69 resultados para DLTS


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应用深能级瞬态谱(DLTS)技术详细研究低压-金属有机物汽相外延(LP-MOVPE)生长的Ga_(0.74)In_(0.53)As/InP量子阱、宽接触和质子轰击条形异质结激光器中的深能级。样品的DLTS表明,在宽接触激光器的i-Ga_(0.47)In(0.53)As有源层里观察到 H1(Ev+0.09eV)和E1(E_c-0.35eV)陷阱,它们可能分别与样品生长过程中扩散到i-Ga_(0.47)In_(0.53)As有源层的Zn和材料本身的原生缺陷有关。而条形激光器的i-Ga_(0.47)In_(0.53)A_s有源层的 H_2(E_v+0.11eV)和 E_2(E_q-0.42eV)陷阱则可能是H1和E1与质子轰击引起的损伤相互作用的产物 。

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利用扩展电阻探针(SRP)和深能级瞬态谱(DLTS)技术详细研究了直接键合的n-si/n~+-si界面附近的深能级.实验结果表明,在直接键合的n-Si/n~+-si一侧附近可观察到一个明显的电子陷阱E1(E_c-0.39eV),E1可能是由若干个能级位置相近的陷阱迭加而成的,其浓度在10~(13)-10~(14)cm~(-3)之间.它可能是与制备键合材料的高温(1000-1100℃)处理过中程产生的空位和热应力有关。

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用深能级瞬态谱(DLTS)系统地研究了GaAs(50A)/GaAlAs(50A)超晶格中的电子辐照缺陷,证实其亚稳态特性的存在,对其恢复温度、转变条件进行了研究,指出在体材料中不能观察到电子辐照缺陷亚稳态的原因。

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利用深能级瞬态谱(DLTS), 详细研究了(Pt及其硅化物)/Si界面上存在的各种深能级缺陷中心,并分析了引起这些缺陷的原因及与界面原子结构的关系。

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Deep defects in annealed InP have been investigated by deep level transient capacitance spectroscopy (DLTS), photo induced current transient spectroscopy (PICTS) and thermally stimulated current spectroscopy (TSC). Both DLTS results of annealed semiconducting InP and PICTS and TSC results of annealed semi-insulating InP indicate that InP annealed in phosphorus ambient has five defects, while lid? annealed in iron phospbide ambient has two defects. Such a defect formation phenomenon is explained in terms of defect suppression by the iron atom diffusion process. The correlation of the defects and the nature of the defects in annealed InP are discussed based on the results.

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Deep level transient spectroscopy (DLTS) technique was used to investigate deep electron states in n-type Al-doped ZnS1-xTex epilayers grown by molecular fiction epitaxy (MBE), Deep level transient Fourier spectroscopy (DLTFS) spectra of the Al-doped ZnS1-xTex (x = 0. 0.017, 0.04 and 0.046. respectively) epilayers reveal that At doping leads to the formation of two electron traps at 0.21 and 0.39 eV below the conduction hand. 1)DLTFS results suggest that in addition to the rules of Te as a component of [lie alloy as well as isoelectronic centers, Te is also involved in the formation of all electron trip, whose energy level relative to the conduction hand decreases a, Te composition increases.

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Confirmation of quantum dot lasing have been given by photoluminescence and electro-luminescence spectra. Energy levels of QD laser are distinctively resolved due to band filling effect, and the lasing energy of quantum dot laser is much lower than quantum well laser. The energy barrier at InAs/GaAs interface due to the built-in strain in self-organized system has been determined experimentally by deep level transient spectroscopy (DLTS). Such barrier has been predicted by previous theories and can be explained by the apexes appeared in the interface between InAs and GaAs caused by strain.

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Deep-level transient spectroscopy and photoluminescence studies have been carried out on structures containing self-assembled InAs quantum dots formed in GaAs matrices. The use of n- and p-type GaAs matrices allows us to study separately electron and hole levels in the quantum dots by the deep-level transient spectroscopy technique. From analysis of deep-level transient spectroscopy measurements it follows that the quantum dots have electron levels 130 meV below the bottom of the GaAs conduction band and heavy-hole levels at 90 meV above the top of the GaAs valence band. Combining with the photoluminescence results, the band structures of InAs and GaAs have been determined. (C) 2000 Elsevier Science B.V. All rights reserved.

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Deep Level Transient Spectroscopy (DLTS) has been applied to investigate the electronic properties of self-organized InAs quantum dots. The energies of electronic ground states of 2.5ML and 1.7ML InAs quantum dots (QDs) with respect to the conduction band of bulk GaAs are about 0.21 eV and 0.09 eV, respectively. We have found that QDs capture electrons by lattice relaxation through a multi-phonon emission process. The samples are QDs embedded in superlattices with or without a 500 Angstrom GaAs spacing layer between every ten periods of a couple of GaAs and InAs layers. The result shows that the density of dislocations in the samples with spacer layers is much lower than in the samples without the spacer layers.