A mechanism for two-electron capture at deep level defects in semiconductors

1989 ◽  
Vol 29 (4) ◽  
pp. 663
1992 ◽  
Vol 262 ◽  
Author(s):  
Irai Lo ◽  
W. C. Mitchel ◽  
C. E. Stutz ◽  
K. R. Evans ◽  
M. O. Manasreh

ABSTRACTWe have performed Shubnikov-de Haas (SdH) measurements on the AlxGa1-xSb/InAs QW's with x from 0.1 to 1.0 under the negative persistent photoconductivity (NPPC) conditions and confirmed the prediction of Ionized Deep Donor model that the NPPC effect is a universal property for the materials containing ionized deep donors at low temperatures. The time-dependent recombination (electron capture) of the ionized deep donors is similar to that of DX centers. The saturated reduction of carrier concentration in the InAs well increases with increasing x, and rises steeply at about x=0.4. The concentration of deep donors which cause the NPPC in the AlxGa1-xSb/InAs QW's increases with the Al composition.


2003 ◽  
Vol 94 (3) ◽  
pp. 1485-1489 ◽  
Author(s):  
H. K. Cho ◽  
C. S. Kim ◽  
C.-H. Hong
Keyword(s):  

1992 ◽  
Vol 281 ◽  
Author(s):  
J. Piprek ◽  
P. Krispin ◽  
H. Kostial ◽  
K. W. BÖer

ABSTRACTThe occupation of deep-level defects in semiconductors is investigated by delta-doping such impurities at a specified distance from the metallurgical boundary within Schottky diodes. Capacitance-voltage characteristics are analyzed using ID device simulation software. These characteristics change significantly depending on the deep-level energy and the sheet position. This new approach to deep-level analysis is applied to Schottky diodes on MBE-grown n-GaAs with a planar titanium doped sheet. At moderate Ti concentrations the well-known Ti acceptor level near Ec-0.2 eV governs the electrical properties. In addition, two other types of Ti defects are found.


2004 ◽  
Vol 815 ◽  
Author(s):  
X. D. Chen ◽  
C. C. Ling ◽  
S. Fung ◽  
C. D. Beling ◽  
H. S. Wu ◽  
...  

AbstractDeep level transient spectroscopy (DLTS) was used to study deep level defects in He-implanted n-type 6H-SiC samples. Low dose He-implantation (fluence ∼2×1011 ions/cm2) has been employed to keep the as-implanted sample conductive so that studying the introduction and the thermal evolution of the defects becomes feasible. A strong broad DLTS peak at 275K-375K (called signal B) and another deep level at EC-0.50eV were observed in the as-implanted sample. The intensity of the peak B was observed to linearly proportional to the logarithm of the filling pulse width, which is a signature for electron capture into a defect related to dislocation. After annealing at 500°C, the intensity of peak was significantly reduced and the remained signal has properties identical to the well known Z1/Z2 deep defects, although it is uncertain whether the Z1/Z2 exist in the as-implanted sample or it is the annealing product of the dislocation-related defect. The E1/E2 defect (EC-0.3/0.4eV) was not presence in the as-implanted sample, but was observed after the 300°C annealing.


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