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OPTICAL PROPERTIES OF CVD GROWN DILUTED Ⅱ-Ⅵ MAGNETIC SEMICONDUCTOR NANOSTRUCTURES

机译:化学气相沉积生长的Ⅱ-Ⅵ型磁性半导体纳米结构的光学性质

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Optical properties of diluted magnetic semiconductor (DMS) are not well understood so far, especially relationship to their ferromagnetism. Here we prepared Mn ion doped ZnO, CdS and ZnSe nanostructures by CVD method, studied their optical properties via microphotoluminescence techniques, found many very interesting properties, which are all related to the exciton magnetic polaron (EMP), itinerant or partially itinerant, their energy levels are agree well with the AB initio calculations. In ZnO:Mn nanowires, the EMP can show up with free exciton together for very diluted doping(<0.001%), this EMP can form condensate to produce single mode lasing line at fs pulse excitation along with the disappearing of free excitons. With a little bit large amount of Mn doping, the nanowire show EMP lasing mode with background at fs laser pulse excitation, but at even high power, some electron-hole plasma induced lasing modes could be observed due to the carrier effect. The time-delay photoluminescence by ns laser pulse are also studied, only free EMP and localized EMP(d-d transition) show up in the emission spectra, we gave the clear assignments for all the d-d transitions of Mn in ZnO, which have been argued for a long time. It is more interesting that these d-d transitions exhibit clear enhanced coherent relaxation behaviors with increasing excitation power, like that by free excitons, behave a collective spin-dependent coherent radiation. We also observed the Mn-O-Mn cluster peak in the long wavelength range, which may be related to the ferromagnetic properties. In CdS:Mn nanowires, we found many peaks above the single Mn ion emission band (575nm) when increasing the Mn concentration, we used a simple Hydrogen-like cloud theoretical model to describe them well, in this model, the Mn-S-Mn- cluster with variable Mn ion number and their ferromagnetic coupling are considered. The SQUID detection proved its ferromagnetic behavior, and MFM result indicated its cluster nature in nanobelt. Ab initio calculation results also support our cluster assignments. In ZnSe:Mn nanobelt, doping often produce many optical domains which can works as optical cavities to produce cavity modes in a wide spectral range, this can be easily observed in the CW laser excitation. If we turn to the ns laser, we can detect bandedge emission at low power, but they goes to stimulated emission by EMP at high power excitation. This stimulated emission is usually limited by the magnitude of optical domain size. All above experimental results indicate that the d-d transition is not absolutely localized within Mn ion, it is excited by light to become localized EMP. The Mn-O(or S)-Mn aggregate can be detected by the microphotoluminescence technique with their emission and ferromagnetism, this may be used to study more DMS substances with wide band. These findings facilitate to get better understanding of DMS ferromagnetism and find novel applications in booptics and magnetics.
机译:到目前为止,对稀磁半导体(DMS)的光学特性还没有很好的了解,尤其是与它们的铁磁性的关系。在这里,我们通过CVD方法制备了掺杂Mn离子的ZnO,CdS和ZnSe纳米结构,通过微光致发光技术研究了它们的光学性质,发现了许多非常有趣的性质,这些性质与激子磁极化子(EMP),流动性或部分流动性,它们的能量有关。的水平与AB初始计算非常吻合。在ZnO:Mn纳米线中,EMP可以与自由激子一起出现,以进行非常稀释的掺杂(<0.001%),该EMP可以在fs脉冲激发下形成凝结产生单模激射线,同时自由激子消失。在少量的Mn掺杂下,纳米线在fs激光脉冲激发下显示出具有背景的EMP激光模式,但是即使在高功率下,由于载流子效应,也可以观察到一些电子空穴等离子体诱导的激光模式。还研究了ns激光脉冲的时延光致发光,在发射光谱中仅显示了自由EMP和局部EMP(dd跃迁),我们对ZnO中Mn的所有dd跃迁给出了明确的分配,这被认为是很长时间。有趣的是,这些d-d跃迁表现出明显的增强的相干弛豫行为,其激发功率增加,就像自由激子所表现出的那样,表现出集体自旋相关的相干辐射。我们还观察到了长波长范围内的Mn-O-Mn团簇峰,这可能与铁磁性能有关。在CdS:Mn纳米线中,当增加Mn浓度时,我们在单个Mn离子发射带(575nm)上方发现了许多峰,我们使用简单的类似于氢的云理论模型对其进行了很好的描述,在该模型中,Mn-S-考虑了具有可变Mn离子数的Mn团簇及其铁磁耦合。 SQUID检测证明了其铁磁行为,MFM结果表明其在纳米带中具有簇性质。从头算计算结果也支持我们的集群分配。在ZnSe:Mn纳米带中,掺杂通常会产生许多光畴,这些光畴可以用作光腔以在宽光谱范围内产生腔模,这在连续波激光激发中很容易观察到。如果我们转向ns激光器,我们可以在低功率下检测到带边发射,但是在高功率激发下,它们会被EMP激发。这种受激发射通常受光学域大小的大小限制。所有上述实验结果表明,d-d跃迁不是绝对地位于Mn离子内,它被光激发成为局部的EMP。 Mn-O(或S)-Mn聚集体可以通过微光致发光技术检测其发射和铁磁性,可用于研究更多具有宽带的DMS物质。这些发现有助于更好地了解DMS铁磁性,并在光学和磁性方面找到新的应用。

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