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作 者:孙萍[1] 王引书[1] 王若桢[1] 林永昌[2]
机构地区:[1]北京师范大学物理系,北京100088 [2]北京理工大学光电工程系,北京100081
出 处:《量子电子学报》2002年第1期70-73,共4页Chinese Journal of Quantum Electronics
基 金:国家自然科学基金资助项目(29890217)
摘 要:对嵌埋于玻璃基体中的CdS0.1Sc0.9纳米晶体进行了室温电调制透射谱测量,观察到较强的共振和非共振电光响应倚号(10-4~10-3).共振电光响应具有如下特征:同一组分的纳米晶体其倩号的峰位随着尺寸减小向高能方向移动;同一样品谱线形状不随外电场强度而变;信号幅度与外电场强度的平方成线性关系,并且随调制频率的增加而减小;共振电光效应的物理机制是量子受限的Stark效应.非共振电光响应信号呈与波长有关的振荡线形;外电场强度增加,非共振电光响应信号幅度也增加;用介电受限的局域场增强理论解释了非共振电光效应的物理机制.Electromodulation transmittance spectroscopy of CdS0.1Se0.9 nanocrystals embeded in the glass matrix is measured at room-temperature. Stronger electro-optical signals (10-4 - 10-3) are observed in both resonant and nonresonant regimes. These are some experimental results in resonant regime. The peak positions of electro-optical signals shift to higher energy direction when the nanocrystal size decreases; the line-shape of spectra for the same sample is independent of the external electric field strength; there are linear relationship between the signal magnitudes scale and the square of applied field strength, which indicates that the electro-optical effect of nanocrystals is the Kerr effect and the nanocrystals have the third-order nonlinear optical sus- ceptibility X(3); the signal magnitudes decrease when the modulation frequencies increase. The physical mechanism of resonant electro-optical effect is consistent with quantum-confined Stark effect. The oscillatory electro-optical signals in nonresonant regime are observed at frequency of 230 Hz. The magnitudes of nonresonant electro-optical signal tend to enhance with the in- creasing of the external electric field strength. The origin of nonresonant electro-optical effect is described with' dielectric confinement' effect.
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