表面效应对过渡金属氧化物微晶非线性光学性质的影响

H. Fei, Xicheng Ai, Li Han, R. Nie, Zhenhua Hu
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For the first time, we studied the nonlinear optical properties of translation metal-oxide microcrystallites by coating the surface with a layer of organic polar molecule(DBS etc.), and found that the change of the surface environment could alter the optical properties greatly. For Fe2O3 as example, (1) the absorption incresed toward the high energy side, (2) the laser induced luminescence intensity decreased by 2 orders in magnitude, and on the contrary, the Raman signal of the surface was enhanced greatly, (3) the saturable absorption phenomenon disappeared, (4) larger third order susceptibility and faster excited state relaxation were obtained compared with uncoated Fe2O3 microcrystallite. 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引用次数: 0

摘要

微晶的光学和电子性质的尺寸依赖性修饰最近引起了相当大的关注[1-4]。当微晶的直径接近其对应的激子玻尔直径时,由于量子约束效应、介电效应和表面[5]的影响,微晶的电子和光学性质开始发生变化。对于如此小尺寸的微晶,很大比例的原子在表面上或表面附近。微晶体与周围介质之间巨大界面的存在对微晶体的非线性光学性质有深远的影响。本文首次通过在金属氧化物微晶表面包覆有机极性分子(DBS等),研究了平移金属氧化物微晶的非线性光学性质,发现表面环境的变化会极大地改变其光学性质。以Fe2O3微晶为例,与未包覆Fe2O3微晶相比,Fe2O3微晶(1)向高能侧吸收增加,(2)激光诱导发光强度降低2个数量级,表面拉曼信号增强,(3)饱和吸收现象消失,(4)三阶磁化率增大,激发态弛豫加快。这些现象是量子约束效应和表面效应引起的电子结构变化的结果,不像半导体微晶中离域的万尼尔激子会受到量子约束效应的很大影响(如PbS微晶)。过渡金属氧化物微晶具有更复杂的电子结构,局域化的d电子对其电子学和光学性质影响很大b[6],并且这种材料中小直径的Frenkel激子受量子约束效应的影响很小,因此在吸收光谱中无法观察到激子结构。但过渡金属氧化物微晶的尺寸对其电子结构影响较大。以Fe2O3为例,其能量结构可定量表示为图(文末),其中a为d-d跃迁,b为电荷转移,c为轨道促进,d为带间跃迁。随着微晶尺寸的减小,3d态和4sp态的偶态越来越多,3d-4sp(轨道促进)态的贡献也相应增加。在一定程度上,d电子和Frenkel激子会离域,被激发的电子-空穴对可以迅速电离并散射到表面。特别是当表面涂覆一层有机极性分子时,在表面强极性相互作用下,3d-4sp态相互作用大大增强,并且会存在一些3d-4sp氢化物态,因此d电子和Frenkel激子会变得更加离域,激光诱导的电子-空穴对会非常快地相互散射到表面,从而产生表面离域态。累积和弛豫非常快,电子-电子相干效应[7]大大增强。这种变化不仅增加了非线性响应,而且导致寿命缩短和非辐射过程增强。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Surface Effect On The Nonlinear Optical Properties Of Transition Metal-Oxode Microcrystallites
The size dependent modifications of the optical and electronic properties of microcrystallites have attracted considerable attention recently[1-4]. As the diameter of the microcrystallite approaches its corresponding exciton Bohr diameter, its electronic and optical properties start to change because of the quantum confinement effect, dielectric effect and the effect of the surface[5]. For microcrystallites in such a small size regime, a large percentage of the atomes is on or near the surfaces. The existence of this vast interface between the microcrystallite and the surrounding medium can have a profound effect on the nonlinear optical properties of the microcrystallites. For the first time, we studied the nonlinear optical properties of translation metal-oxide microcrystallites by coating the surface with a layer of organic polar molecule(DBS etc.), and found that the change of the surface environment could alter the optical properties greatly. For Fe2O3 as example, (1) the absorption incresed toward the high energy side, (2) the laser induced luminescence intensity decreased by 2 orders in magnitude, and on the contrary, the Raman signal of the surface was enhanced greatly, (3) the saturable absorption phenomenon disappeared, (4) larger third order susceptibility and faster excited state relaxation were obtained compared with uncoated Fe2O3 microcrystallite. These phenomena are the results of the change of the electronic structure caused by the quantum confinement effect and the effect of the surface, unlike semiconductor microcrystallites in which the delocalized Wannier excitons can be influenced greatly by the quantum confinement effect (such as PbS microcrystallite). Transition metal oxide microcrystallite has more complicated electronic structure in which localized d electrons influence its electronic and optical properties greatly[6], and the small diameter Frenkel exciton in such material was effected little by the quantum confinement effect, therefore, the exciton structure could not be abserved in the absorption spectrum. But the size of the transition metal oxide microcrystallites influence their electronic structure strongly. For Fe2O3 as example, the energy structure can be quantitatively shown as the Figure (at the end of the paper), in which a is d-d transition, b represents charge transfer, c is orbital promotion and d is interband transitions. As the size of the microcrystallite decreases, the 3d and 4sp state couples increasingly, and the 3d-4sp (orbital promotion) state contribution increases correspondingly. To some extend, the d electrons and the Frenkel exciton will be delocalized, and the excited electron-hole pair can be ionized and scattered to the surface rapidly. In particular, when the surface was coated with a layer of organic polar molecule, the 3d-4sp state interaction was enhanced greatly under the strong polar interaction of the surface, and some 3d-4sp hydride state will exist, thus the d electrons and the Frenkel exciton will became more delocalization, and the laser induced electron-hole pairs interect and scatter to the surface very fast, so the surface delocalization state generate, accumulate and relax very rapidly and the electron-electron coherence effect[7] is enhanced greatly. Such changes not only increased the nonlinear response, but also resulted in shorter lifetime and stronger nonraditive process.
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