Introduction
It is expected that lighting will ultimately move towards “smart lighting”, meaning that such smart lighting can exhibit multiple functions for not only general illumination but also digitalized applications, where visible light wireless communication such as Light Fidelity (Li-Fi) is a typical example. The key component for smart lighting is a white light-emitting diode (LED) featured with both high efficiency and high data transmission rates. The last two decades have seen major progress in developing white LEDs overwhelmingly based on III-nitride semiconductors. So far, the current state-of-the-art white LEDs mainly based on the well-known “blue LED + yellow phosphor” method have approached their limit in terms of overall performance including both efficiency and color rendering index. However, such phosphor-converted white LEDs are still far from satisfactory. One of the fatal issues is due to the very slow response time of yellow phosphors, typically on the order of microseconds, leading to a limited bandwidth down to several MHz level for Li-Fi applications [1] , [2].
In order to achieve the best lighting quality (in terms of both color rendering index and chromaticity) with multiple functions (display, communications, detection, etc.), it is an ideal solution to fabricate white LEDs by mixing individually addressable red, green and blue (RGB) LED components. In that case, three independent RGB components forming a white LED can be modulated using the wavelength division multiplexing (WDM) technology. In [3], by means of the RGB LED approach, a 3.4 Gbit/s data rate has been demonstrated. Furthermore, augmented reality/virtual reality (AR/VR) requires portable display, where a micro-display with an ultrafast response is required. Therefore, the fabrication of a micro-display using RGB LEDs demonstrates a great potential to offer high color quality and dimmable display pixels [4]. For opto-genetics applications, where the blue/green opsin can be driven by blue and green LEDs [5], a green LED is also an indispensable component which needs to be modulated for opsin excitation.
The above facts indicate that only all the three discrete red, green and blue LED components are well controlled and modulated in an ultra-fast manner can these multiple functions be achieved. Therefore, an electrical channel with an ultrafast speed is necessary for the interconnection between LED driving transistors and individual LED components, for which high electron mobility transistors (HEMTs) are a good option. Therefore, in order to address the above issues, the fabrication of an integrated HEMT-LED is a promising and reliable approach [6].
Except of the bandwidth, a uniform light emission is also necessary for many applications. For instance, the short-distance transmission via plastic optical fiber (POF) also requires a green light source at 500 nm with uniform light emission for the POF systems [7].
So far, the progress on the fabrication of integrated HEMT-LED is limited to the blue spectral range and lateral layout arrangement [11], [12], where the HEMT is located side-by-side to the blue LED. The existing layout will cause serious current crowding and heating issue especially at high injection current. Moreover, there is no any report about the fabrication of an integrated HEMT-LED in the longer wavelength such as green regime. One of the fundamental reasons is due to the well-known “green gap” issue, although great efforts have been invested in order to bridge the gap [8]–[10]. Consequently, it is crucial to develop a uniform green HEMT-LED served as an essential element for the RGB LED approach stated above. In this paper, for the first time, we report a monolithically integrated HEMT-LED with a circular layout arrangement, which can emit uniform green light and be well controlled by its gate voltage.
Experimental Details
Among all the approaches developed for monolithically integrating HEMTs with LEDs so far, the metal-interconnection-free scheme reported has demonstrated major advantages in terms of higher reliability and less parasitic effects [12]. In this scheme, the LED can be electrically integrated with an HEMT via the 2DEG channel of the HEMT to form a compact HEMT-LED device. The growth procedure is described as following. First, a GaN HEMT epiwafer is grown on a standard c-plane sapphire substrate by means of a metal-organic vapor phase epitaxy (MOVPE) technique. The GaN HEMT epiwafer is grown by using our high-temperature AlN (HT-AlN) buffer approach [13]. After the sapphire substrate is initially subject to a high temperature annealing process under H2 ambient, a 600 nm HT-AlN layer is grown, followed by a 1.5 μm undoped GaN layer, then a 1 nm AlN spacer layer and a final 25 nm Al0.25 Ga0.75N barrier layer.
As shown in Fig. 3(a) and (b), in order to prepare a patterned template for further green LED overgrowth, a 500 nm SiO2 layer is deposited on the HEMT epiwafer by plasma-enhanced chemical vapor deposition (PECVD), and then patterned by a combination of standard lithography technique and subsequent dry etching processes in order to form window regions where a green LED structure will be selectively grown later. Within the window regions, the active region of HEMT epiwafer has been etched down to 300 nm, namely, down to the GaN buffer layer of the HEMT epiwafer.
