Feras AlQatari’s research while affiliated with King Abdullah University of Science and Technology and other places

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Publications (29)


Advanced Semiconductor Laboratory, Thuwal 23955-6900
  • Poster

October 2024

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19 Reads

Zahrah Alnakhli

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Zhiyuan Liu

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Feras Alqatari

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This work investigates the impact of the Silicon (Si) loading effect induced by Deep Reactive Ion Etching (DRIE) on UV-nanoimprint lithography (NIL) patterning of nanofeatures. Silicon was chosen for its known stiffness, ability to achieve very small pattern sizes down to 6 nm with a high aspect ratio, and cost-effectiveness. However, creating a stamp for nanoimprint lithography with complex patterns presents challenges due to the silicon loading problem. Silicon molds, patterned with metasurface features of varying widths from 270 nm to 60 nm, were analyzed using Focused Ion Beam Scanning Electron Microscopy (FIB-SEM) and Atomic Force Microscopy (AFM). The Si loading effect, characterized by variations in feature depth, showed that smaller features etch more slowly due to difficulties in etchant penetration and byproduct diffusion. Silicon's excellent etching properties and ability to maintain feature integrity at sub-10 nm scales make it an ideal choice for NIL despite these challenges. Our results are crucial for advancing NIL in commercial applications, ensuring high-quality pattern transfer for diverse nanostructures. Figure 4. Optical setup used to characterize the optical behavior of the NIL-fabricated metalens. The setup includes a laser source, a series of lenses, and a camera. Images of the focal point were obtained and analyzed to study the intensity distribution. Each image corresponds to a different lens, highlighting the focal point characteristics. METALENS DESIGN METHOD-10-5 0 5 10 0.0 0.5 1.0 Normalized Intensity (a.u.) x (µm) 0°0 .460mm Metalens FDTD Results Unit-Cell RESULTS AND DISCUSSION [1]. Baracu, A., et al; Silicon Metalens Fabrication from Electron Beam to UV-Nanoimprint Lithography. Nanomaterials, 11(9), pp.2329-2329. [2].. Alnakhli, Z., et al., UV-assisted nanoimprint lithography: the impact of the loading effect in silicon on nanoscale patterns of metalens. Nanoscale Advances, 2024. 6(11): p. 2954-2967. Figure 3. Effects of silicon loading on metalens fabrication. The silicon master mold, processed by Bosch-DRIE, shows that minimal silicon loading ensures successful metalens creation. AFM characterization and precise removal of the photoresist residual layer are critical to the process. Significant silicon loading and improper residual layer removal hinder successful fabrication. VS We utilized UV-assisted NIL to fabricate metalenses, beginning with the creation of a silicon master mold. The process included: Master Mold Creation: Patterning of silicon with metasurface features using DRIE. Stamp Mold Preparation: Using a glass plate and prepolymer mixture cured with UV light to form the stamp mold. Our study revealed that the Si loading effect significantly impacts the etching uniformity in DRIE. Specifically, areas with higher silicon loading exhibited slower etch rates and increased byproduct accumulation, leading to variations in feature depth. This finding emphasizes the need for optimized etching parameters to achieve uniform nanostructures. Optimizing DRIE parameters for silicon master molds is crucial for achieving high-quality NIL patterning. Our findings provide valuable insights into controlling the Si loading effect, paving the way for advanced nanofabrication techniques in commercial applications. REFERENCES




