DLTS Study on Annealed Low-Temperature GaAs Layers with An n-I(LT)-n Structure Grown by MBE

1995 ◽  
Vol 378 ◽  
Author(s):  
Tsai-Cheng Lin ◽  
Hiromasa T Kaibe ◽  
Tsugunori Okumura

AbstractDeep levels in the annealed low-temperature molecular beam epitaxial (LT-MBE) GaAs layer were successfully characterized by using the capacitance deep-level transient spectroscopy (C-DLTS) as well as photocapacitance quenching technique in combination with a unique sample structure. In this work, we have fabricated the samples by inserting the LT-GaAs layer into two n-type semi-conductive layers, like a sandwich (n-LT-n structure), grown at normal substrate temperatures. DLTS measurements have revealed that one electron trap dominates the annealed LT-MBE GaAs. The dominant electron trap was very similar to the so-called EL3 level. Moreover, we found the midgap level appeared upon 800-900°C RTA, although no midgap level was detected in the as-grown n-LT-n sample (annealed at 620°C) and confirmed with photoquenching measurements that it is the EL2 level.

2011 ◽  
Vol 295-297 ◽  
pp. 777-780 ◽  
Author(s):  
M. Ajaz Un Nabi ◽  
M. Imran Arshad ◽  
Adnan Ali ◽  
M. Asghar ◽  
M. A Hasan

In this paper we have investigated the substrate-induced deep level defects in bulk GaN layers grown onp-silicon by molecular beam epitaxy. Representative deep level transient spectroscopy (DLTS) performed on Au-GaN/Si/Al devices displayed only one electron trap E1at 0.23 eV below the conduction band. Owing to out-diffusion mechanism; silicon diffuses into GaN layer from Si substrate maintained at 1050°C, E1level is therefore, attributed to the silicon-related defect. This argument is supported by growth of SiC on Si substrate maintained at 1050°C in MBE chamber using fullerene as a single evaporation source.


1987 ◽  
Vol 92 ◽  
Author(s):  
Akio Kitagawa ◽  
Yutaka Tokuda ◽  
Akira Usami ◽  
Takao Wada ◽  
Hiroyuki kano

ABSTRACTRapid thermal processing (RTP) using halogen lamps for a Si-doped molecular beam epitaxial (MBE) n-GaAs layers was investigated by deep level transient spectroscopy. RTP was performed at 700°C, 800°C and 900°C for 6 s. Two electron traps NI ( Ec-0.5-0.7eV) and EL2 (Ec - 0.82 eV) are produced by RTP at 800 and 900°C.The peculiar spatial variations of the Nl and EL2 concentration across the MBE GaAs films are observed. The larger concentrations of the trap N1 and EL2 are observed near the edge of the samples, and the minima of N1 and EL2 concentration lie between the center and the edge of the sample. It seems that these spatial variations of N1 and EL2 concentration are consistent with that of the thermal stress induced by RTP. Furthermore, the EL2 concentration near the edge of the sample is suppressed by the contact with the GaAs pieces on the edge around the sample during RTP.


1994 ◽  
Vol 33 (Part 2, No. 12A) ◽  
pp. L1651-L1654 ◽  
Author(s):  
Tsai-Cheng Lin ◽  
Hiromasa T. Kaibe ◽  
Tsugunori Okumura

2004 ◽  
Vol 853 ◽  
Author(s):  
D. Koh ◽  
J.-B. Park ◽  
Y. J. Park ◽  
J. I. Lee ◽  
C. Park ◽  
...  

