Deep level effects on the characteristics of Al0.24Ga0.76As/In0.20Ga0.80As/GaAs and In0.48Ga0.52P/In0.20Ga0.80As/GaAs high electron mobility transistors grown by solid source molecular beam epitaxy

Citation
Sf. Yoon et al., Deep level effects on the characteristics of Al0.24Ga0.76As/In0.20Ga0.80As/GaAs and In0.48Ga0.52P/In0.20Ga0.80As/GaAs high electron mobility transistors grown by solid source molecular beam epitaxy, SOL ST ELEC, 44(11), 2000, pp. 1909-1916
Citations number
15
Categorie Soggetti
Apllied Physucs/Condensed Matter/Materiales Science","Eletrical & Eletronics Engineeing
Journal title
SOLID-STATE ELECTRONICS
ISSN journal
00381101 → ACNP
Volume
44
Issue
11
Year of publication
2000
Pages
1909 - 1916
Database
ISI
SICI code
0038-1101(200011)44:11<1909:DLEOTC>2.0.ZU;2-G
Abstract
Deep level transient spectroscopy has been used to characterise the deep le vels in Al0.24Ga0.76As/In0.20Ga0.80As/GaAs and In0.48Ga0.52P/In0.20Ga0.80As /GaAs pseudomorphic high electron mobility transistors (pHEMTs) grown by so lid source molecular beam epitaxy. Only one electron trap was detected in t he Al(0.24)Ga(0.76)AS and In0.48Ga0.52P layers of the Al0.24Ga0.76As/In0.20 Ga0.80As/GaAs and In0.48Ga0.52P/In0.20Ga0.80As/GaAs pHEMT, respectively. Th e activation energy of the electron trap is 0.49 eV for the Al0.24Ga0.76As/ In(0.20)Ga(0.80)AS/GaAS pHEMT and 0.40 eV for the In0.48Ga0.52P/In0.20Ga0.8 0As/GaAs pHEMT. The trap concentration is 1.72 x 10(20) and 2.38 x 10(20) c m(-3) for these devices, respectively. The current-voltage characteristics of the devices were measured at 300, 77 and 30 K. Drain current collapse at temperature below 77 K at low drain bias and persistent photoconductivity effect was evident in the (Al0.24Ga0.7As)-As-6/In0.20Ga0.80As/GaAs pHEMT. S uch effects were not observed in the In0.48Ga0.52P/In0.20Ga0.80As/GaAs devi ces, indicating that the DX centres are only present in the Al(0.24)Ga(0.76 )AS layers. The drain saturation current of the devices becomes smaller due to the carriers being captured by the defects, and the transconductance be comes higher due to an increase in carrier mobility in the channel as the t emperature was lowered from 300 to 30 K. (C) 2000 Published by Elsevier Sci ence Ltd, All rights reserved.