Figure 1: Illustration of the metasurface structure illustrating a special arrangement of rectangular with varying length and (b) Scanning electron microscopy (SEM) im age of fabricated NIL master mold with metasurface pattern on Silicon.
Figure 2: UV-NIL Metasurface Fabrication Process Overview. (a) Master Fabrication: Steps involve 1. Silicon wafer cleaning and preparation; 2. Spin-coating with photoresist; 3. Electron beam exposure; 4. Wafer development; 5. Metal deposition and lift-off of the photoresist to transfer the metasurface pattern, followed by 6. Silicon Bosch Deep Reactive Ion Etching Process using SF₆ and C₄F₈, and a final chemical etching step to remove the metal layer completely. So, holes are obtained (b) Stamp Fabrication: Steps include 1. Prepolymer mixture preparation; 2. Degassing to remove trapped air; 3. Cleaning and preparing the glass substrate; 4. Dropping the soft stamp prepolymer mixture; 5. Placing the master mold on stamp mold; 6. UV-curing the stamp material; 7. Removing the stamp from the master mold. (c) Metasurface Fabrication by UV-NIL: Involves 1. TiO₂ deposition by EBE followed by surface preparation; 2. Spin coating with UV photoresist; 3. Aligning the stamp; 4. UV exposure for resist curing; 5. O₂ plasma strip to remove unwanted photoresist residuals post-stamp detachment; 6. Masking material deposition followed by lift-off; 7. RIE process and chemical removal of the masking layer.
Figure 4: AFM top view images showing a comparison between different geometries after the fabrication of the stamps mold: (a) the right part is a top view for stamp S-MM_1 showing the fully replicated pattern using master (MM-1), and the left Part shows the observed height for all pattern pillars. (b) Stamp mold (S-MM-2) with slightly less pillars height difference. (c) Stamp mold (S-MM-3) with too less pillars height difference. (d) Comparison summary between the width of the square holes in the master mold (MM-3) and the corresponding pillars of stamp mold (S-MM-3).
Figure 5: SEM and AFM images demonstrating the metasurface structure transfer via UV-NIL using diverse stamp molds. (a) SEM shows a 200 nm-thick photoresist layer deposited on a TiO 2 thin film, patterned utilizing stamp S-MM-1. (b) An SEM image captures the 200 nm photoresist structure following the NIL process with stamp S-MM-2. (c) SEM illustrates a replicated 2D nanosquare array achieved through NIL with stamp S-MM-3. (d) A 3D AFM image reveals the successful pattern transformation obtained with stamp S-MM-3. (e) AFM provides a detailed view of the 2D nanosquare array created by stamp MM-3, including a height profile that highlights the topographical contrast within a 5 μm × 5 μm area, showcasing the distinctions between peaks and valleys.
Figure 6: Top-view SEM images of the metasurface via UV-NIL and ICP-RIE etch process for TiO2 thin film after "photoresist metasurace " structure was dry etched by RIE to remove photoresist residual layer. (a) Side-View SEM image of the fabricated metasurface after residual layer removal using RIE process for 20 (sec). (b) Top-View SEM image of as a result of photoresist over-etched for 40 (sec). (C) Top-View SEM image of metasurface after residual layer removal for 30 (sec). (d) Zoom in-View SEM of the nanopattrned metasurface via UV-NIL and RIE method of the photoresist for 30 (sec).

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UV-Assisted Nanoimprint Lithography: The Impact of Loading Effect in Silicon on Nanoscale Pattern of Metalens
  • Article
  • Full-text available

April 2024

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81 Reads

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4 Citations

This work studies the impact of the silicon (Si) loading effect induced by deep reactive ion etching (DRIE) of silicon master molds on the UV-nanoimprint lithography (NIL) patterning of nanofeatures. The silicon molds were patterned with metasurface features with widths varying from 270 to 60 nm. This effect was studied by focus ion beam scanning electron microscopy (FIB-SEM) and atomic force microscopy (AFM). The Si loading etching effect is characterized by the variation of pattern feature depth concerning feature sizes because smaller features tend to etch more slowly than larger ones due to etchants being more difficult to pass through the smaller hole and byproducts being harder to diffuse out too. Thus, the NIL results obtained from the Si master mold contain different pattern geometries concerning pattern quality and residual photoresist layer thickness. The obtained results are pivotal for NIL for fabricating devices with various geometrical nanostructures as the research field moves towards commercial applications.

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Polarization-matching and carrier confinement in III-nitride deep-ultraviolet light-emitting diodes

November 2023

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22 Reads

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1 Citation

The polarization-induced quantum confined Stark effect has been recognized as a significant factor contributing to the Internal Quantum Efficiency (IQE) droop in light-emitting diodes (LEDs). This study focuses on the design of LEDs by investigating the InAlN/AlGaN interface. By incorporating InAlN quantum wells, a polarization-matched (PM) multi-quantum well (MQW) LED architecture was developed. While the flat conduction and valence bands on PM MQWs indicate an improved recombination rate, it is crucial to examine the impact on IQE, considering carrier confinement and injection efficiency influenced by the band offsets. This paper presents a numerical analysis comparing two LEDs emitting at 245 and 275 nm, respectively. The results demonstrate that the PM LED operating at 275 nm exhibits enhanced performance, benefiting from high probability density overlap. Conversely, the PM LED emitting at 245 nm demonstrates poor confinement, resulting in an overall low performance, regardless of polarization matching.


