- Nano Express
- Open Access
Enhancement of light output power of GaN-based light-emitting diodes with photonic quasi-crystal patterned on p-GaN surface and n-side sidewall roughing
© Lai and Yang; licensee Springer. 2013
- Received: 2 November 2012
- Accepted: 6 December 2012
- Published: 17 May 2013
In this paper, GaN-based light-emitting diodes (LEDs) with photonic quasi-crystal (PQC) structure on p-GaN surface and n-side roughing by nano-imprint lithography are fabricated and investigated. At an injection current of 20 mA, the LED with PQC structure on p-GaN surface and n-side roughing increased the light output power of the InGaN/GaN multiple quantum well LEDs by a factor of 1.42, and the wall-plug efficiency is 26% higher than the conventional GaN-based LED type. After 500-h life test (55°C/50 mA), it was found that the normalized output power of GaN-based LED with PQC structure on p-GaN surface and n-side roughing only decreased by 6%. These results offer promising potential to enhance the light output powers of commercial light-emitting devices using the technique of nano-imprint lithography.
- Light-emitting diodes (LEDs)
- Photonic quasi-crystal (PQC)
- Nano-imprint lithography (NIL)
Impressive recent developments of high-brightness light extraction of GaN-based nitride light-emitting diodes (LEDs) is dominated on both material techniques such as metal organic chemical vapor deposition (MOCVD) epitaxial growth and device fabrication processes. Thus, high-brightness LEDs have been used in various applications, including large- and small-sized flat panel displays backlight, traffic signal light, and illumination lighting by white light LEDs [1, 2]. In order to get higher brightness of LEDs, extensive research has been conducted. One of the biggest problems in limited brightness of LEDs is the total internal reflection, which reduces the photon extraction efficiency of LEDs. Furthermore, the external quantum efficiency of GaN-based LEDs is low because the refractive index of the nitride epitaxial layer differs greatly from that of the air. The refractive indexes of GaN and air are 2.5 and 1.0, respectively. Thus, the critical angle at which light generated in the InGaN-GaN active region can escape is approximately [θ c = sin − 1(n air /n Gan )] ∼ 23°, which limits the external quantum efficiency of conventional GaN-based LEDs to only a few percent [3, 4]. In order to avoid total internal reflection, various improving of the light extraction efficiency and brightness in the LEDs have been studied, including surface roughening texturing method [4–12], sidewall roughness [13, 14], and insertion of two-dimensional (2D) photonic crystals (PhCs) [15–21]. All of these processes allow the photons generated within the LEDs to find the escape cone by multiple scattering from a rough surface, and a similar concept can also be applied to chip sidewalls. In other words, more photons should be able to escape from LEDs with surface patterned and textured chip sidewalls compared to LEDs with conventional flat chip. However, wet etching or nano-particle pattern with wet or dry etching used in most surface roughening techniques suffered the uniformity and reproduction problems.
In this paper, we report a feasibility of using nano-imprinting technique to fabricate patterned surface and sidewall of GaN-based LEDs for mass production. The nano-imprint technique is not only making well in controlling the nano-size coming truth but also highly reproducible. Hence, it is suitable for the mass production. Furthermore, only one pattern was used in this study to form structures in both top surface and sidewall region to combine the light enhancement effect of top and sidewall rough. The 12-fold photonic quasi-crystal (PQC) pattern was chosen as top and sidewall pattern owing to its capability to better enhance surface emission comparing with 2D PhC pattern approach . Besides, according to the results of our previous work, the PQC pattern applied on the GaN LED could get more concentrated in the far field pattern of the GaN LED by comparing with the simply roughed surface and other extraction structures. As a result, the light output efficiency of LED with PQC structure on n-side roughing and p-GaN surface was significantly higher than that of a conventional LED. Additionally, the intensity-current (L-I) measurements demonstrate that the light output power of LED with PQC on p-GaN surface, LED with PQC on n-side roughing, and LED with PQC structure on p-GaN surface and n-side roughing was higher than that of a conventional LED at 20 mA with standard device processing.
The GaN-based LED samples are grown by MOCVD with a rotating-disk reactor (Veeco, Plainview, NY, USA) on a c-axis sapphire (0001) substrate at the growth pressure of 200 mbar. The LED structure consists of a 50-nm-thick GaN nucleation layer grown at 500°C, a 2-μm un-doped GaN buffer, a 2-μm-thick Si-doped GaN buffer layer grown at 1,050°C, an unintentionally doped InGaN/GaN multiple quantum well (MQW) active region grown at 770°C, a 50-nm-thick Mg-doped p-AlGaN electron blocking layer grown at 1,050°C, and a 120-nm-thick Mg-doped p-GaN contact layer grown at 1,050°C. The MQW active region consists of five periods of 3 nm/7-nm-thick In0.18Ga0.82N/GaN quantum well layers and barrier layers.
