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1.
利用固态源分子束外延技术,按S-K模式生长出五层堆垛InAs/GaAs量子点(QD)微结构材料.用这种QD材料制成的激光器,内光学损耗为2.1cm-1,透明电流密度为15士10 A/cm2.对于条宽100μm,腔长2.4mm的激光器(腔面未经镀膜处理),室温下基态激射的波长为1.08μm,阈值电流密度为144A/cm2,连续波光功率输出达2.67W(双面),外量子效率为63%,特征温度为320K.研究了QD激光器翟激射特性,并对结果作了讨论.  相似文献   

2.
利用固态源分子束外延技术,按S-K模式生长出五层堆垛InAs/GaAs量子点(QD)微结构材料.用这种QD材料制成的激光器,内光学损耗为2.1cm-1,透明电流密度为15士10 A/cm2.对于条宽100μm,腔长2.4mm的激光器(腔面未经镀膜处理),室温下基态激射的波长为1.08μm,阈值电流密度为144A/cm2,连续波光功率输出达2.67W(双面),外量子效率为63%,特征温度为320K.研究了QD激光器翟激射特性,并对结果作了讨论.  相似文献   

3.
利用分子束外延技术和 S- K生长模式 ,系统研究了 In As/Ga As材料体系应变自组装量子点的形成和演化 .研制出激射波长λ≈ 960 nm,条宽 1 0 0μm,腔长 80 0μm的 In( Ga) As/Ga As量子点激光器 :室温连续输出功率大于 3.5W,室温阈值电流密度 2 1 8A/cm2 ,0 .61 W室温连续工作寿命超过 3760小时  相似文献   

4.
利用分子束外延技术和S-K生长模式,系统研究了InAs/GaAs材料体系应变自组装量子点的形成和演化.研制出激射波长λ≈960nm,条宽100μm,腔长800μm的In(Ga)As/GaAs量子点激光器:室温连续输出功率大于3.5W,室温阈值电流密度218A/cm2,0.61W室温连续工作寿命超过3760小时.  相似文献   

5.
报道了激射波长为5.4和7.84μm的应变补偿In1-xGaxAs/In1-yAlyAs量子级联激光器的单模激射.以高质量的应变补偿量子级联激光器材料为支撑,通过减小FP腔长,开辟实现单模器件的新途径.首次实现阈值电流仅为50mA、腔长为145μm的激射波长在λ≈5.4μm的单模激射和阈值电流仅为80mA、腔长为170μm的激射波长在λ≈7.84μm的单模激射.这是目前InGaAs/InAlAs材料体系最短腔长的边发射量子级联激光器.  相似文献   

6.
报道了激射波长为5.4和7.84μm的应变补偿In1-xGaxAs/In1-yAlyAs量子级联激光器的单模激射.以高质量的应变补偿量子级联激光器材料为支撑,通过减小FP腔长,开辟实现单模器件的新途径.首次实现阈值电流仅为50mA、腔长为145μm的激射波长在λ≈5.4μm的单模激射和阈值电流仅为80mA、腔长为170μm的激射波长在λ≈7.84μm的单模激射.这是目前InGaAs/InAlAs材料体系最短腔长的边发射量子级联激光器.  相似文献   

7.
研究了原位和非原位退火对分子束外延生长的GaInNAsSb/GaNAs/GaAs量子阱激光器的作用.通过快速热退火量子阱质量得到很大提高,这一方法还很少被应用于激光器的制作,特别是波长在1.55μm波段的激光器.生长量子阱时采用的生长速率、Sb诱导等,将量子阱激光器发光波长拓展到1.59μm,并制作了脊型波导FP腔GaInNAsSb单阱激光器,成功实现了室温连续激射,激射波长达到1.59μm,阈值电流为2.6kA/cm2.  相似文献   

