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Magnetic Polarons in (Zn,Mn)Se/ZnTe and ZnSe/(Zn,Mn)Te quantum dots.

机译:(Zn,Mn)Se / ZnTe和ZnSe /(Zn,Mn)Te量子点中的磁极化子。

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摘要

Quantum dots are highly tunable zero dimensional nanostructures as they give researchers the freedom of artificially controlling their size for a wide variety of applications from opto-electronics to solar cells. In dilute magnetic semiconductor (DMS) quantum dots (QD) the incorporation of magnetic ions leads to exotic magnetic effects. In this thesis, exchange interaction between magnetic ions and charge carriers in both MBE grown and colloidal QDs are explored.;We used continuous wave photoluminescence (cw-PL) and time resolved photoluminescence (TR-PL) spectroscopy to compare the properties of magnetic polarons (MP) in two related spatially indirect II-VI epitaxially grown quantum dot systems. In the ZnTe/(Zn,Mn)Se system the holes are confined in the non-magnetic ZnTe quantum dots (QDs), and the electrons reside in the magnetic (Zn,Mn)Se matrix. On the other hand, in the (Zn,Mn)Te/ZnSe system, the holes are confined in the magnetic (Zn,Mn)Te QDs, while the electrons remain in the surrounding non-magnetic ZnSe matrix. The magnetic polaron formation energies EMP in both systems were measured from the temporal red-shift of the band-edge emission. The magnetic polaron exhibits distinct characteristics depending on the location of the Mn ions.;In the ZnTe/(Zn,Mn)Se system the magnetic polaron shows conventional behavior with decreasing with increasing temperature T and increasing magnetic field B. In contrast, EMP in the (Zn,Mn)Te/ZnSe system has unconventional dependence on temperature T and magnetic field B; EMP is weakly dependent on T as well as on B. We discuss a possible origin for such a striking difference in the MP properties in two closely related QD systems. In the (Zn,Mn)Te/ZnSe QD system, we investigate time evolution of the peak energy of the and circularly-polarized photoluminescence components, and of the circular polarization of the emitted light. We find that this system exhibits unexpected characteristics, such as different time scales for the evolution of the magnetic polaron on one hand and the photoluminescence circular polarization on the other. We discuss these results within the framework of a theoretical model developed to describe the properties of magnetic polarons.;For the colloidal system, carrier spin polarization studies in narrow band gap Mn-doped PbS quantum dots, have been reported. The PbMnS quantum dots were synthesized by hot colloidal solution technique. They were single crystalline with cubic structure. The doping concentration was 3-4% as measured by energy dispersive X-ray spectroscopy. The system was paramagnetic down to 2 K, as measured by VSM. The PL spectra was recorded in the Faraday geometry for magnetic fields of up to 7 tesla in the 0-50 K temperature range. The PL was excited at 1590 meV and the emission was centered at 940 meV with a full width at half maximum of 100 meV. In the presence of magnetic field the emission became strongly sigma+ polarized (P = 35% at 4 tesla), suggesting carrier spin polarization. The polarization was temperature sensitive and decreased sharply with increasing temperature, eventually vanishing at around T = 40 K.
机译:量子点是高度可调谐的零维纳米结构,因为它们使研究人员可以自由控制其大小,以用于从光电到太阳能电池的各种应用。在稀磁半导体(DMS)量子点(QD)中,磁离子的引入会导致奇特的磁效应。本文研究了MBE生长和胶体量子点中磁性离子与载流子之间的交换相互作用。;我们使用连续波光致发光(cw-PL)和时间分辨光致发光(TR-PL)光谱比较了磁极化子的性质。 (MP)在两个相关的空间间接II-VI外延生长的量子点系统中。在ZnTe /(Zn,Mn)Se系统中,空穴被限制在非磁性ZnTe量子点(QDs)中,并且电子驻留在磁性(Zn,Mn)Se基质中。另一方面,在(Zn,Mn)Te / ZnSe系统中,空穴被限制在磁性(Zn,Mn)Te QDs中,而电子保留在周围的非磁性ZnSe基体中。从带边缘发射的时间红移测量了两个系统中的磁极化子形成能EMP。磁极化子表现出独特的特性,具体取决于Mn离子的位置。在ZnTe /(Zn,Mn)Se体系中,磁极化子表现出常规的行为,随温度T的增加和磁场B的增加而降低。 (Zn,Mn)Te / ZnSe体系对温度T和磁场B具有非常规的依赖关系; EMP几乎不依赖于T和B。我们讨论了两个紧密相关的QD系统中MP特性如此显着差异的可能起源。在(Zn,Mn)Te / ZnSe QD系统中,我们研究了圆偏振光和圆偏振光致发光组件的峰值能量以及发射光的圆偏振的时间演化。我们发现该系统展现出出乎意料的特性,例如一方面磁极化子的演化具有不同的时标,另一方面具有光致发光圆极化。我们在描述磁极化子特性的理论模型的框架内讨论了这些结果。对于胶体系统,已经报道了在窄带隙锰掺杂的PbS量子点中的载流子自旋极化研究。通过热胶体溶液技术合成了PbMnS量子点。它们是具有立方结构的单晶。通过能量色散X射线光谱法测得的掺杂浓度为3-4%。根据VSM的测量,该系统是顺磁的,低至2K。在0-50 K温度范围内,法拉第几何的PL光谱记录了高达7特斯拉的磁场。 PL在1590 meV处激发,发射集中在940 meV处,半峰全宽为100 meV。在存在磁场的情况下,发射变为强烈的sigma +极化(在4特斯拉时P = 35%),表明载流子自旋极化。极化是温度敏感的,并且随着温度的升高而急剧下降,最终在T = 40 K时消失。

著录项

  • 作者

    Barman, Biplob.;

  • 作者单位

    State University of New York at Buffalo.;

  • 授予单位 State University of New York at Buffalo.;
  • 学科 Condensed matter physics.;Low temperature physics.
  • 学位 Ph.D.
  • 年度 2015
  • 页码 135 p.
  • 总页数 135
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

  • 入库时间 2022-08-17 11:53:04

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