首页> 外文期刊>The Journal of Chemical Physics >CO ON PT(335) - ELECTRIC FIELD SCREENING ON A STEPPED SURFACE
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CO ON PT(335) - ELECTRIC FIELD SCREENING ON A STEPPED SURFACE

机译:CO ON PT(335)-阶梯表面上的电场筛选

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We compare CO's response to electric fields at edge and terrace sites on the stepped Pt(335) surface. The comparison is made at zero frequency and at the frequency of the C-O stretch vibration. Atop-bonded CO is observed with reflection-absorption ir spectroscopy (RAIRS), electroreflectance vibrational spectroscopy (EVS), and high-resolution electron energy loss spectroscopy (HREELS). Coadsorbed H or O is used to control the CO adsorption site. With both RAIRS and HREELS the measured vibrational cross-section of atop CO at the step edge is 2.0+/-0.2 times greater than for CO on the terrace. The vibrational Stark effect-the change of CO's vibrational frequency with externally applied electrostatic field-is also a factor 2.0+/-0.2 larger for atop CO at the step edge than it is for atop CO on the terrace. Because the vibrational cross section varies as the square of the field while the Stark effect is linear, a model in which CO responds to the screened local field at a single point cannot simultaneously explain the observed site dependence of both the vibrational Stark effect and the vibrational cross section. The most plausible explanation is that CO's response to electric fields is nonlocal. A simple model is presented that can account for our data. (C) 1995 American Institute of Physics. [References: 80]
机译:我们比较了CO对阶梯式Pt(335)表面边缘和平台部位电场的响应。比较是在零频率和C-O拉伸振动频率下进行的。通过反射吸收红外光谱(RAIRS),电反射振动光谱(EVS)和高分辨率电子能量损失光谱(HREELS)观察到键合顶部的CO。共吸附的H或O用于控制CO的吸附位置。使用RAIRS和HREELS时,台阶边缘上CO的测量振动截面比平台上CO的测量振动截面大2.0 +/- 0.2倍。斯塔克振动效应-外加静电场引起的CO振动频率的变化-与台阶处的CO顶部相比,阶梯边缘的CO顶部的系数也大2.0 +/- 0.2。因为振动横截面随场的平方而变化,而斯塔克效应是线性的,所以其中CO对单个点处的屏蔽局部场做出响应的模型无法同时解释观测到的振动斯塔克效应和振动的站点依赖性。横截面。最合理的解释是CO对电场的响应是非局部的。提出了一个可以解释我们数据的简单模型。 (C)1995年美国物理研究所。 [参考:80]

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