CHARACTERIZATION OF THE RH(111) ELECTRODE BY CEELS, AES, LEED, AND VOLTAMMETRY - ADSORPTION OF (BI)SULFATE, PERCHLORATE, AND CARBON-MONOXIDE

Citation
Ye. Sung et al., CHARACTERIZATION OF THE RH(111) ELECTRODE BY CEELS, AES, LEED, AND VOLTAMMETRY - ADSORPTION OF (BI)SULFATE, PERCHLORATE, AND CARBON-MONOXIDE, Journal of physical chemistry, 99(36), 1995, pp. 13513-13521
Citations number
60
Categorie Soggetti
Chemistry Physical
ISSN journal
00223654
Volume
99
Issue
36
Year of publication
1995
Pages
13513 - 13521
Database
ISI
SICI code
0022-3654(1995)99:36<13513:COTREB>2.0.ZU;2-W
Abstract
We studied the Rh(111) electrode in sulfuric and perchloric acid solut ions, and in sulfuric acid solutions containing dissolved carbon monox ide, using voltammetry, core electron energy loss spectroscopy (CEELS) , Auger electron spectroscopy (AES), and low-energy electron diffracti on (LEED). Emersion of the electrode from the clean H2SO4 solution to ultrahigh vacuum (UHV) produces a stable (root 3 x root 3)R 30 degrees (bi)sulfate surface structure. The (bi)sulfate coverage is close to 0 .33 ML, the valency of (bi)sulfate sulfur is +6, and the oxygen-to-sul fur ratio is 4, the proper value for the (bi)sulfate adsorbate. When ( bi)sulfate is adsorbed from mixed sulfuric/perchloric acid solutions, the (bi)sulfate coverage is lower, namely 0.24 ML. This and some other measurements show that adsorption of perchlorate on rhodium is strong and successfully competes with (bi)sulfate adsorption. CO replaces (b i)sulfate adsorbate irreversibly. In agreement with recent STM investi gations, we observe that the main CO structure is (2 x 2). However, de pending on experimental conditions, a split (2 x 2) also appears, a LE ED analogue of STM's Rh(111)(3 x root 3). The (2 x 2)-CO surface struc ture corresponds to Theta = 0.75 +/- 0.03 ML, while the split (2 x 2) structure corresponds to Theta = 0.65 +/- 0.08 ML. AES shows that at a low potential the linear-bonded CO molecules from the (2 x 2)-CO surf ace structure is substituted in part by the bridge-bonded CO, which in creases back-donation of metal d-electrons to the CO. The stronger bac k-bonding increases the electron screening of the orbital (core) hole, leading to a more fully relaxed final state of the Rh(111)-CO system.