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Investigation of band gap narrowing in nitrogen-doped La2Ti2O7 with transient absorption spectroscopy

机译:瞬态吸收光谱研究掺氮La2Ti2O7中的带隙变窄

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Doping a semiconductor can extend the light absorption range, however, it usually introduces mid-gap states, reducing the charge carrier lifetime. This report shows that doping lanthanum dititinate (La2Ti2O7) with nitrogen extends the valence band edge by creating a continuum of dopant states, increasing the light absorption edge from 380 nm to 550 nm without adding mid-gap states. The dopant states are experimentally resolved in the excited state by correlating transient absorption spectroscopy with a supercontinuum probe and DFT prediction. The lack of mid-gap states is further confirmed by measuring the excited state lifetimes, which reveal the shifted band edge only increased carrier thermalization rates to the band edge and not interband charge recombination under both ultraviolet and visible excitation. Terahertz (time-domain) spectroscopy also reveals that the conduction mechanism remains unchanged after doping, suggesting the states are delocalized.
机译:掺杂半导体可以扩大光吸收范围,但是,通常会引入中间能隙状态,从而缩短了载流子寿命。该报告表明,用氮掺杂二钛酸镧(La2Ti2O7)通过创建连续的掺杂状态扩展了价带边缘,从而将光吸收边缘从380 nm增加到550 nm,而没有增加中间间隙状态。通过将瞬态吸收光谱与超连续谱探针和DFT预测相关联,可以在激发态下通过实验解析掺杂态。通过测量激发态寿命进一步证实了中间带隙态的缺乏,这表明位移的谱带边缘仅在紫外和可见光激发下增加了载流子对谱带边缘的热化速率,而没有谱带间的电荷复合。太赫兹(时域)光谱还揭示了掺杂后的传导机制保持不变,表明这些状态是离域的。

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