2016
DOI: 10.1038/srep34586
|View full text |Cite
|
Sign up to set email alerts
|

Effective suppression of efficiency droop in GaN-based light-emitting diodes: role of significant reduction of carrier density and built-in field

Abstract: A critical issue in GaN-based high power light-emitting diodes (LEDs) is how to suppress the efficiency droop problem occurred at high current injection while improving overall quantum efficiency, especially in conventional c-plane InGaN/GaN quantum well (QW), without using complicated bandgap engineering or unconventional materials and structures. Although increasing thickness of each QW may decrease carrier density in QWs, formation of additional strain and defects as well as increased built-in field effect … Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1

Citation Types

0
19
0

Year Published

2017
2017
2022
2022

Publication Types

Select...
8
1

Relationship

0
9

Authors

Journals

citations
Cited by 37 publications
(19 citation statements)
references
References 32 publications
(28 reference statements)
0
19
0
Order By: Relevance
“…Figure 4b shows that the PL peak energy and the corresponding FWHM remained roughly constant at RT as the carrier density increases to 50×10 3 kW/cm 2 and 2×10 3 kW/cm 2 , respectively, indicating a negligible QCSE and confirming our EL results. When the excitation density increases further (> 10×10 3 kW/cm 2 ), the FWHM gradually increases due to the contribution of the band-filling effect of the high-energy localized centers, 27,29 resulting in a peak blue-shift above 50×10 3 kW/cm 2 . The IQE is calculated from the PDPL measurements using the ABC model (Equation S1, generated in terms of the optically generated carriers ‫ܩ(‬ ௧ ) in the Supporting Information); by using the fitting parameter (ܳ ଶ ) (Supporting Information Equation S7), the IQE can be expressed as 25…”
Section: Resultsmentioning
confidence: 99%
“…Figure 4b shows that the PL peak energy and the corresponding FWHM remained roughly constant at RT as the carrier density increases to 50×10 3 kW/cm 2 and 2×10 3 kW/cm 2 , respectively, indicating a negligible QCSE and confirming our EL results. When the excitation density increases further (> 10×10 3 kW/cm 2 ), the FWHM gradually increases due to the contribution of the band-filling effect of the high-energy localized centers, 27,29 resulting in a peak blue-shift above 50×10 3 kW/cm 2 . The IQE is calculated from the PDPL measurements using the ABC model (Equation S1, generated in terms of the optically generated carriers ‫ܩ(‬ ௧ ) in the Supporting Information); by using the fitting parameter (ܳ ଶ ) (Supporting Information Equation S7), the IQE can be expressed as 25…”
Section: Resultsmentioning
confidence: 99%
“…11,12 In addition, the straininduced internal polarization field will tilt the green LED band diagrams of QWs more seriously than those of blue ones, leading to a so-called "efficiency droop" in InGaN-based green LEDs, which has been attributed to the inefficient hole transport and increased electron overflow out of the active region. 13,14 These two problems have seriously hampered the development of SSL, especially for high-power LEDs, whose operating current is usually greater than 350 mA and even up to 1 A, having dimensions of approximately 1 × 1 mm 2 . 15 Many efforts have been made to solve these two problems, such as designing novel MQW structures 14−16 or optimizing growth parameters.…”
mentioning
confidence: 99%
“…Additionally, in order to incorporate In sufficiently, it is usually accomplished by sacrificing the growth temperature of InGaN quantum wells (QWs), resulting in a significant deterioration of the material quality in the QWs due to crystal defects. , On the other hand, the higher In composition in well layers induces a larger piezoelectric polarization electric field, resulting in a quantum confinement Stark effect (QCSE). The QCSE restricts the internal quantum efficiency (IQE) by reducing the overlap integral between the electron and hole wave functions, resulting in a lower recombination efficiency. , In addition, the strain-induced internal polarization field will tilt the green LED band diagrams of QWs more seriously than those of blue ones, leading to a so-called “efficiency droop” in InGaN-based green LEDs, which has been attributed to the inefficient hole transport and increased electron overflow out of the active region. , These two problems have seriously hampered the development of SSL, especially for high-power LEDs, whose operating current is usually greater than 350 mA and even up to 1 A, having dimensions of approximately 1 × 1 mm 2 …”
mentioning
confidence: 99%
“…As the strength of the internal electric field increases, electron leakage from the MQWs to the p-GaN layer increases and hole injection into the MQW active region becomes increasingly inefficient, which aggravates the efficiency droop problem. In addition, the internal electric field was reported to increase the Auger recombination rate, which also leads to an increase in efficiency droop 13 14 15 . Therefore, a number of studies have been devoted to reducing the polarization-induced field in InGaN QWs.…”
mentioning
confidence: 99%