Recovery Effect of Deep Level Luminescence Induced by Below Band-Gap Excitation in GaAs

1985 ◽  
Vol 24 (Part 2, No. 1) ◽  
pp. L47-L49 ◽  
Author(s):  
Michio Tajima
Keyword(s):  
Band Gap ◽  
1995 ◽  
Vol 395 ◽  
Author(s):  
U. Rossner ◽  
J.-L. Rouviere ◽  
A. Bourret ◽  
A. Barski

ABSTRACTElectron Cyclotron Resonance Plasma Assisted Molecular Beam Epitaxy (ECR-MBE) and Gas Source Molecular Beam Epitaxy (GSMBE) have been used to grow hexagonal GaN on Si (111). In the ECR-MBE configuration high purity nitrogen has been used as nitrogen source. In GSMBE ammonia was supplied directly to the substrate to be thermally cracked in the presence of gallium.By a combined application of in-situ reflection high-energy electron-diffraction (RHEED) and cross-sectional transmission electron microscopy (TEM) the growth mode and structure of GaN were determined. The growth mode strongly depends on growth conditions. Quasi two dimensional growth was observed in ECR-MBE configuration for a substrate temperature of 640°C while three dimensional growth occured in GSMBE configuration in the temperature range from 640 to 800°C.Low temperature (9 K) photoluminescence spectra show that for samples grown by ECR-MBE and GSMBE a strong near band gap emission peak dominates while transitions due to deep level states are hardly detectable. The best optical results (the highest near band gap emission peak intensity) have been observed for samples grown by GSMBE at high temperature (800°C). This could be explained by the increase of grain dimensions (up to 0,3 – 0,5 μm) observed in samples grown by GSMBE at 800°C.


2005 ◽  
Vol 97 (8) ◽  
pp. 083529 ◽  
Author(s):  
A. Armstrong ◽  
A. R. Arehart ◽  
S. A. Ringel

1989 ◽  
Vol 163 ◽  
Author(s):  
John D. Dow ◽  
Shang Yuan Ren ◽  
Jun Shen ◽  
Min-Hsiung Tsai

AbstractThe physics of deep levels in semiconductors is reviewed, with emphasis on the fact that all substitutional impurities produce deep levels - some of which may not lie within the fundamental band gap. The character of a dopant changes when one of the deep levels moves into or out of the fundamental gap in response to a perturbation such as pressure or change of host composition. For example, Si on a Ga site in GaAs is a shallow donor, but becomes a deep trap for x>0.3 in AℓxGa1-xAs. Such shallow-deep transitions can be induced in superlattices by changing the period-widths and quantum confinement. A good rule of thumb for deep levels in superlattices is that the energy levels with respect to vacuum are relatively insensitive (on a >0.1 eV scale) to superlattice period-widths, but that the band edges of the superlattices are sensitive to changes of period. Hence the deep level positions relative to the band edges are sensitive to the period-widths, and shallow-deep transitions can be induced by band-gap engineering the superlattice periods.


Coatings ◽  
2020 ◽  
Vol 10 (3) ◽  
pp. 206
Author(s):  
Jinhee Park ◽  
You Seung Rim ◽  
Pradeep Senanayake ◽  
Jiechen Wu ◽  
Dwight Streit

The characterization of defect states in a hydrothermally grown single crystal of ZnO was performed using deep-level transient spectroscopy in the temperature range of 77–340 K. The native intrinsic defect energy level within the ZnO band gap occurred in the depletion region of ZnO Schottky barrier diodes. A major defect level was observed, with a thermal activation energy of 0.27 eV (E3) within the defect state distribution from 0.1 to 0.57 eV below the conduction band minimum. We confirmed the maximum defect concentration to be 3.66 × 1016 cm−3 at 0.27 eV (E3). As a result, we clearly confirmed the distribution of density of defect states in the ZnO band gap.


1998 ◽  
Vol 532 ◽  
Author(s):  
F. Boussaid ◽  
F. Olivie ◽  
M. Benzohra ◽  
D. Alquier ◽  
A. Claverie ◽  
...  

ABSTRACTUltra-shallow p+ -n junctions have been obtained from Ge+ -preamorphized and crystalline <100> silicon substrates. B+ and BF2+ dopants have been used. Boron was implanted at low energy 3 keV / 1015 cm−2 while an equivalent energy of 15 keV / 1015 cm−2 was chosen for BF2+. Rapid Thermal Annealing (RTA) for 15 s at 950 °C was then used for dopant electrical activation and implantation damage removal. Electrically active defects in these samples were characterized using Deep Level Transient Spectroscopy (DLTS) and isothermal transient capacitance (ΔC(t, T)). Two electron traps were detected in the upper half of the band gap at Ec – 0.20 eV and Ec – 0.45 eV, respectively. These traps are shown to be induced by the Ge+ preamorphization stage. Dopant implantation along with RTA result in the formation of a depth distributed energy continuum for B+ and BF2+ implants. Each continuum has been ascribed to annealing residual defects. Low energy B+ implantation is seen to induce twice as many defects as BF2+, implantation. From isothermal transient capacitance (ΔC(t, T)), reliable damage concentration profiles have been obtained, revealing that preamorphization induces not only defects in the regrown silicon layer but also a relatively high concentration of electrically active defects up to 3.5 μm into the bulk.


2008 ◽  
Vol 1 ◽  
pp. 091101 ◽  
Author(s):  
Yoshitaka Nakano ◽  
Yoshihiro Irokawa ◽  
Masaki Takeguchi

1986 ◽  
Vol 77 ◽  
Author(s):  
Run-Di Hong ◽  
David W. Jenkins ◽  
S. Y. Ren ◽  
John D. Dow

ABSTRACTWe report theoretical calculations of deep levels in GaAs/AlxGa1−xAs superlattices under hydrostatic pressure. We predict phase diagrams for DX centers: for a given composition x there is a function p(a), which relates pressure p and GaAs quantum-well width a, and defines a phase boundary between two regions: one in which DX is a deep trap in the fundamental band gap and another in which the DX deep level lies in the conduction band.


Sign in / Sign up

Export Citation Format

Share Document