8.
研究了原位和非原位退火对分子束外延生长的GaInNAsSb/GaNAs/GaAs量子阱激光器的作用.通过快速热退火量子阱质量得到很大提高,这一方法还很少被应用于激光器的制作,特别是波长在1.55μm波段的激光器.生长量子阱时采用的生长速率、Sb诱导等,将量子阱激光器发光波长拓展到1.59μm,并制作了脊型波导FP腔GaInNAsSb单阱激光器,成功实现了室温连续激射,激射波长达到1.59μm,阈值电流为2.6kA/cm2.  相似文献   

9.
报道了中国第一只1.30μm单量子阱边发射激光器的材料生长、器件制备及特性测试.通过优化分子束外延生长参数,调节In和N组分含量使GaInNAs量子阱的发光波长覆盖1.3μm范围.脊形波导条形结构单量子阱边发射激光器,实现了室温连续激射,激射波长为1.30μm,阈值电流密度为1kA/cm2,输出功率为30mW.  相似文献   

10.
报道了 GSMBE方法生长波长 1.84μm的 In Ga As/ In Ga As P/ In P应变量子阱激光器 . 40 μm条宽、 80 0 μm腔长的平面电极条形结构器件 ,室温下以脉冲方式激射 ,2 0℃下阈值电流密度为 3.8k A/ cm2 ,外微分量子效率为9.3%  相似文献   

11.
SnS quantum dots (QDs) with size of 8 nm were synthesized by an in-situ room temperature solution chemical reaction process. Stannous chloride, as Sn precursor, was coated on the TiO2 photo-anodes to form a solid precursor film. Ammonium sulfide was dissolved into ethanol to form anionic reaction solution. SnS quantum dots were generated by immersing the Sn-coated TiO2 photo-anodes into the anionic solution. The structure, morphology and optical absorption properties of the SnS/TiO2 photoanodes were investigated by means of XRD, SEM, TEM and UV–vis measurements. The photovoltaic properties of the SnS QDs sensitized TiO2 solar cells were optimized by changing the number of deposition cycles of the SnS QDs. It turns out that the SnS/TiO2 solar cell with 20 deposition cycles exhibited the best photovoltaic performance with an open-circuit voltage Voc of 510 mV, a short-circuit current density Jsc of 2.41 mA, a fill factor FF of 0.49 and a power conversion efficiency η of 0.61% under AM 1.5 illumination. This result is interpreted in terms of minimization of the charge transfer resistance. The performance will drop for further deposition because the charge transfer resistance will increase due to QDs agglomeration.  相似文献   

12.
量子点(quantum dots,QDs),也被称为半导体纳米晶体,得益于其廉价的制造成本和独特的光学物理学特性,已经广泛应用于光电探测器和太阳能电池的设计和开发.而量子点的合成则是制备光电探测器和太阳能电池的重要组成部分之一.本文对几种不同的量子点合成技术进行了概述,对国内外不同的基于量子点的光电探测器和太阳能电池进...  相似文献   

13.
应变自组装InAlAs量子点材料和红光量子点激光器   总被引:1,自引:0,他引:1  
通过提高量子点材料的质量和优化量子点激光器材料的结构 ,研制出高质量的应变自组装 In Al As/Al Ga As/Ga As量子点材料和低温连续激射的红光量子点激光器。器件性能达到国际同类研究的最好水平  相似文献   

14.
对单光子波包与腔-量子点模型相互作用的动力学过程进行了数学推导,并通过数值模拟实现了静态量子比特与飞行光子比特之间的相互转换。结果表明:由腔-量子点系统输出到光纤的光子是一个平滑的波包;通过改变激光脉冲作用时间等系统参数,可实现量子点中的原子和光子的纠缠,在此基础上,即可实现不同量子点中原子的纠缠。研究结果对解决利用腔-量子点系统来构造量子计算机的接口、制备纠缠态以及实现受控量子门等热点问题具有积极意义。  相似文献   

15.
Raman scattering measurements were carried out in a self-organized multi-layered Ge quantum dot sample, which was grown using solid-source molecular-beam epitaxy, and consisted of 25 periods of 20-Å-high Ge quantum dots sandwiched by 20-nm Si spacers. The Ge-Ge optical phonon mode was found at 298.2 cm?1, which was tuned by the phonon confinement and strain effects. Acoustic phonons related to Ge quantum dots have also been demonstrated.  相似文献   

