TY - JOUR
T1 - Structure of rutile TiO2 (1 1 0) in water and 1 molal Rb+ at pH 12
T2 - Inter-relationship among surface charge, interfacial hydration structure, and substrate structural displacements
AU - Zhang, Zhan
AU - Fenter, Paul
AU - Sturchio, Neil C.
AU - Bedzyk, Michael J.
AU - Machesky, Michael L.
AU - Wesolowski, David J.
N1 - Funding Information:
We would like to thank Dr. Lawrence Anovitz for the treatments of the rutile crystal. We would also like to thank Drs. Peter Lee, Yuegang Zhang, and Suresh Narayanan for their assistance in beamline setup. This work was performed primarily at beamline 1-BM at the Advanced Photon Source, with preliminary measurements performed at 12-BM, 11-ID-D and 12-ID-D. This work was supported by U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences, Chemical Sciences, Geosciences, and Biosciences Division, and through its support for the Advanced Photon Source, under Contract DE-AC02-06CH11357.
PY - 2007/2/15
Y1 - 2007/2/15
N2 - The rutile (1 1 0)-aqueous solution interface structure was measured in deionized water (DIW) and 1 molal (m) RbCl + RbOH solution (pH 12) at 25 °C with the X-ray crystal truncation rod method. The rutile surface in both solutions consists of a stoichiometric (1 × 1) surface unit mesh with the surface terminated by bridging oxygen (BO) and terminal oxygen (TO) sites, with a mixture of water molecules and hydroxyl groups (OH-) occupying the TO sites. An additional hydration layer is observed above the TO site, with three distinct water adsorption sites each having well-defined vertical and lateral locations. Rb+ specifically adsorbs at the tetradentate site between the TO and BO sites, replacing one of the adsorbed water molecules at the interface. There is no further ordered water structure observed above the hydration layer. Structural displacements of atoms at the oxide surface are sensitive to the solution composition. Ti atom displacements from their bulk lattice positions, as large as 0.05 Å at the rutile (1 1 0)-DIW interface, decay in magnitude into the crystal with significant relaxations that are observable down to the fourth Ti-layer below the surface. A systematic outward shift was observed for Ti atom locations below the BO rows, while a systematic inward displacement was found for Ti atoms below the TO rows. The Ti displacements were mostly reduced in contact with the RbCl solution at pH 12, with no statistically significant relaxations in the fourth layer Ti atoms. The distance between the surface 5-fold Ti atoms and the oxygen atoms of the TO site is 2.13 ± 0.03 Å in DIW and 2.05 ± 0.03 Å in the Rb+ solution, suggesting molecular adsorption of water at the TO site to the rutile (1 1 0) surface in DIW, while at pH 12, adsorption at the TO site is primarily in the form of an adsorbed hydroxyl group.
AB - The rutile (1 1 0)-aqueous solution interface structure was measured in deionized water (DIW) and 1 molal (m) RbCl + RbOH solution (pH 12) at 25 °C with the X-ray crystal truncation rod method. The rutile surface in both solutions consists of a stoichiometric (1 × 1) surface unit mesh with the surface terminated by bridging oxygen (BO) and terminal oxygen (TO) sites, with a mixture of water molecules and hydroxyl groups (OH-) occupying the TO sites. An additional hydration layer is observed above the TO site, with three distinct water adsorption sites each having well-defined vertical and lateral locations. Rb+ specifically adsorbs at the tetradentate site between the TO and BO sites, replacing one of the adsorbed water molecules at the interface. There is no further ordered water structure observed above the hydration layer. Structural displacements of atoms at the oxide surface are sensitive to the solution composition. Ti atom displacements from their bulk lattice positions, as large as 0.05 Å at the rutile (1 1 0)-DIW interface, decay in magnitude into the crystal with significant relaxations that are observable down to the fourth Ti-layer below the surface. A systematic outward shift was observed for Ti atom locations below the BO rows, while a systematic inward displacement was found for Ti atoms below the TO rows. The Ti displacements were mostly reduced in contact with the RbCl solution at pH 12, with no statistically significant relaxations in the fourth layer Ti atoms. The distance between the surface 5-fold Ti atoms and the oxygen atoms of the TO site is 2.13 ± 0.03 Å in DIW and 2.05 ± 0.03 Å in the Rb+ solution, suggesting molecular adsorption of water at the TO site to the rutile (1 1 0) surface in DIW, while at pH 12, adsorption at the TO site is primarily in the form of an adsorbed hydroxyl group.
KW - Adsorption
KW - Electrical double layer
KW - Oxide-water interface
KW - Single crystal surface
KW - Surface structure
KW - Titanium oxide (Rutile)
KW - X-ray reflection
UR - http://www.scopus.com/inward/record.url?scp=33846820452&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=33846820452&partnerID=8YFLogxK
U2 - 10.1016/j.susc.2006.12.007
DO - 10.1016/j.susc.2006.12.007
M3 - Article
AN - SCOPUS:33846820452
SN - 0039-6028
VL - 601
SP - 1129
EP - 1143
JO - Surface Science
JF - Surface Science
IS - 4
ER -