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通过分子波函数的细微变化测量表面散射中与温度相关的立体动力学。

Temperature dependent stereodynamics in surface scattering measured through subtle changes in the molecular wave function.

作者信息

Chadwick Helen, Alexandrowicz Gil

机构信息

Department of Chemistry, Faculty of Science and Engineering, Swansea University, Swansea, SA2 8PP, UK.

出版信息

Faraday Discuss. 2024 Aug 27;251(0):76-91. doi: 10.1039/d4fd00007b.

DOI:10.1039/d4fd00007b
PMID:38775459
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC11349063/
Abstract

A magnetically manipulated molecular beam technique is used to change the rotational orientation of H molecules which collide with a stepped Cu(511) surface and explore how the polarisation dependence of molecules scattering into the specular channel changes as a function of surface temperature. At all temperatures, H molecules that are rotating like cartwheels are more likely to be scattered into the specular channel than those that are rotating like helicopters. Furthermore, the scattered molecules are more likely to be rotating like cartwheels, regardless of their state before the collision. Increasing the temperature of the Cu(511) surface causes the polarisation effects to become stronger, with the scattering becoming more selective for H with cartwheel like rotation. Therefore, scattering a molecular beam of H from a Cu(511) surface and taking the molecules scattered into the specular channel provides a method to create a rotationally polarised beam of H, where the polarisation can be tuned by changing the surface temperature. In contrast, the rotational orientation dependence observed for specular scattering from a flat Cu(111) surface is independent of surface temperature within the same temperature range.

摘要

一种磁控分子束技术被用于改变与阶梯状Cu(511)表面碰撞的H分子的旋转取向,并探索散射到镜面通道中的分子的极化依赖性如何随表面温度变化。在所有温度下,像侧手翻一样旋转的H分子比像直升机一样旋转的分子更有可能散射到镜面通道中。此外,无论碰撞前分子的状态如何,散射后的分子更有可能像侧手翻一样旋转。提高Cu(511)表面的温度会使极化效应变得更强,散射对像侧手翻一样旋转的H变得更具选择性。因此,从Cu(511)表面散射H分子束并收集散射到镜面通道中的分子,提供了一种创建旋转极化H束的方法,其中极化可以通过改变表面温度来调节。相比之下,在相同温度范围内,从平坦的Cu(111)表面进行镜面散射所观察到的旋转取向依赖性与表面温度无关。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3ada/11349063/4476c695afe5/d4fd00007b-f6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3ada/11349063/aab7f35b81ea/d4fd00007b-f1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3ada/11349063/49a8865d59d5/d4fd00007b-f2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3ada/11349063/8587c3e19662/d4fd00007b-f3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3ada/11349063/ec5b19f5d94d/d4fd00007b-f4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3ada/11349063/9276fd11c818/d4fd00007b-f5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3ada/11349063/4476c695afe5/d4fd00007b-f6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3ada/11349063/aab7f35b81ea/d4fd00007b-f1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3ada/11349063/49a8865d59d5/d4fd00007b-f2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3ada/11349063/8587c3e19662/d4fd00007b-f3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3ada/11349063/ec5b19f5d94d/d4fd00007b-f4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3ada/11349063/9276fd11c818/d4fd00007b-f5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3ada/11349063/4476c695afe5/d4fd00007b-f6.jpg

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