物理化学学报
物理化學學報
물이화학학보
ACTA PHYSICO-CHIMICA SINICA
2012年
8期
1861-1868
,共8页
赵伟娜%林华香%李奕%章永凡%黄昕%陈文凯
趙偉娜%林華香%李奕%章永凡%黃昕%陳文凱
조위나%림화향%리혁%장영범%황흔%진문개
密度泛函理论%TiO2(110)表面%双金属簇
密度汎函理論%TiO2(110)錶麵%雙金屬簇
밀도범함이론%TiO2(110)표면%쌍금속족
Density functional theory%TiO2(110) surface%Bimetallic cluster
采用自旋极化密度泛函和广义梯度近似的方法并结合周期平板模型,探讨了不同覆盖度(θ)下双金属簇X (X=Pt-Au,Au-Au)在(3x2)riO2(110)完整表面上的吸附行为.另外,在本文给出的所有覆j盖度模式下(θ=1/6-1 ML),我们仪研究其基态构型.计算结果表明:当θ<1/2 ML时,金属簇X在TiO2(110)表面上吸附能随覆盖度的增加而增加;当θ>1/2 ML时,除了饱和覆盖度下,吸附能随覆盖度的增加而减小;当θ=1/2 ML时,吸附能最大.即使Pt-Au/TiO2体系的吸附能比Au-Au/TiO2体系的小,但相对于Au-Au簇,Pt-Au簇更容易在TiO2(110)表面上形成双金属单分子层.在半覆盖和全覆盖下,X簇的峰与TiO2的峰在-3.0 eV到费米能级之间产生明显重叠,表明簇与底物之间存在化学作用.且当覆盖度小时,X-TiO2相互作用是成簇的主要因素;随着覆盖度的增大,X-X原子间相互作用就逐渐变成了成簇的主要动力.
採用自鏇極化密度汎函和廣義梯度近似的方法併結閤週期平闆模型,探討瞭不同覆蓋度(θ)下雙金屬簇X (X=Pt-Au,Au-Au)在(3x2)riO2(110)完整錶麵上的吸附行為.另外,在本文給齣的所有覆j蓋度模式下(θ=1/6-1 ML),我們儀研究其基態構型.計算結果錶明:噹θ<1/2 ML時,金屬簇X在TiO2(110)錶麵上吸附能隨覆蓋度的增加而增加;噹θ>1/2 ML時,除瞭飽和覆蓋度下,吸附能隨覆蓋度的增加而減小;噹θ=1/2 ML時,吸附能最大.即使Pt-Au/TiO2體繫的吸附能比Au-Au/TiO2體繫的小,但相對于Au-Au簇,Pt-Au簇更容易在TiO2(110)錶麵上形成雙金屬單分子層.在半覆蓋和全覆蓋下,X簇的峰與TiO2的峰在-3.0 eV到費米能級之間產生明顯重疊,錶明簇與底物之間存在化學作用.且噹覆蓋度小時,X-TiO2相互作用是成簇的主要因素;隨著覆蓋度的增大,X-X原子間相互作用就逐漸變成瞭成簇的主要動力.
채용자선겁화밀도범함화엄의제도근사적방법병결합주기평판모형,탐토료불동복개도(θ)하쌍금속족X (X=Pt-Au,Au-Au)재(3x2)riO2(110)완정표면상적흡부행위.령외,재본문급출적소유복j개도모식하(θ=1/6-1 ML),아문의연구기기태구형.계산결과표명:당θ<1/2 ML시,금속족X재TiO2(110)표면상흡부능수복개도적증가이증가;당θ>1/2 ML시,제료포화복개도하,흡부능수복개도적증가이감소;당θ=1/2 ML시,흡부능최대.즉사Pt-Au/TiO2체계적흡부능비Au-Au/TiO2체계적소,단상대우Au-Au족,Pt-Au족경용역재TiO2(110)표면상형성쌍금속단분자층.재반복개화전복개하,X족적봉여TiO2적봉재-3.0 eV도비미능급지간산생명현중첩,표명족여저물지간존재화학작용.차당복개도소시,X-TiO2상호작용시성족적주요인소;수착복개도적증대,X-X원자간상호작용취축점변성료성족적주요동력.
Based on spin-polarized density functional theory and generalized gradient approximation (DFT-GGA) calculations,the coverage-dependent adsorption of X bimetallic clusters (X=Pt-Au,Au-Au) on the (3 × 2) TiO2(110) surface has been investigated utilizing periodic supercell models in the absence of oxygen vacancy sites.Only the ground-state structures corresponding to the given coverage patterns (θ=1/6-1 ML) for X clusters are discussed in this work.The unambiguous results reveal that the adsorption energies increase with coverage up to 1/2 ML and then decrease except for when saturated coverage is reached.According to the interaction with X clusters,it is more feasible at all coverage levels to create a monolayer film of Pt-Au bimetallic clusters on the TiO2(110) surface than it is to create a monolayer of Au-Au clusters,even though the adsorption energy of the Pt-Au/TiO2 adsorption system is smaller in comparison with that of the Au-Au/TiO2 system.Importantly,especially for the half and saturated coverages,there is a broadening of X peaks overlapping with the TiO2 state ranging from -3.0 eV to the Fermi level,suggesting a strong interaction between the surface and bimetallic cluster.Also of particular interest is the adsorptive mechanism where the X-TiO2 interaction is the main driving force at the initial stage of the adsorption process,whereas the X-X interaction controls the process as the coverage increases.