(a) Flat band model of type-II alignment of materials X and Y showing the relationship between the quantities in equation (1). (b) Schematic showing energy levels typically measured when aligning bands using equation (2). Notice the different Fermi levels (E F) for each sample. (c) The resulting VBO (in red) when the energy levels are aligned. The Fermi level of the interface sample is highlighted as an effective reference energy. (d) The valence energies of the interface sample can be measured for alignment using equation (3). The arrows in (b)–(d) point in the direction of increasing binding energy.
(a) 2θ-ω XRD scan showing the (002) peaks for AlN and BGaN. The AlN double-peak feature is due to x-rays containing both Kα 1 and Kα 2 emissions. The inset in (a) shows the calculated 2θ at different compositions based on linear interpolation of the indicated lattice constants. (b) Tauc plot and responsivity spectrum of the BGaN film showing similar bandgap values. The inset in (b) is a schematic of the interdigitated MSM photodetector (not to scale). The thickness is 120 nm in both (a) and (b).
(a) High resolution dark field STEM image near the BGaN/AlN interface. (b) and (c) The smoothed EELS spectra of AlN and BGaN, respectively, with the bandgaps highlighted by the dotted lines. The window of points for the smoothing process is 10 (equal to 50 meV).
(a) Schematic of the samples needed for the alignment of BGaN/AlN using the method in equation (2). The AlN layers are part of 1.5 µm thick templates. (b) Schematic of the BGaN/GaN sample. The GaN regrowth layer is lightly Si doped (∼10¹⁷/cm³), and the GaN underlayer is a 2.5 µm thick template. (c) The measured XPS spectra of the samples in (a). (d) The measured spectrum of the sample in (b) in the low binding energy range. The dashed lines in (d) correspond to the valence band edges of the GaN and BGaN layers withing the sample.
(a) Histogram representing the results of our statistical method for finding the VBM of BGaN and GaN layers from the low binding energy region of the XPS spectrum. (b) Summary of the alignments of B0.097Ga0.903N with AlN and GaN. The literature accepted values of the gaps of GaN and AlN are used to find the CBO values with BGaN.
Detailed band alignment of high-B-composition BGaN with GaN and AlN

June 2023

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106 Reads

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2 Citations

The electronic structure of B 0.097 Ga 0.903 N was determined by examining its bandgap and valence band offset (VBO) in detail. The BGaN sample was grown using a horizontal reactor metalorganic chemical vapor deposition. For bandgap determination, three different techniques were utilized yielding similar results, which are: UV-Vis spectroscopy, Schottky photodiodes, and electron energy-loss spectroscopy. The bandgap was determined to be ~3.55 eV. For measuring the VBO, the valence edges and the core levels of Al 2s and Ga 2p were measured using x-ray photoelectron spectroscopy (XPS). The valence edges were then fitted and processed along with the core levels using the standard Kraut method for VBO determination with AlN. The BGaN/AlN alignment was found to be -1.1 ± 0.1 eV. Due to core level interference between GaN and BGaN, the Kraut method fails to provide precise VBO for this heterojunction. Therefore, a different technique is devised to analyze the measured XPS data which utilizes the alignment of the Fermi levels of the BGaN and GaN layers when in contact. Statistical analysis was used to determine the BGaN/GaN alignment with decent precision. The value was found to be -0.3 ± 0.1 eV.


