Ying-Yuan Huang
National Taiwan University
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Featured researches published by Ying-Yuan Huang.
Optics Express | 2010
Liang-Yi Chen; Ying-Yuan Huang; Chun-Hsiang Chang; Yu-Hsuan Sun; Yun-Wei Cheng; Min-Yung Ke; Cheng-Pin Chen; JianJang Huang
We fabricated InGaN/GaN nanorod light emitting diode (LED) arrays using nanosphere lithography for nanorod formation, PECVD (plasma enhanced chemical vapor deposition) grown SiO(2) layer for sidewall passivation, and chemical mechanical polishing for uniform nanorod contact. The nano-device demonstrates a reverse current 4.77nA at -5V, an ideality factor 7.35, and an optical output intensity 6807mW/cm(2) at the injection current density 32A/cm(2) (20mA). Moreover, the investigation of the droop effect for such a nanorod LED array reveals that junction heating is responsible for the sharp decrease at the low current.
Nanotechnology | 2011
Ying-Yuan Huang; Liang-Yi Chen; Chun-Hsiang Chang; Yu-Hsuan Sun; Yun-Wei Cheng; Min-Yung Ke; Yu-Hsin Lu; Hao-Chung Kuo; JianJang Huang
For InGaN/GaN based nanorod devices using a top-down etching process, the optical output power is affected by non-radiative recombination due to sidewall defects (which decrease light output efficiency) and the mitigated quantum confined Stark effect (QCSE) due to strain relaxation (which increases internal quantum efficiency). Therefore, the exploration of low-temperature optical behaviors of nanorod light emitting diodes (LEDs) will help identify the correlation between these two factors. In this work, low-temperature electroluminescent (EL) spectra of InGaN/GaN nanorod arrays were explored and compared with those of planar LEDs. The nanorod LED exhibits a much higher optical output percentage increase when the temperature decreases. The increase is mainly attributed to the increased carriers in the quantum wells for radiative recombination. Also, due to a better spatial overlap of electrons and holes in the quantum wells, the increased number of carriers can be more efficiently recombined in the nanorod device. Next, while the nanorod array shows nearly constant peak energy in the EL spectra at various injection currents at the temperature of 300 K, a blue shift has been observed at 190 K. The results suggest that with less non-radiative recombination and thus more carriers in the quantum wells, carrier screening and band filling still prevail in the partially strain relaxed nanorods. Moreover, when the temperature drops to 77 K, the blue shift of both nanorod and planar devices disappears and the optical output power decreases since there are fewer carriers in the quantum wells for radiative recombination.
IEEE Electron Device Letters | 2011
Yu-Hsuan Sun; Yun-Wei Cheng; Szu-Chieh Wang; Ying-Yuan Huang; Chun-Hsiang Chang; Sheng-Chieh Yang; Liang-Yi Chen; Min-Yung Ke; Chi-Kang Li; Yuh-Renn Wu; JianJang Huang
Partial strain relaxation from the light-emitting diode (LED) with surface-textured p-GaN was observed. The textured device possesses less efficiency droop and a higher current level at the efficiency maximum, as compared with the planar one. The results suggest that surface roughening affects not only the external light extraction but also the internal quantum efficiency. Furthermore, the photoluminescent (PL) measurement at low temperature reveals that the percentage increment of the optical power of the textured LED over that of the planar LED becomes lower. In addition to the effect of frozen nonradiative defect states, the PL difference is related to the strain-correlated quantum-confined Stark effect.
Optics Express | 2011
Liang-Yi Chen; H. L. Huang; Chun-Hsiang Chang; Ying-Yuan Huang; Yuh-Renn Wu; JianJang Huang
Strain in the semiconductor light emitting layers has profound effect on the energy band structure and the optical properties of the light emitting diodes (LEDs). Here, we report the fabrication and characterization of GaN nanorod LED arrays. We found that the choice of nanorod passivation materials results in the variation of strain in the InGaN/GaN quantum wells, and thus the corresponding change of light emission properties. The results were further investigated by performing Raman measurement to understand the strain of nanorods with different passivation materials and by calculating the optical transition energy of the devices under the influence of strain-induced deformation potential and the piezoelectric polarization field.
Nanotechnology | 2010
Cheng-Pin Chen; Pei-Hsuan Lin; Yen-Jen Hung; Shao-Shun Hsu; Liang-Yi Chen; Yun-Wei Cheng; Min-Yung Ke; Ying-Yuan Huang; Chun-Hsiang Chang; Ching-Hua Chiu; Hao-Chung Kuo; JianJang Huang
In this work, n-GZO/a:amorphous-Si(i:intrinsic)/p( + )-Si photodiodes are fabricated. We employed a nanosphere lithographic technique to obtain nanoscale patterns on either the a-Si(i) or p( + )-Si surface. As compared with the planar n-GZO/p( + )-Si diode, the devices with nanopatterned a-Si(i) and nanopatterned p( + )-Si substrates show a 32% and 36.2% enhancement of photoresponsivity. Furthermore, the acceptance angle measurement reveals that the nanostructured photodiodes have larger acceptance angles than the planar structure. It also shows that the device with the nanocone structure has a higher acceptance angle than that with the nanorod structure.
