Optical deep level transient spectroscopy of minority carrier traps in n-type high-purity germanium

1997 ◽  
Vol 81 (10) ◽  
pp. 6767-6772 ◽  
Author(s):  
A. Blondeel ◽  
P. Clauws ◽  
D. Vyncke
Keyword(s):  
High Purity ◽  
Deep Level Transient Spectroscopy ◽  
Minority Carrier ◽  
Deep Level ◽  
High Purity Germanium ◽  
Carrier Traps ◽  
Transient Spectroscopy

scholarly journals Deep Level Transient Spectroscopy of High-Purity Germanium Diodes/Detectors

1979 ◽  
Vol 26 (1) ◽  
pp. 265-270 ◽  
Author(s):  
Eugene E. Haller ◽  
Pearl P. Li ◽  
G. Scott Hubbard ◽  
William L. Hansen
Keyword(s):  
High Purity ◽  
Deep Level Transient Spectroscopy ◽  
Deep Level ◽  
High Purity Germanium ◽  
Transient Spectroscopy

Characterization of Traps in GaN pn Junctions Grown by MOCVD on GaN Substrate Using Deep-Level Transient Spectroscopy

2008 ◽  
Vol 600-603 ◽  
pp. 1297-1300 ◽  
Author(s):  
Yutaka Tokuda ◽  
Youichi Matsuoka ◽  
Hiroyuki Ueda ◽  
Osamu Ishiguro ◽  
Narumasa Soejima ◽  
...  
Keyword(s):  
Deep Level Transient Spectroscopy ◽  
Minority Carrier ◽  
Deep Level ◽  
Electron Traps ◽  
Majority Carrier ◽  
Sapphire Substrates ◽  
Carrier Traps ◽  
Pn Junctions ◽  
Transient Spectroscopy

Minority- and majority-carrier traps were studied in GaN pn junctions grown homoepitaxially by MOCVD on n+ GaN substrates. Two majority-carrier traps (MA1,MA2) and three minority-carrier traps (MI1, MI2, MI3) were detected by deep-level transient spectroscopy. MA1 and MA2 are electron traps commonly observed in n GaN on n+ GaN and sapphire substrates. No dislocation-related traps were observed in n GaN on n+ GaN. Among five traps in GaN pn on GaN, MI3 is the main trap with the concentration of 2.5x1015 cm-3.

Investigating Minority-Carrier Traps in p-type Cu(InGa)Se2 Using Deep Level Transient Spectroscopy

2005 ◽  
Vol 865 ◽  
Author(s):  
Steven W. Johnston ◽  
Jehad A. M. AbuShama ◽  
Rommel Noufi
Keyword(s):  
Deep Level Transient Spectroscopy ◽  
Minority Carrier ◽  
Deep Level ◽  
Thermionic Emission ◽  
Small Peak ◽  
Carrier Traps ◽  
Transient Spectroscopy ◽  
Lower Temperature ◽  
And Shifts ◽  
P Type

AbstractMeasurements of p-type Cu(InGa)Se2 (CIGS) using deep-level transient spectroscopy (DLTS) show peaks associated with minority-carrier traps, even though data were collected using reverse bias conditions not favorable to injecting minority-carrier electrons. These DLTS peaks occur in the temperature range of 50 to 150 K for the rate windows used and correspond to electron traps having activation energies usually in the range of 0.1 to 0.2 eV for alloys of CIS, CGS, and CIGS. The peak values also depend on the number of traps filled. For short filling times of 10 μs to 100 μs, a small peak appears. As the DLTS filling pulse width increases, the peak increases in response to more traps being filled, but it also broadens and shifts to lower temperature suggesting that a possible series of trap levels, perhaps forming a defect band, are present. The peaks usually saturate in a timeframe of seconds. These filling times are sufficient for electrons to fill traps near the interface from the n-type side of the device due to a thermionic emission current. Admittance spectroscopy data for the same samples are shown for comparison.

scholarly journals Characterization of a Dominant Electron Trap in GaNAs Using Deep-Level Transient Spectroscopy

2005 ◽  
Vol 891 ◽  
Author(s):  
Steven W. Johnston ◽  
Sarah R. Kurtz ◽  
Richard S. Crandall
Keyword(s):  
Deep Level Transient Spectroscopy ◽  
Minority Carrier ◽  
Deep Level ◽  
Chemical Vapor ◽  
Electron Trap ◽  
Organic Chemical ◽  
Conduction Band Offset ◽  
Carrier Traps ◽  
Transient Spectroscopy ◽  
P Type

ABSTRACTDilute-nitrogen GaNAs epitaxial layers grown by metal-organic chemical vapor deposition were characterized by deep-level transient spectroscopy (DLTS). For all samples, the dominant DLTS signal corresponds to an electron trap having an activation energy of about 0.25 to 0.35 eV. The minority-carrier trap density in the p-type material is quantified based on computer simulation of the devices. The simulations show that only about 2% of the traps in the depleted layer are filled during the transient. The fraction of the traps that are filled depends strongly on the depth of the trap, but only weakly on the doping of the layers and on the conduction-band offset. The simulations provide a pathway to obtain semi-quantitative data for analysis of minority-carrier traps by DLTS.

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