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EXCITONIC STATES AND THE INFLUENCE OF THE EXCHANGE INTERACTION IN THE SEMIMAGNETIC SEMICONDUCTOR CADMIUM(1-X) MANGANESE(X) SELENIUM.

机译:电磁态镉(1-X)锰(X)硒的激发态和交换相互作用的影响。

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摘要

The results of a photoluminescence spectroscopy study of the properties of excitonic states under the influence of the exchange interaction with the Mn('++)-ion spins in the semimagnetic semiconductor Cd(,l-x)Mn(,x)Se are presented. It is found that, in the absence of an external magnetic field, the donor-bound exciton energy shows unusual dependences on temperature and Mn composition. This is interpreted to be a consequence of a local magnetization of the Mn('++)-ion spins within the bound exciton volume. The finite size magnetization effect on the bound exciton energy is qualitatively explained if both the thermodynamic fluctuations of the Mn('++)-ion spin cloud and the influence of the localized carriers on the spin state of the Mn('++)-ions are considered. The latter results in the formation of a bound magnetic polaron for x = .10 Mn concentration (the highest studied) at T < 10 K. With increasing temperature, a transition from a magnetic polaron regime to a fluctuation dominated regime is observed for this composition.; The possibility of a long-range, magnetically ordered state in Cd(,l-x)Mn(,x)Se at low temperatures (T = 1.8 K), induced by the exchange interaction between the Mn('++)-ion spins and a dense electron-hole plasma generated by intense optical excitation has also been investigated. The observed luminescence spectra yield information about the temporal evolution of inelastic scattering processes in a dense exciton gas, with a likely contribution by an electron-hole plasma. The short carrier lifetimes measured, less than 100 psec for x = .10, together with possible plasma expansion may prevent the realization of a spin ordered state under our experimental conditions.
机译:提出了在半磁性半导体Cd(,l-x)Mn(,x)Se中与Mn('++)离子自旋发生交换相互作用影响下激子态性质的光致发光光谱研究结果。已经发现,在没有外部磁场的情况下,施主结合的激子能量显示出对温度和Mn组成的异常依赖性。这被解释为是在受激激子体积内Mn('++)离子自旋局部磁化的结果。如果Mn('++)-离子自旋云的热力学涨落和局部载流子对Mn('++)-自旋态的影响都定性地解释了有限大小的磁化对束缚激子能量的影响。考虑离子。后者导致在T <10 K时形成x = .10 Mn浓度的结合的磁极化子(研究的最高值)。随着温度的升高,观察到该成分从磁极化子态过渡到波动为主的态。; Mn('++)-离子自旋与金属间的交换相互作用引起的低温(T = 1.8 K)下Cd(,lx​​)Mn(,x)Se处于长距离,有序磁化状态的可能性还研究了由强光激发产生的致密电子空穴等离子体。观察到的发光光谱可得出有关稠密激子气体中非弹性散射过程随时间演变的信息,其中电子空穴等离子体可能会做出贡献。在我们的实验条件下,测得的短载流子寿命(对于x = .10小于100 psec)以及可能的等离子体膨胀可能会阻止自旋有序状态的实现。

著录项

  • 作者

    HUBER, CARMEN ISABEL A.;

  • 作者单位

    Brown University.;

  • 授予单位 Brown University.;
  • 学科 Physics Condensed Matter.
  • 学位 Ph.D.
  • 年度 1984
  • 页码 129 p.
  • 总页数 129
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 O49;
  • 关键词

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