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均苯三甲酸在Cu(110)上的氢键和配位键超分子结构

Hydrogen and coordination bonding supramolecular structures of trimesic acid on Cu(110).

作者信息

Classen Thomas, Lingenfelder Magalí, Wang Yeliang, Chopra Rishav, Virojanadara Chariya, Starke Ulrich, Costantini Giovanni, Fratesi Guido, Fabris Stefano, de Gironcoli Stefano, Baroni Stefano, Haq Sam, Raval Rasmita, Kern Klaus

机构信息

Max-Planck-Institut für Festkörperforschung, Heisenbergstrasse 1, D-70569 Stuttgart, Germany.

出版信息

J Phys Chem A. 2007 Dec 13;111(49):12589-603. doi: 10.1021/jp076037o. Epub 2007 Nov 10.

Abstract

The adsorption of trimesic acid (TMA) on Cu(110) has been studied in the temperature range between 130 and 550 K and for coverages up to one monolayer. We combine scanning tunneling microscopy (STM), low-energy electron diffraction (LEED), reflection absorption infrared spectroscopy (RAIRS), X-ray photoemission spectroscopy (XPS), and density functional theory (DFT) calculations to produce a detailed adsorption phase diagram for the TMA/Cu(110) system as a function of the molecular coverage and the substrate temperature. We identify a quite complex set of adsorption phases, which are determined by the interplay between the extent of deprotonation, the intermolecular bonding, and the overall energy minimization. For temperatures up to 280 K, TMA molecules are only partly deprotonated and form hydrogen-bonded structures, which locally exhibit organizational chirality. Above this threshold, the molecules deprotonate completely and form supramolecular metal-organic structures with Cu substrate adatoms. These structures exist in the form of single and double coordination chains, with the molecular coverage driving distinct phase transitions.

摘要

在130至550 K的温度范围内,研究了均苯三甲酸(TMA)在Cu(110)上的吸附情况,覆盖度高达一个单层。我们结合扫描隧道显微镜(STM)、低能电子衍射(LEED)、反射吸收红外光谱(RAIRS)、X射线光电子能谱(XPS)以及密度泛函理论(DFT)计算,得出了TMA/Cu(110)体系详细的吸附相图,该相图是分子覆盖度和衬底温度的函数。我们确定了一组相当复杂的吸附相,这些吸附相由去质子化程度、分子间键合以及整体能量最小化之间的相互作用决定。对于高达280 K的温度,TMA分子仅部分去质子化并形成氢键结构,这些结构局部呈现出组织手性。高于此阈值,分子完全去质子化并与Cu衬底吸附原子形成超分子金属有机结构。这些结构以单配位链和双配位链的形式存在,分子覆盖度驱动着不同的相变。

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