Hsin-Hung Yao’s research while affiliated with King Abdullah University of Science and Technology and other places

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Publications (4)


Precise determination of polarization fields in c-plane GaN/Al x Ga 1- x N/GaN heterostructures with capacitance–voltage-measurements
  • Article

June 2019

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64 Reads

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3 Citations

Japanese Journal of Applied Physics

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Michael Narodovitch

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Figure 1. The cross-sectional schematics and Al composition profiles of Samples A, B, and C with different Al-composition QB grading schemes based on the conventional DUV LED emitting at ~270 nm. Sample A is the reference without grading.
Figure 2(a)-(c) show the band diagrams of Samples A, B, and C at 90 mA. The grading impacts the slope of the QB conduction and valence bands considerably. For the QB conduction band, Sample B shows steeper potential barrier due to the IAC grading as compared to Sample A, while Sample C exhibits flatter barrier due to compensation of existing interface charge by the DAC grading. For the QB valence band, however, Sample B and Sample C manifest flatter and steeper QB valence bands, respectively, which is the opposite behavior to the QB conduction bands. In addition, the QB grading can cause considerable changes to the EBL conduction and valence band offsets ΔEc and ΔEv since the last QB is adjacent to the EBL. ΔEc for electron blocking in Samples A, B, and C are 263, 188, and 243 meV, respectively. Notably, Sample B possesses the smallest ΔEc while those of Samples A and C are similar. ΔEv related to hole injection in Sample A, B, and C are 180, 168, 171 meV, respectively. The hole barriers of Sample B and C are slightly lower than that of Sample A. If the active regions of Samples A, B, and C were the same, it would be straightforward to predict that Sample B would have the largest electron overflow and Sample C would have larger hole concentration than Sample A in the QWs. However, they are not necessarily the case, because the slopes of the QB conduction and valence bands can strongly influence the carrier transport that is the key to the electron containing capability. The change of the QB band slope versus the end composition of the IAC grading can be quantified as shown in the Supplementary Material.
Figure 3. (a) Electron concentration [NQW], (b) hole concentration [PQW], and (c) radiative recombination rate Rrad in the QWs of Samples A, B, and C at 90 mA.
Figure 3(a)-(b) show electron concentration [NQW] and hole concentration [PQW] in the QWs from the band diagram of Figure 2. Overall, [NQW] is larger than [PQW] mainly due to the lower activation energy of electrons than holes. Specifically, Sample C has the highest average [NQW], Sample B has the highest average [PQW], and Sample A shows intermediate behavior. For electrons, the higher [NQW] in Sample C is attributed to the flatter QB conduction band, which is in favor of the electron injection in QWs. For Samples A and B, although Sample B has steeper QB conduction band, electrons can still overcome it due to large mobility, eventually causing [NQW] of Sample B to be just slightly reduced from that of Sample A. More discussion concerning the relationship between the steeper QB conduction band and [NQW] is below related to Figure 5(a). For holes, on the other hand, the highest [PQW] of Sample B is due to flatter QBs and thus lower effective transport barrier. At the same time, the slightly lower [PQW] in Sample C than that of Sample A can be explained by that the lower EBL barrier of Sample C is compensated by the steeper QB and thus higher transport barrier.
Figure 5. (a) Peak carrier concentration and peak radiative recombination rate Rrad in the middle QW of the active region versus the end Al composition of the IAC grading. (b) Electron concentration [Np-AlGaN] in the p-Al0.6Ga0.4N layer with different IAC grading ranges, indicating degree of electron overflow.