Step 3 is in a simultaneous thermal and UV imprinting process, which is executed by the IPS imprinted on a pre-heated polymer layer. Applying a high pressure of 40 bar, the UV radiation time of 10 s and the constant working temperature of 65°C, the PQC pattern on the IPS can fully transfer to the polymer layer. In step 4, the LED samples and the IPS were then cooled down to the room temperature and release the IPS automatically. In step 5, the dry etching process of reactive ion etching (RIE) with CF4 plasma can remove the residual polymer layer and transfer the pattern onto the SiO2 film. The nano-imprint resin consists of a perfluorinated acrylate polymer and a photoinitiator. In step 6, we then used an inductively coupled plasma reactive ion etching (ICP-RIE) with BCl3/Ar plasma to transfer the pattern onto p-GaN surface.
The ‘photonic quasi-crystal’ is unusual with respect that on first sight, they appear random; however, on closer inspection, they were revealed to possess long range order but short range disorder [22, 23]. The 12-fold PQC pattern was obtained from the PhCs with a dodecagonal symmetric quasi-crystal lattice than regular PhCs with triangular lattice and 8-fold PQC . The recursive tiling of offspring dodecagons packed with random ensembles of squares and triangles in dilated parent cells forms the lattice. Additionally, the PQC rod dimension and pattern pitch were approximately 515 and 750 nm in this study according to  and roughly simulate calculation. Besides, dry etching depth of PQC structure was approximately 95 nm which was optimized through various depth etching, (the data is not shown here) since this etching depth could attain the best performance of light extraction efficiency of our LED structure from our etching test experiments. Figure 3c,d shows the p-GaN surface and the n-side roughing regions of cross section SEM images with PQC pattern, respectively. Further, the dry etching depth of the LED with PQC on n-side roughing was approximately 1.02 μm.
The light output is detected by calibrating an integrating sphere with Si photodiode on the package device. The intensity-current (L-I) characteristics of the LEDs with and without PQC structure are shown in Figure 4b. At an injection current of 20 mA and peak wavelength of 460 nm for TO (transistor outline) can package, the light output powers of conventional LED, LED with PQC on p-GaN surface, LED with PQC on n-side roughing, and LED with PQC structure on p-GaN surface and n-side roughing on TO can are given by 11.6, 13.5, 15.1, and 16.5 mW, respectively. Hence, the enhancement percentages of LED with PQC on p-GaN surface, LED with PQC on n-side roughing, and LED with PQC structure on p-GaN surface and n-side roughing were 16%, 30%, and 42%, respectively, compared to that of the conventional LED. The higher enhancement of LED with both PQC structures was scattering and guiding light from LED top surface and n-side roughing onto the LED top direction [14, 21, 24] to increase more light output power. In addition, the corresponding wall-plug efficiencies (WPE) of conventional LED, LED with PQC on p-GaN surface, LED with PQC on n-side roughing, and LED with PQC structure on p-GaN surface and n-side roughing were 19%, 22%, 24%, and 26%, respectively, which addresses a substantial improvement by the PQC structures on top surface and n-side roughing as well at a driving current of 20 mA. Comparing with the conventional LED, the WPEs of LED with PQC on p-GaN surface, LED with PQC on n-side roughing, and LED with PQC structure on p-GaN surface and n-side roughing were increased by 15.8%, 26.3%, and 36.8%, respectively, at an injection current of 20 mA, The enhancement of WPE of LED with PQC structure on p-GaN surface and n-side roughing is relatively high comparing with other researches [10, 13, 14, 24, 25], which is because the light emitted from LED scattered by top PQC pattern and guided onto the LED top direction by n-side roughing [22, 23, 26], therefore resulting in the enhancement of WPE.
The GaN-based LEDs with PQC structure on p-GaN surface and n-side roughing by nano-imprint lithography are fabricated and investigated. At a driving current of 20 mA on TO can package, the light output power of LED with PQC on p-GaN surface, LED with PQC on n-side roughing, and LED with PQC structure on p-GaN surface and n-side roughing were enhanced by a factor of 1.16, 1.30, and 1.42, respectively, and the wall-plug efficiency of the InGaN/GaN LED was increased by 26% with the PQC structure on p-GaN surface and n-side roughing. After 500-h life test (55°C/50 mA) condition, the normalized output power of LED with PQC structure on p-GaN surface and n-side roughing only decreased by 6%. This work offers promising potential to increase output powers of commercial light-emitting devices by using nano-imprint lithography.
The authors would like to thank Dr. H.W. Huang for the valuable discussions and experimental assistance. The authors gratefully acknowledge a partial financial support from the National Science Council (NSC) of Taiwan under contract no. NSC 99-2221-E-155-014-MY3.
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