FIG. 1. Cross-sectional view of (a) the recessed gate. 3D schematics of (b) nonrecessed and (c) recessed gates. (d) Fabrication process flow. (e) Scanning electron microscopy (SEM) top view of the b-Ga 2 O 3 MOSFETs.
FIG. 2. b-Ga 2 O 3 film characterization: (a) x-ray diffraction and (b) atomic force microscopy (AFM) image. AFM image of (c) the recess profile, (c-inset) recess depth, and(d) surface topography (inside recess). Scanning transmission electron microscopy (STEM) image of (e) the sidewall (highlighting a recess depth of 11 nm) and (f) the bottom facet of gate recess.
FIG. 3. Transfer (logarithmic and linear) and output characteristics, respectively, (a) and (b) non-recessed and (c) and (d) recessed MOSFETs at different drainsource (V DS ) and gate-source voltages (V GS ). Linear transfer behavior is at V DS ¼ 5 V, shown in (a) and (c).
FIG. 4. Hysteresis transfer behavior of MOSFETs (in the logarithmic scale): (a) non-recessed and (b) recessed gate. (c) Cross-sectional schematic of depletion depths explaining the mechanism of E-mode operation of recessed MOSFETs. (All numbers are in nm.)
FIG. 5. Depletion load n-type metal oxide semiconductor (NMOS) inverter: (a) top microscopic view and (b) circuit diagram. Electrical characterization of the NMOS inverter: (c) voltage transfer curve and (d) voltage gain.
Monolithic β -Ga 2 O 3 NMOS IC based on heteroepitaxial E-mode MOSFETs

April 2023

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672 Reads

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13 Citations

In this Letter, we report on a monolithically integrated β-Ga 2 O 3 NMOS inverter integrated circuit (IC) based on heteroepitaxial enhancement mode (E-mode) β-Ga 2 O 3 metal-oxide-semiconductor field-effect transistors on low-cost sapphire substrates. A gate recess technique was employed to deplete the channel for E-mode operation. The E-mode devices showed an on-off ratio of ∼10 ⁵ with a threshold voltage of 3 V. In comparison, control devices without the gate recess exhibited a depletion mode (D-mode) with a threshold voltage of [Formula: see text]3.8 V. Furthermore, depletion-load NMOS inverter ICs were fabricated by monolithically integrating D- and E-mode transistors on the same substrate. These NMOS ICs demonstrated inverter logic operation with a voltage gain of 2.5 at V DD = 9 V, comparable with recent GaN and other wide-bandgap semiconductor-based inverters. This work lays the foundation for heteroepitaxial low-cost and scalable β-Ga 2 O 3 ICs for monolithic integration with (ultra)wide bandgap Ga 2 O 3 power devices.


Piezoelectric Sensors Operating at Very High Temperatures and in Extreme Environments Made of Flexible Ultrawide‐Bandgap Single‐Crystalline AlN Thin Films (Adv. Funct. Mater. 10/2023)

March 2023

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59 Reads

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2 Citations

Piezoelectric Sensor In article number 2212538, Jae‐Hyun Ryou and co‐workers develop a highly sensitive and mechanically flexible piezoelectric sensor using an ultrawide‐bandgap single‐crystalline AlN semiconductor thin film that can operate at higher than 900 °C. The operation temperature is believed to be amongst the highest for pressure sensors, and the inherent properties of AlN indicate that this approach offers a new solution for sensing in extreme environments often faced in current and next‐generation energy, transportation, and defense applications.


Piezoelectric Sensors Operating at Very High Temperatures and in Extreme Environments Made of Flexible Ultrawide‐Bandgap Single‐Crystalline AlN Thin Films

December 2022

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363 Reads

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34 Citations

Extreme environments are often faced in energy, transportation, aerospace, and defense applications and pose a technical challenge in sensing. Piezoelectric sensor based on single‐crystalline AlN transducers is developed to address this challenge. The pressure sensor shows high sensitivities of 0.4–0.5 mV per psi up to 900 °C and output voltages from 73.3 to 143.2 mV for input gas pressure range of 50 to 200 psi at 800 °C. The sensitivity and output voltage also exhibit the dependence on temperature due to two origins. A decrease in elastic modulus (Young's modulus) of the diaphragm slightly enhances the sensitivity and the generation of free carriers degrades the voltage output beyond 800 °C, which also matches with theoretical estimation. The performance characteristics of the sensor are also compared with polycrystalline AlN and single‐crystalline GaN thin films to investigate the importance of single crystallinity on the piezoelectric effect and bandgap energy‐related free carrier generation in piezoelectric devices for high‐temperature operation. The operation of the sensor at 900 °C is amongst the highest for pressure sensors and the inherent properties of AlN including chemical and thermal stability and radiation resistance indicate this approach offers a new solution for sensing in extreme environments.