ABSTRACTWe investigated the effects of V/III flux ratios on the Curie temperature, TC, in Ga1−x Mnx As layers with various Mn mole fractions of x = 0.03 and 0.05. A 75 nm thick GaMnAs layer was grown at the temperature of 250 °C with various V/III flux ratios of 25∼34. The low temperature molecular beam epitaxy (LT-MBE) method for growth of GaMnAs layer caused the defects related by excess As and Mn interstitial, and these leaded the formation of deep level. We investigated that formation of deep level was established with various Mn mole fraction for V/III flux ratio 34. The changes of TC are observed by varying V/III flux ratio with a fixed Mn mole fraction. The TC in the sample grown with a lower V/III flux ratio of 25 is found to be higher comparing to that with higher V/III flux ratio of 34 at a fixed high Mn concentration (x = 0.05). Although the Mn concentration increases, the TC is not much changed when the V/III flux ratio is high of 34. The changes of TC with various V/III flux ratios are explained by the existence of low temperature grown defects, which are clarified by the deep level transient spectroscopy measurement. The prime species of defects are found to be AsGa and MnI etc.


1988 ◽  
Vol 126 ◽  
Author(s):  
H. Ueda ◽  
A. Kitagawa ◽  
Y. Tokuda ◽  
A. Usami ◽  
T. Wada ◽  
...  

ABSTRACTUsing deep level transient spectroscopy we have studied the variations of electron traps in molecular beam epitaxial (MBE) AlxGa1−xAs by rapid thermal processing (RTP) using halogen lamps. RTP was performed at 700, 800 and 900 °C for 6s under a SiO2 cap and a capless condition. It is found that during RTP the electron traps with the thermal activation energies of 0.89 and 0.99 eV are produced in Al0.lGa0.9As and Al0.3Ga0.7As, respectively. The thermal activation energies of these traps are close to the reported ones for the trap EL2 in AlxGaM1−xAs. Therefore, these traps are probably related to the trap EL2. In the RTP samples under a capless condition, the concentrations of the trap EL2 in AlxGa1−xAs (x=0.1, 0.3) decreases from the surface to the deeper position in MBE layers, while the depth profile of the trap EL2 in GaAs is flat. It is suggested that the origin of the trap EL2 formation in AlxGa1−xAs is different from one in GaAs.


1989 ◽  
Vol 146 ◽  
Author(s):  
A. Ito ◽  
A. Kitagawa ◽  
Y. Tokuda ◽  
A. Usami ◽  
H. Kano ◽  
...  

ABSTRACTVariations of electron traps in molecular-beam-epitaxial (MBE) GaAs layers grown on Si substrates by rapid thermal processing (RTP) have been investigated with deep level transient spectroscopy (DLTS). RTP was performed at 760 – 910 °C for 9s with Si02 encapsulant. In contrast with the layer on GaAs, the traps AI(Ec – 0.65eV) and A2(Ec – 0.81eV) are observed in the layer on Si. The trap EL2h, one of the EL2 family, is produced by RTP in the layer on Si. Some GaAs surfaces were etched to prove the deeper region. In the surface region, the concentrartion of EL2h is comparable to that of EL2 produced by RTP in the layer on GaAs. On the other hand, in ∿ 1 μm below the surface, the concentration of EL2h is about ten times as large as that of EL2. It is speculated that the stress from the GaAs/Si interface enhances the production of the EL2h concentration. In addition to the EL2, the traps R1(Ec – 0.23 eV), R2(Ec – 0.40 eV), R3(Ec – 0.43eV) and R4(Ec – 0.56 eV) are produced by RTP in the GaAs grown on Si.


2012 ◽  
Vol 1432 ◽  
Author(s):  
Takuma Fuyuki ◽  
Shota Kashiyama ◽  
Kunishige Oe ◽  
Masahiro Yoshimoto

ABSTRACTDeep-level densities of p-GaAs1−xBix and at the GaAs/p-GaAs1−xBix heterointerface have been shown to be sufficiently low for device applications based on the results of deep-level transient spectroscopy, isothermal capacitance transient spectroscopy and admittance spectroscopy. Although the metastable alloy of GaAs1−xBix is grown by molecular beam epitaxy at low temperature (370 °C), the deep-level density of p-GaAs1−xBix is suppressed such that it is on the order of 1015 cm−3. The state density at the heterointerface was determined to be 8 · 1011 cm−2eV−1, which is comparable to other III–V heterointerfaces formed at high temperatures. The surfactant-like effect of Bi is believed to prevent defect formation during low-temperature growth.


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