Subsequently, the patterned template featured with selective etching is reloaded into the MOVPE chamber for further LED growth after a special surface treatment of 5-min photo-assisted KOH etching which aims to remove any damages induced during the dry-etching processes. A 100 nm undoped GaN is initially selectively grown within the window regions for a better n-GaN interface, followed by a 1 μm n-GaN layer. Three periods of InGaN/GaN multiple quantum wells (MQWs) are then grown, where each quantum well consists of a 2.5 nm InGaN quantum well separated by a 10 nm GaN barrier. Finally, 15 nm p-AlGaN as an electron blocking layer and then a 150 nm p-doped GaN followed by a 5 nm heavily doped GaN capping layer are grown. After the selective epitaxial overgrowth, the SiO 2 mask has been completely removed by a 40% HF solution.
X-ray diffraction (XRD) and photoluminescence (PL) measurements have been performed in order to characterize the
sample. Fig. 1 shows excitation-power dependent PL spectra, still
exhibiting a green emission centered at 500 nm and a clear blue-shift (to 493 nm) under the strong
excitation power density increasing from
Finally, an integrated HEMT-LED device will be fabricated. In the very first step of HEMT-LED fabrication, the HEMT mesa (300 nm) and LED mesa (500 nm) are defined by a standard inductively coupled etching (ICP), respectively. A source/drain Ohmic contact (Ti/Al/Ti/Au: 20/50/150/80 nm) for the HEMT are deposited by thermal evaporation and then annealed in 850˚C under N2 ambient. A Ni/Au layer with their individual thickness of 7 and 7 nm is used as a current spreading layer. A layer of Ti/Al/Ti/Au with their thickness of 20/150/50/50 nm as an electrode for LED and a Schottky contact (Ni/Au: 50/150 nm) for the gate of HEMT are finally deposited. A schematic illustration for the whole fabrication process is depicted in Fig. 3, where the red dash line represents the 2DEG channel serving as an interconnection between the HEMT and the green LED.
Results
Fig. 4(a)–(c) show the
optical microscope image and the layout of our green HEMT-LED device, respectively. A circular layout design is
adopted, meaning that the ring-shaped LED surrounds the HEMT in order to facilitate current spreading. For the
ring-shaped LED, the inner and outer diameter are 140 μm and 600 μm, respectively. As for the HEMT driving
transistor's layout parameters shown in Fig. 4(c), source diameter
(a) Optical microscope image of our HEMT-LED devices. (b) Schematic illustration of our device in 3D. (c) Layout parameters for the integrated HEMT.
Fig. 5 shows current-voltage (I-V) and transfer characteristics of our integrated green HEMT-LED devices, indicating a turn-on voltage of 3 V, which is reasonable considering the serially connected LED diode to the drain terminal of the HEMT. The maximum current density and trans conductance for HEMT is 35 mA/mm and 16.7 mS/mm, respectively. The whole HEMT-LED device shows a static on resistance of 441 Ω, including the on resistance of 300 μm-width HEMT and the ring-shaped LED. Since the current of HEMT-LED can be simply tuned by its gate voltage, the HEMT-LED itself can be used as a modulated light source. Fig. 6(a) and (b) show an electroluminescence (EL) emission image taken at 1 mA and EL spectra as a function of injection current, respectively. A very uniform green light emission has been achieved. Fig. 6(b) shows a peak wavelength shifting from 507.5 nm to 503.5 nm when the injection current increases from 1 to 6 mA.
HEMT-LED devices (a) I-V (inset: an equivalent circuit of HEMT-LED). (b) Transfer characteristics.
(a) EL emission image taken at 1 mA. (b) EL spectra as a function of injection current.
At the moment, the HEMT features a low maximum current density (35 mA/mm), almost one order smaller than the reported current density of GaN HEMT [18]. Further investigation is ongoing in order to identify whether the low current is due to either overgrowth or dry-etching induced damages. It should be noted that a low growth temperature for the overgrowth of InGaN/GaN MQWs is required in order to achieve green emission.
Conclusion
To conclude, we have demonstrated a prototype green HEMT-LED device with uniform light emission at 507 nm. The ring-shaped LED can be driven and well controlled by the integrated circular HEMT through simply tuning the gate voltage of HEMT. This controllable uniform green HEMT-LED device paves the way for applying the RGB-LED solution in fabricating smart lighting devices for many practical applications where controllable green LEDs are an essential component, such as tunable spectrum white LED for high-quality lighting, three-channel visible light communication for Li-Fi, full color LED displays for AR/VR and optogenetics for biomedical diagnosis.