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Probing InGaN RGB micro-LEDs on silicon

Time: 2024-03-01From: Shenzhen ADY Lighting Factory

The author Mike Cooke is a freelance technology journalist who has worked in the semiconductor and advanced technology sectors since 1997.

Xiamen University and Latticepower Co Ltd in China report on the characteristics of micron-scale light-emitting diodes (LEDs) fabricated from aluminum indium gallium nitride (AlInGaN) structures grown on silicon (Si) with a view to their use in displays, particular for virtual-reality and augmented-reality (VR/AR) systems [Xi Zheng et al, Appl. Phys. Lett., v124, p051103, 2024].

The team comments: “Few investigations have been carried out on the chromatic characteristics of the InGaN-based red, green, and blue (RGB) micro-LEDs system grown on silicon substrates, which can contribute to a better understanding of the designs of the driver, back-plane integration, and heat dissipation.”

Figure 1: (a) Electroluminescence emission images (at 1A/cm2) of red, green, and blue micro-LEDs with diameters of 8μm and 20μm, respectively. (b) Schematic cross-section for red/green/blue micro-LEDs.

The researchers used metal-organic chemical vapor deposition (MOCVD) on 4-inch (111)silicon to prepare the materials for the respective micro-LEDs (Figure 1).

LEDs with 8μm and 20μm diameters were fabricated: The first step was to deposit silver/titanium/tungsten (Ag/Ti/W) on the p-GaN contactlayer, using electron-beam evaporation. The material was flipped and bonded onto a (100)Si substrate, and the (111) growth substrate was removed. The n-contact electrode consisted of indium tin oxide (ITO). Silicon dioxide (SiO2) was used for passivation.

While the green and blue multiple quantum well (MQW) active regions used 8-period structures with InGaNwells and GaN barriers, the red device had only three wells of InGaN separated by AlN/AlGaN/GaN hybrid barrier layers. The aim was to reduce lattice mismatch, relieving the strain of the high-indium-content InGaN epitaxial layers.

The longer-wavelength red-emitting devices suffered from reduced performance. Current-voltage measurements showed an ideality factor (n, ‘ideal’=1) increasing with wavelength: 1.79, 2.60, and 3.08 for the blue, green, and red micro-LEDs, respectively. The team comments: “When the factor n is larger than 2, the inferior carrier injection efficiency may originate from the severe defect-assisted non-ideal carrier transport, including trap-assisted tunneling, carrier leakage, etc, the larger n of the red micro-LEDs can be attributed to the non-radiative centers induced by defects.”

Table 1: Micro-LED performance, 8μm diameter.


Color

EQEmax

Wavelength

FWHM

EQE droop @100A/cm2

Blue 6.1% (@16A/cm2) 467nm 22nm 9.6%
Green 3.8% (10A/cm2) 545nm 35nm 26.6%
Red 0.23% (0.265A/cm2) 689nm 70nm 55.3%

A study of the light-emission of the 8μm- (Tableb) and 20μm-diameter (Tablec) LEDs showed reduced external quantum efficiency (EQEmax) maximum performance for the longer wavelengths and smaller diameter. Also, the full-width at half-maximum (FWHM) of the emission spectrum was broader for the green and red devices.

The reduced performance of the smaller devices is attributed to the increased importance of sidewall damage leading to greater non-radiative recombination of electron and hole charge carriers.

Table 2: Micro-LED performance, 20μm diameter.


Color

EQEmax

Centroid wavelength

FWHM

EQE droop @100A/cm2

Blue 8.2% (2.65A/cm2) 467nm 23nm 18.6%
Green 5.1% (5.3A/cm2) 544nm 36nm 36.2%
Red 0.62% (0.1A/cm2) 688nm 72nm 59.5%

Also, stronger quantum-confined Stark effect (QCSE) and higher defect densities in the higher-indium-content MQWs needed for longer wavelengths result in a more severe droop in EQE at higher current injection from the maximum value. QCSE refers to the presence of strong electric fields in strained semiconductor structures from the different charge polarizations of the chemical bonds in the various layers.

The reduced droop effect in the smaller devices was attributed to “better current crowding and heat dissipation in a smaller mesa”.

The devices also suffered from a blue shift at higher current injection due to screening of built-in QCSE electric field and band-filling effects effectively widening the bandgap.

The researchers calculated the color performance of the devices in combination and separately (Figure 2). The researchers used comparison standards from the ITU-Recommendation BT.2020 (Rec.2020) and the National Television Systems Committee (NTSC). Area ratios compare the color triangle areas on the chromaticity diagram of a notional display using the RGB LEDs relative to the standard (hence it can exceed 100%). The coverage ratio only includes the display triangle area inside the standard relative to the standard (and hence must be less than 100%).

Figure 2: (a) Current density dependence of area ratio of NTSC for mixed RGB micro-LED systems. (b)The coverage ratio of NTSC and Rec.2020 under different current densities. (c)Color purity versus current density for separate RGB micro-LEDs with dimensions of 8μm and 20μm.

In terms of color purity of the RGB devices, the green LED was seen to suffer from a severe decline as the current injection increased. The team comments: “Since the color gamut of the RGB mixed system is more sensitive to the chromaticity coordinate of the green self-emitting unit, the lower color purity of the 20μm green micro-LED can result in the decrease in the area ratio and the coverage ratio of the standard color gamut of the RGB mixed micro-LED systems.”

The researchers also studied the thermal stability of the devices between 290K and 350K. The shift for the 20μm LEDs was larger than for 8μm. The researchers say that this suggests that “the micro-LEDs with a shrunken mesa dimension can exhibit superior chromatic stability with temperature, which can be explained by the better heat dissipation and higher color purity of the 8μm micro-LEDs.”

Tags: LEDs AlInGaN InGaN MOCVD