16.
We present a quantum dot structure fabricated by the lithographic positioning, which can be used as a prototype of the quantum dot register for quantum computing. Using simple model calculations we show that parameters of our quantum dot structure are very close to the ones required for two possible embodiments of a quantum computer. Results of numerical simulation of the quantum dot register, as well as discussion of materials and technological issues of fabrication of quantum logic gates are also presented.  相似文献   

17.
Binary CdS and ZnS and ternary CdZnS alloy quantum dots (QDs) were synthesized via a simple, inexpensive, and reproducible route using sulfur, cadmium stearate, and zinc stearate as precursors and N-oleoylmorpholine as the reaction medium and solvent. Both binary and ternary QDs exhibited a narrow size distribution and high crystallinity as confirmed TEM and HRTEM images. The alloy QDs exhibited excellent composition-dependent optical properties and a narrow full-width at half maximum of 19–21 nm. UV-visible absorbance and photoluminescence (PL) emission spectra of the CdZnS QDs showed a blue shift during growth, indicating the formation of alloy QDs. ZnS shells were successively coated onto the alloy core via decomposition of zinc diethyldithiocarbamate at a relatively low temperature. The CdZnS/ZnS core/shell QDs obtained showed a significant increase in size and exhibited strong band edge emission with a significant increase in PL quantum yield. XRD patterns revealed that all the QDs had a zinc blende structure. The QD diffraction peaks gradually shifted to higher angle in the order CdS < CdZnS < CdZnS/ZnS < ZnS. The mechanism for the synthesis of CdZnS alloy and CdZnS/ZnS core/shell QDs is discussed.  相似文献   

18.
在InAs自组织量子点的GaAs覆盖层中引入生长停顿,将这种量子点结构作激光器的有源区,与不引入生长停顿的量子点激光器进行对比后发现:生长停顿可以降低激光器的阈值电流,提高其特征温度,改善激光波长的温度稳定性。简单的分析表明,量子点中的能带填充效应影响了激光波长的温度特性。  相似文献   

19.
用MOCVD技术在偏(1100)GaAs衬底上生长了发光波长在1.3μm的线状空间规则排列InAs量子点.光致发光实验表明,相对于正(100)衬底,偏(100)GaAs衬底上生长的InAs量子点具有更好的材料质量,光谱有更大的强度和更窄的线宽.为了得到发光波长为1.3μm的量子点,对比研究了不同In含量的InGaAs应力缓冲层(SBL)和应力盖层(SCL)的应力缓冲作用.结果表明,增加SCL中In含量能有效延伸量子点发光波长到1. 3μm,但是随着SBL中In的增加,发光波长变化不明显,并且材料质量明显下降.  相似文献   

20.
The conditions under which the band gaps of free standing and embedded semiconductor quantum dots are direct or indirect are discussed. Semiconductor quantum dots are classified into three categories; (i) free standing dots, (ii) dots embedded in a direct gap matrix, and (iii) dots embedded in an indirect gap matrix. For each category, qualitative predictions are first discussed, followed by the results of both recent experiments and state of the art pseudopotential calculations. We show that:
–  Free standing dots of InP, InAs, and CdSe will remain direct for all sizes, while dots made of GaAs and InSb will turn indirect below a critical size.
–  Dots embedded within a direct gap matrix material will either stay direct (InAs/GaAs at zero pressure) or will become indirect at a critical size (InSb/InP).
–  Dots embedded within an indirect gap matrix material will exhibit a transition to indirect gap for sufficiently small dots (GaAs/AlAs and InP/GaP quantum well) or will be always indirect (InP/GaP dots, InAs/GaAs above 43 k bar pressure and GeSi/Si dots).
In indirect nanostructures, charge separation can occur with electrons and holes localized on different materials (flat InP/GaP quantum well) or with electrons and holes localized in different layers of the same material (concentric cylindrical GaAs/AlAs layers).  相似文献   

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