III-nitride unipolar light emitting devices

Citation
Yg. Shreter et al., III-nitride unipolar light emitting devices, PHYS ST S-A, 180(1), 2000, pp. 307-313
Citations number
4
Categorie Soggetti
Apllied Physucs/Condensed Matter/Materiales Science
Journal title
PHYSICA STATUS SOLIDI A-APPLIED RESEARCH
ISSN journal
00318965 → ACNP
Volume
180
Issue
1
Year of publication
2000
Pages
307 - 313
Database
ISI
SICI code
0031-8965(20000716)180:1<307:IULED>2.0.ZU;2-7
Abstract
Unipolar light emitting device based on III-nitride superlattices for the g eneration of visible light is suggested. The main idea of the unipolar ligh t emitting device (U-LED) is to create the analogue of an n-p junction betw een two n-type superlattices with a shallow and a deep subband. The superla ttice with the shallow subband acts as an effective n-type semiconductor, w hereas the superlattice with deep subband plays the role of an effective p- type semiconductor. The radiation arises due to the electron transitions fr om the shallow subband superlattice into the deep subband superlattice. The conduction band off-set between AIN and InN is about 3 eV and this value c an be reduced using the alloys of AlGaN. This allows one to get electron tr ansitions between two superlattices based on these alloys with energies in the range of 0 to 3 eV, which covers the visible and the infrared range of the spectra. The quantum efficiency of these transitions could be enhanced by inserting between two superlattices some optically active layer with two quantum states, which can be a specially designed quantum well, impurity l ayer or quantum dot layer. The active layer can be pumped directly electric ally through the superlattice subbands. The efficiency of the device is lim ited by the non-radiative energy relaxation channel related to phonon emiss ion and is rather low for the simple U-LED without an active layer or an U- LED with a single quantum well active layer. A significant increase in the efficiency can be achieved with the use of the active layer doped with deep accepters. In this case the optical transitions take place from the quantu m well subband of the active layer into the deep acceptor impurity band. Th e transition metals Fe and Ni are considered as possible deep accepters for the active layer in GaInN/AlN superlattices.