TY - GEN
T1 - Low-voltage CMOS/BiCMOS light emitting devices
AU - Du Plessis, Monuko
AU - Aharoni, Herzl
AU - Snyman, Lukas W.
PY - 2005/12/1
Y1 - 2005/12/1
N2 - Low-voltage Si-LED operation can be achieved by fabricating devices with heavily doped n+p+ junctions. Differences are observed between high-voltage avalanche and low-voltage field emission LED performance. The low-voltage devices exhibit a non-linear light intensity L vs. reverse current I relationship at low current levels, but a linear dependency at higher currents, compared to the linear behavior of avalanche devices at all current levels. Three regions of operation are identified for the low-voltage field emission LED's, namely L ∝ I3 at low currents, L ∝ I 2 at medium currents and eventually L ∝ I at higher currents. In the low-voltage non-linear region of operation, the shape of the emitted spectrum changes with reverse current. At low reverse current the field emission devices emit more long wavelength radiation than short wavelength radiation. As the reverse current increases, the short wavelength radiation increases relative to the long wavelength radiation, and at higher currents in the linear region of operation the ratio between long and short wavelength radiation remains constant.
AB - Low-voltage Si-LED operation can be achieved by fabricating devices with heavily doped n+p+ junctions. Differences are observed between high-voltage avalanche and low-voltage field emission LED performance. The low-voltage devices exhibit a non-linear light intensity L vs. reverse current I relationship at low current levels, but a linear dependency at higher currents, compared to the linear behavior of avalanche devices at all current levels. Three regions of operation are identified for the low-voltage field emission LED's, namely L ∝ I3 at low currents, L ∝ I 2 at medium currents and eventually L ∝ I at higher currents. In the low-voltage non-linear region of operation, the shape of the emitted spectrum changes with reverse current. At low reverse current the field emission devices emit more long wavelength radiation than short wavelength radiation. As the reverse current increases, the short wavelength radiation increases relative to the long wavelength radiation, and at higher currents in the linear region of operation the ratio between long and short wavelength radiation remains constant.
KW - Electroluminescence
KW - Light emitting device
KW - Silicon
UR - http://www.scopus.com/inward/record.url?scp=46149126889&partnerID=8YFLogxK
U2 - 10.1109/COMMAD.2004.1577572
DO - 10.1109/COMMAD.2004.1577572
M3 - Conference contribution
AN - SCOPUS:46149126889
SN - 0780388208
SN - 9780780388208
T3 - Conference on Optoelectronic and Microelectronic Materials and Devices, Proceedings, COMMAD
SP - 393
EP - 396
BT - COMMAD04 - 2004 Conference on Optoelectronic and Microelectronic Materials and Devices -Proceedings
T2 - COMMAD04 - 2004 Conference on Optoelectronic and Microelectronic Materials and Devices
Y2 - 8 December 2004 through 10 December 2004
ER -