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III-nitride Deep UV LED without Electron Blocking Layer
  • Article
  • Full-text available

March 2019

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331 Reads

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47 Citations

IEEE Photonics Journal

AlGaN-based deep UV (DUV) LEDs generally employ a p-type electron blocking layer (EBL) to suppress electron overflow. However, Al-rich III-nitride EBL can result in challenging p-doping and large valence band barrier for hole injection as well as epitaxial complexity. As a result, wall plug efficiency (WPE) can be compromised. Our systematic studies of band diagram and carrier concentration reveal that carrier concentrations in the quantum well (QW) and electron overflow can be significantly impacted because of the slope variation of the QB conduction and valence bands, which in turn influence radiative recombination and optical output power. Remarkably, grading the Al composition from 0.60 to 0.70 for the 12-nm-thick AlGaN QB of the DUV LED without the EBL can lead to 13.5% higher output power and similar level of overflown electron concentration (1×1015/cm3)(\rm \sim 1\times 10^{15} /cm^3) as opposed to the conventional DUV LED with the p-type EBL. This paradigm is significant for the pursuit of higher WPE or shorter emission wavelength for DUV LEDs and lasers, as it provides a new direction for addressing electron overflow and hole injection issues.

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Figure 1. Schematic diagram of the band alignment diagram in the III-N/β-Ga2O3 heterojunction, (Refs. 40,41).
AlN/beta-Ga2O3 based HEMT: a potential pathway to ultimate high power device

January 2019

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892 Reads

Gallium Oxide (Ga2O3) has a huge potential on the power device for its high breakdown filed and good transport properties. beta-Ga2O3 as the thermodynamics stable phase, has been demonstrated to form high electron mobility transistor (HEMT) through delta-doping in the barrier due to its none-polar property. Following the development in III-V HEMT which turns from delta-doping-induced to polarization-induced 2DEG, an alternative method based on III-N materials/beta-Ga2O3 heterostructure is proposed that utilizing the polarization difference on the interface. Further requirements of electric field and conduction band difference show that only nitrogen (N)-polar AlN on beta-Ga2O3 can form the channel and hold large 2DEG concentration on the interface. Compared with conventional metal-polar AlN/GaN HEMT, the proposed N-polar AlN/beta-Ga2O3 HEMT show a much larger 2DEG concentration, the spontaneous-polarization-dominated electric field, better DC output performance, as well as higher breakdown voltage. This study provides a new research approach that shifting from delta-doping-induced to polarization-induced on beta-Ga2O3-based HEMT, which can also be a guideline for community excavating the application potential of Ga2O3.

Citations (3)


... So to be able to compare to experiment we calculate the total-polarization charge for the ternary-alloy heterostructures, using the method outlined in the previous section. For (AlGa)N/GaN, Eq. 12 becomes: 53 Davidsson et al., 54 Arulkumaran et al., 55 Ng et al., 56 Smorchkova et al., 57 Jia et al., 58 Li et al., 59 Jho et al., 60 Lai et al. 61 and Turchinovich et al. 62 Some of these values are modified from field to charge for comparison. Data points in (c) are theoretical values obtained by Caro et al. 17 See text for a thorough discussion. ...

Reference:

Polarization Properties of Wurtzite III-Nitride Alloys Using the Hexagonal Reference Structure
Precise determination of polarization fields in c-plane GaN/Al x Ga 1- x N/GaN heterostructures with capacitance–voltage-measurements
  • Citing Article
  • June 2019

Japanese Journal of Applied Physics

... Our study indicates that reducing the polarization of the electric field is essential to achieve InGaNbased red LEDs with a low operating voltage; and heterojunction polarization engineering is a promising path for future device optimization. For example, we employed an AlN SCL in this study, a polarization-matched MQW in our previous study, and a staggered InGaN QW in Zhao et al.'s work [28,29]. We hope that this paper will increase interest in this topic and aid in the development and commercialization of high-performance InGaN-based red LEDs. ...

Polarization matched c-plane III-nitride quantum well structure
  • Citing Conference Paper
  • March 2019

... However, the p-type doping of EBL has some limitations. Excellent p-type doping is necessary for the EBL to achieve low layer resistance [7]. In addition to, the ineffective Mg-doping leads to very low concentrations of free holes in AlGaN [8,9]. ...

III-nitride Deep UV LED without Electron Blocking Layer

IEEE Photonics Journal