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Investigating Polaron Formation in Anatase and BrookiteTiO2 by Density Functional Theory with Hybrid-Functionaland DFT + U Methods

机译:研究锐钛矿和板钛矿中的极化子形成混合功能的密度泛函理论研究TiO2和DFT + U方法

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摘要

Anatase and brookite are robust materials with enhanced photocatalytic properties. In this study, we used density functional theory (DFT) with a hybrid functional and the Hubbard on-site potential methods to determine electron- and hole-polaron geometries for anatase and brookite and their energetics. Localized electron and hole polarons were predicted not to form in anatase using DFT with hybrid functionals. In contrast, brookite formed both electron and hole polarons. The brookite electron-polaronic solution exhibits coexisting localized and delocalized states, with hole polarons mainly dispersed on two-coordinated oxygen ions. Hubbard on-site potential testing over the wide 4.0–10 eV range revealed that brookite polarons are formed at U = 6 eV, while anatase polarons are formed at U = 8 eV. The brookite electron polaron was always localized on a single titanium ion under the Hubbard model, whereas the hole polaron was dispersed over four oxygen atoms, consistent with the hybrid DFT studies. The anatase electron polarons were dispersed at lower on-site potentials but were more localized at higher potentials. Both methods predictthat brookite has a higher driving force for the formation of polaronsthan anatase.
机译:锐钛矿和板钛矿是具有增强的光催化性能的坚固材料。在这项研究中,我们使用具有混合功能的密度泛函理论(DFT)和Hubbard现场电势方法来确定锐钛矿和板钛矿及其能量学的电子和空穴极化子几何形状。使用具有混合功能的DFT,可以预测在锐钛矿中不会形成局部电子和空穴极化子。相反,板钛矿同时形成电子和空穴极化子。板钛矿电子极化溶液具有局域和局域共存的状态,空穴极化子主要分散在两个配位的氧离子上。 Hubbard在4.0-10 eV宽范围内的现场电势测试表明,板钛矿极化子在U = 6 eV时形成,而锐钛矿极化子在U = 8 eV时形成。在Hubbard模型下,板钛矿电子极化子始终位于单个钛离子上,而空穴极化子则分散在四个氧原子上,这与混合DFT研究一致。锐钛矿型电子极化子分散在较低的现场电势,但更多地位于较高的电势。两种方法都可以预测板钛矿对极化子的形成具有更高的驱动力比锐钛矿。

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