based on density functional theory. On either (2 × 1)O–Cu(110) or c(6 × 2)O–Cu(110) surface, the deposited Au nucleated into fractal two-dimensional islands and grew further into thin films via a layer-by-layer fashion. Both the (2 × 1) and c(6 × 2) ordered structures persisted notably despite the grown Au thin films, not only as the Au atoms were stacked according to the O–Cu(110) lattice but also as both O and Cua (referring to the added Cu alternating with O at the O–Cu(110) surfaces) remained at the surface and formed Cua–O–Au structures to promote the surface stability. In contrast, the Rh on the O–Cu(110) surfaces formed round, structurally ordered three-dimensional nanoclusters, at the expense of the (2 × 1) and c(6 × 2) structures. The Rh clusters grew preferentially in an fcc phase and (110) orientation, as the (110) facet matched better, structurally, with either (2 × 1)O–Cu(110) or Cu(110) surfaces. The disparate structuring of Au and Rh on O–Cu(110) surfaces was controlled by both lattice and energetic effects; in particular, the bond strengths in the order of Rh–Rh > Rh–O > Au–O > Au–Au at the surfaces predominated. The formation of the surface Cua–O–Au structure, instead of the pure Au multilayers, arose from the stronger Au–O and enhanced Cua–O bonds in the Cua–O–Au structure.

Article Details

Volume / Issue Vol. 163, Issue 2
Published July 14, 2025
ISSN 0021-9606
Publisher American Institute of Physics

Journal Info

The Journal of Chemical Physics

American Institute of Physics

ISSN: 0021-9606 Physical Sciences

Authors (9)

Y

Yi-Lin Li

Department of Physics, National Central University 1 , No. 300 Jhongda Road, Jhongli District, Taoyuan 320317,

T

Tzu-Yu Liu

G

Guan-Chen Liu

Department of Physics, National Central University 1 , No. 300 Jhongda Road, Jhongli District, Taoyuan 320317,

Y

Yu-Yao Hsia

Department of Physics, National Central University 1 , No. 300 Jhongda Road, Jhongli District, Taoyuan 320317,

Y

Yu-Ling Lai

National Synchrotron Radiation Research Center 3 , 101 Hsin-Ann Road, Hsinchu Science Park, Hsinchu 300092,

H

Hung-Wei Shiu

National Synchrotron Radiation Research Center 3 , 101 Hsin-Ann Road, Hsinchu Science Park, Hsinchu 300092,

Y

Yao-Jane Hsu

National Synchrotron Radiation Research Center 3 , 101 Hsin-Ann Road, Hsinchu Science Park, Hsinchu 300092,

J

Jeng-Han Wang

Department of Chemistry, National Taiwan Normal University 2 , No. 88, Sec. 4, Ting-Zhou Road, Taipei 116059,

M

Meng-Fan Luo

Department of Physics, National Central University 1 , No. 300 Jhongda Road, Jhongli District, Taoyuan 320317,