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Coupled quantum well to quantum dot heterostructure laser.

机译:将量子阱耦合到量子点异质结构激光器。

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摘要

Quantum-dot (QD) active layers have received much attention because of the possibility of changing the step-density of states of a quantum well (QW, thin layer Lz 500 Å) to the discrete states of a QD (small “box” Lx, Ly, Lz 500 Å), potentially leading to an ultimate form of laser. However, significant inferior properties relative to the QW, such as carrier collection and redistribution properties, assure that the QW cannot be completely displaced by the QD. A new heterostructure system that combines the comparative advantages of the QW and the QD is proposed leading to the development of the coupled QW to QD heterostructure laser.; Data are presented demonstrating continuous 300-K photopumped InP quantum dot (QD) laser operation (656–679 nm) realized by coupling, via tunneling, an auxiliary InGaP QW to the QDs of an InP-In(AlGa)P-InAlP heterostructure.; Data are presented showing that a QD+QW laser diode has a steeper I-V characteristic than does a similar diode with no auxiliary QW. The InP+InGaP QD+QW diode is capable of 300-K visible-spectrum QD laser operation, while the single-layer InP QD diode (single QD layer) saturates at low current ( 1 mA) and does not exhibit stimulated emission.; Data are presented demonstrating the cw 300-K visible spectrum (654 nm) laser operation of a single 7.5 ML InP QD layer coupled by a 20-Å In 0.5Al0.3Ga0.2P barrier to an auxiliary 70-Å In0.5Ga0.5P QW. The simple stripe-geometry (530 μm × 10 μm) InP QD + InGaP QW heterostructure laser, enhanced by the QW and operating on an upper QD state (42% quantum efficiency), is capable of over 10-mW/facet cw 300-K operation in spite of the weak heat sinking of probe operation.; Data are presented demonstrating the cw 300-K visible spectrum of a 642-nm, 646-nm and 654-nm QD+QW laser. Data indicate that stronger coupling between QW and QD layers results in better (weaker) wavelength shift versus temperature characteristics (Δλ/ΔT ∼ 0.13nm/°C for strong coupling and ∼0.19nm/°C for weak coupling).; Data are presented showing that the gain of a QD laser is improved by strong resonance-enhanced coupling of QD states to MQW states for pulsed laser operation between λ = 607 and 619.7 nm.; Despite the use of tensile strained MQWs (strong TM radiation recombination), pulsed laser operation with TE polarization is observed.; Data (infrared wavelengths) are presented showing that it is advantageous to locate strain-matching auxiliary InGaAs layers QWs within tunneling distance of a single QD layer of an AlGaAs-GaAs-InGaAs-InAs QD heterostructure laser to realize also smaller size QDs of greater density and uniformity. (Abstract shortened by UMI.)
机译:量子点(QD)有源层备受关注,因为它有可能改变量子阱状态的阶跃密度(QW,薄层L z ≲ 500Å)到QD的离散状态(小“盒子” L x ,L y ,L z ≲ 500Å),有可能导致最终的激光形式。但是,相对于QW而言,明显的劣等属性(例如载流子收集和重新分配属性)确保了QW无法完全被QD取代。提出了一种结合QW和QD的比较优势的新型异质结构系统,从而导致了QW与QD耦合异质结构激光器的发展。呈现的数据演示了通过隧道将辅助InGaP QW耦合到InP-In(AlGa)P-InAlP异质结构的QD来实现的连续300-K光泵浦InP量子点(QD)激光操作(656-679 nm)。 ;呈现的数据表明,与没有辅助QW的类似二极管相比,QD + QW激光二极管具有更陡的I-V特性。 InP + InGaP QD + QW二极管能够进行300-K可见光QD激光操作,而单层InP QD二极管(单QD层)在低电流( ≲ 1 mA),并且不显示受激发射。呈现的数据表明了单个7.5 ML InP QD层与20-ÅIn 0.5 Al 0.3 Ga耦合的cw 300-K可见光谱(654 nm)激光操作辅助70-ÅIn 0.5 Ga 0.5 P QW的 0.2 P势垒。简单的条纹几何形状(530μm×10μm)InP QD + InGaP QW异质结构激光器,通过QW增强并在较高的QD状态下工作(量子效率为42%),其单面连续光功率可超过10mW 300-尽管探针运行散热能力较弱,但仍为K运行。呈现的数据表明了642nm,646nm和654nm QD + QW激光器的cw 300-K可见光谱。数据表明,QW和QD层之间更强的耦合导致相对于温度特性的更好(更弱)的波长偏移(强耦合为Δλ/ΔT〜0.13nm /°C,弱耦合为〜0.19nm /°C)。数据表明,对于在λ= 607和619.7 nm之间的脉冲激光操作,QD状态与MQW状态之间的强共振增强耦合提高了QD激光器的增益。尽管使用了拉伸应变的MQW(强TM辐射复合),但观察到具有TE偏振的脉冲激光操作。呈现的数据(红外波长)表明,将应变匹配辅助InGaAs层QW放置在AlGaAs-GaAs-InGaAs-InAs QD异质结构激光器的单个QD层的隧穿距离内是有利的,从而也可以实现更大密度的更小尺寸的QD和均匀性。 (摘要由UMI缩短。)

著录项

  • 作者

    Walter, Gabriel.;

  • 作者单位

    University of Illinois at Urbana-Champaign.;

  • 授予单位 University of Illinois at Urbana-Champaign.;
  • 学科 Engineering Electronics and Electrical.
  • 学位 Ph.D.
  • 年度 2003
  • 页码 p.3980
  • 总页数 109
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 无线电电子学、电信技术;
  • 关键词

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