IEEE Photonics Technology Letters | 2009
Kun-Mao Pan; Yun-Wei Cheng; Liang-Yi Chen; Ying-Yuan Huang; Min-Yung Ke; Cheng-Pin Chen; Yuh-Renn Wu; JianJang Huang
The polarization behavior of the light-emitting diodes (LEDs) with nanorods surrounding the p-mesa is investigated. The nanorods were fabricated using a natural nanosphere lithography and are intended to diffract laterally propagated light. In the horizontal direction, s-polarized light is dominated since the injected carriers choose to fill up the lowest energy state in a direction parallel to the quantum-well layers. The p/s-polarized ratio starts to increase with the increase of radiated angles and eventually saturates. Since the Bragg diffraction of laterally propagated p-polarized mode by nanorods is more efficient than the s-polarized light, the p/s-ratio of the device with nanorods is higher than that without rods. The p/s-ratio of the LED with nanorods is 1.96 at 90deg, and is 1.52 when the integrating intensity between 0deg and 90deg is considered.
Spie Newsroom | 2011
JianJang Huang; Liang-Yi Chen; Ying-Yuan Huang; Chun-Hsiang Chang
In recent years, 1D nanorods, nanocolumns, and nanowires have been synthesized, while their electrical and material properties have been studied. Among various semiconductor materials employed for nanostructures, gallium nitride (GaN) is one of the most popular choices for solid-state lighting. The sidewall areas of the nanorods that form LED arrays (see Figure 1) give them an increased effective surface. This leads to better external extraction efficiencies. The nanorods may also act as waveguides in which optical modes propagate vertically, which affects their radiation profiles. In addition, the light-emitting efficiency of GaN-based LEDs can be improved by decreasing their defect density. This can be achieved using nanorods with diameters of less than 100nm. There are two approaches to fabricating nanorod-based LED arrays. These include the bottom-up method of growing nanostructures directly on the samples and the alternative, topdown technique of growing planar epi-structures that are subsequently subject to an etching process. Fabrication of nanostructured devices using the latter approach presents several technical and economic challenges. The commercial viability of nanostructures depends on the ability to obtain an affordable nanopattern definition covering large chip sizes. In addition, the nanorod-sidewall damage needs to be repaired. Otherwise, this will lead to sidewall leakage currents and nonradiative recombination, which will seriously degrade device performance. Moreover, since each nanorod forms a vertically stacked p-i-n multilayer structure (see Figure 2)—where the intrinsic (i) part is usually composed of multiple quantum wells—a suitable planarization layer is required to prevent the p-type contact metal from shorting the underlying n-type semiconductor. Our group has developed techniques to address these issues. We established nanosphere lithography, a technique that Figure 1. Scanning-electron-microscopy image of the nanorod array.
Proceedings of SPIE | 2011
Liang-Yi Chen; Chun-Hsiang Chang; Ying-Yuan Huang; JianJang Huang
For InGaN/GaN based nanorod devices using top-down etching process, the optical output power is affected by non-radiative recombination due to sidewall defects (which decrease light output efficiency) and mitigated quantum confined Stark effect (QCSE) due to strain relaxation (which increases internal quantum efficiency). Therefore, the exploration of low-temperature optical behaviors of nanorod light emitting diodes (LEDs) will help identify the correlation between those two factors. In this work, low-temperature EL spectra of InGaN/GaN nanorod arrays was explored and compared with those of planar LEDs. The nanorod LED exhibits a much higher optical output percentage increase when the temperature decreases. The increase is mainly attributed to the increased carriers and a better spatial overlap of electrons and holes in the quantum wells for radiative recombination. Next, while the nanorod array shows nearly constant peak energy with increasing injection currents at the temperature of 300K, the blue shift has been observed at 190K. The results suggest that with more carriers in the quantum wells, carrier screening and band filling still prevail in the partially strain relaxed nanorods. Moreover, when the temperature drops to 77K, the blue shift of both nanorod and planar devices disappears and the optical output power decreases since there are few carriers in the quantum wells for radiative recombination.
quantum electronics and laser science conference | 2009
Liang-Yi Chen; Ying-Yuan Huang; Pei-Hsuan Lin; Min-Yung Ke; JianJang Huang
We have developed a natural lithography method to fabricate nanorod structure. The spin-on glass is used as a space layer to realize the nanorod LED. The strain is released in nanorod structured LED which is indicated by their nearly constant electroluminescent peak wavelength at the injection current range between 25mA and 100mA. Furthermore, a highly concentrated radiation profile is observed from the nanorod LED array. We suggest a light guided concept to explain the narrow radiation phenomena.
asia communications and photonics conference and exhibition | 2009
Yun-Wei Cheng; T. C. Lu; Min-Yung Ke; Kun-Mao Pan; Liang-Yi Chen; Hung-Li Chiang; Ying-Yuan Huang; JianJang Huang
The process of nanosphere lithography was developed and applied to LED epistructure. We demonstrated p-i-n nanorod LED arrays with some specific characteristics. Moreover, LEDs encompassed with self-aligned nanorods are fabricated. Light diffraction behaviors are characterized. The results are explained by photonic crystal effect.