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Modeling CO2 reduction on Pt(111)

机译:模拟Pt(111)上的二氧化碳减少量

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Density functional theory was used to model the electrochemical reduction of CO2 on Pt(111) with an explicit solvation layer and the presence of extra hydrogen atoms to represent a negatively charged electrode. We focused on the electronic energy barriers for the first four lowest energy proton-electron transfer steps for reducing CO2 on Pt(111) beginning with adsorbed ~*CO2 and continuing with *COOH, ~*CO + H2O, ~*COH, and ending with ~*C + H2O. We find that simple elementary steps in which a proton is transferred to an adsorbate (such as the protonation of ~*CO to ~*COH) have small barriers on the order of 0.1 eV. Elementary steps in which a proton is transferred and a C-0 bond is simultaneously cleaved show barriers on the order of 0.5 eV. All barriers calculated for these steps show no sign of being insurmountable at room temperature. To explain why these barriers are so small, we analyze the charge density and the density of states plots to see that first, the electron transfer is decoupled from the proton transfer so that in the initial state, the surface and adsorbate are already charged up and can easily accept the proton from solution. Also, we see that in the cases where barriers are on the order of 0.1 eV, electron density in the initial state localizes on the oxygen end of the adsorbate, while electron density is more spread out on the surface for initial states of the C-O bond cleaving elementary steps.
机译:密度泛函理论用于模拟在具有明显溶剂化层的Pt(111)上CO2的电化学还原,以及存在额外的氢原子以表示带负电的电极。我们专注于前四个最低能级质子电子转移步骤的电子能垒,以减少Pt(111)上的CO2,从吸附〜* CO2开始,再从* COOH,〜* CO + H2O,〜* COH到结束用〜* C + H2O。我们发现质子转移到吸附质的简单基本步骤(例如〜* CO到〜* COH的质子化)具有约0.1 eV的小势垒。质子被转移并且C-0键被同时裂解的基本步骤显示出约0.5eV的势垒。计算出的这些步骤的所有势垒都没有迹象表明在室温下是无法克服的。为了解释为什么这些势垒如此之小,我们分析了电荷密度和状态密度图,发现首先,电子转移与质子转移解耦,因此在初始状态下,表面和被吸附物已经带电,可以很容易地接受溶液中的质子此外,我们看到在势垒为0.1 eV量级的情况下,初始状态的电子密度位于被吸附物的氧端,而对于CO键的初始状态,电子密度更多地分布在表面上分解基本步骤。

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