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GaInN‐based LED structures on selectively grown semi‐polar crystal facets
Author(s) -
Scholz Ferdinand,
Wunderer Thomas,
Feneberg Martin,
Thonke Klaus,
Chuvilin Andrei,
Kaiser Ute,
Metzner Sebastian,
Bertram Frank,
Christen Jürgen
Publication year - 2010
Publication title -
physica status solidi (a)
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.532
H-Index - 104
eISSN - 1862-6319
pISSN - 1862-6300
DOI - 10.1002/pssa.200983633
Subject(s) - epitaxy , electric field , materials science , quantum well , light emitting diode , optoelectronics , bar (unit) , quantum confined stark effect , piezoelectricity , nitride , polar , diode , indium nitride , facet (psychology) , indium , crystal (programming language) , optics , condensed matter physics , nanotechnology , physics , laser , computer science , composite material , psychology , social psychology , layer (electronics) , quantum mechanics , big five personality traits , programming language , personality , astronomy , meteorology
In conventional nitride‐based light emitting diodes, huge internal electric fields lead to a reduced overlap of electron and hole wave functions in the active GaInN quantum wells as a consequence of the piezoelectricity of these polar materials. In order to minimize these internal fields while still maintaining the well‐established c‐direction as main epitaxial growth direction for high‐quality low‐defect‐density layers, we have investigated semi‐polar LED structures on the side‐facets of triangular GaN stripes grown by selective area epitaxy. The reduced internal electric field could be confirmed by several spectroscopic methods. We found a strongly facet dependent growth mechanism leading to very flat surfaces on $\{ 1\bar {1}01\}$ facets as opposed to their $\{ 11\bar {2}2\}$ counterparts. An increased indium uptake on semipolar $\{ 1\bar {1}01\}$ facets as compared to conventional c‐plane layers helped to shift the LED emission to longer wave lengths beyond 500 nm in the green spectral range despite the significantly reduced field‐dependent Stark shift.