Origin of interfacial charges of Al2O3/Si and Al2O3/GaN heterogeneous heterostructures

October 2022

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40 Reads

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15 Citations

Applied Surface Science

Al2O3 is a broadly employed dielectric and significant interfacial charges occur at Al2O3/semiconductor interfaces. However, the charge origin is often unclear that severely impacts device engineering and design. Al2O3/Si and Al2O3/GaN are two of the most common heterogeneous heterostructures (H2s) for many crucial devices including GaN transistors and Si solar cells. While negative charges are extensively observed in Al2O3/Si, positive charges exist in Al2O3/GaN, both of which are not well understood. In this study, we performed in-depth interfacial studies of the Al2O3/Si and Al2O3/GaN H2s to clarify the origin of the interfacial charges. Stoichiometry deviations were found at the interfaces of the two H2s where Al surpasses O for Al2O3/GaN, whereas O dominates at the Al2O3/Si interface. Therefore, we propose that the different interfacial charges are caused by nonstoichiometry atomic ratios of Al2O3 at the interface. The study indicates the important role of the semiconductor surface on the device performance, provide a deep understanding on the origin of interfacial charges at the insulator-semiconductor interfaces.


Citations (18)


... However, high-resolution technology is required for the manufacturing of the template (mold). Thermal and UV embossing are components of traditional NIL [64]. Lower-viscosity materials with elevated temperatures are used in thermal embossing. ...

Reference:

Metasurfaces in Optical Biosensing: Revolutionizing Detection Techniques and Shaping the Future
UV-Assisted Nanoimprint Lithography: The Impact of Loading Effect in Silicon on Nanoscale Pattern of Metalens

... However, part of these interface charges can be screened by electrons and holes from trap states and external charges [20], which originate from outside the simulated region. In lieu of a full device transport simulation, we model this as a reduction of the effective polarization charge by a factor p eff which depends on operation mode (electrical [21]- [23] vs. optical pumping [20], [24]). ...

Polarization-matching and carrier confinement in III-nitride deep-ultraviolet light-emitting diodes
  • Citing Article
  • November 2023

... Related to photonics research, Professor Xiaohang Li's Advanced Semiconductor Laboratory [https://cemse.kaust.edu.sa/semiconductor] focused on the formation of ultrawide bandgap semiconductor for ultraviolet optoelectronic devices, notably in group-III-nitrides and group-III-oxides deep ultraviolet light-emitters [126], boron-containing nitrides [127], and Ga2O3 membrane [128]. The team has also reported 5 > REPLACE THIS LINE WITH YOUR MANUSCRIPT ID NUMBER (DOUBLE-CLICK HERE TO EDIT) < significant work in semiconductor heterostructures design and deep-ultraviolet photodetectors [129], [130]. ...

Detailed band alignment of high-B-composition BGaN with GaN and AlN

... ( 201) orientated Ga 2 O 3 is also a widely employed and investigated substrate in developing high-power electronics and solar-blind photonics. 11,30 This is due to its native substrate having a much lower cost and availability of a larger scale wafer compared with (010) Ga 2 O 3 . To directly determine the band offset of p-GaAs/Ga 2 O 3 ( 201) B-C junction, the n-AlGaAs/p-GaAs E-B heterostructure is grafted onto a Ga 2 O 3 ( 201) substrate, and the interface is directly measured by thinning down the E-B layer until detecting the interface between GaAs and Ga 2 O 3 ( 201). ...

Monolithic β -Ga 2 O 3 NMOS IC based on heteroepitaxial E-mode MOSFETs

... However, a piezoresistive 99 sensing mechanism is more immune to radiation compared 100 to other sensing mechanisms [23], [24]. Consequently, the 101 use of piezoresistive sensing-based sensors in extreme radia-102 tion environments has significantly increased [25], [26], [27]. ...

Piezoelectric Sensors Operating at Very High Temperatures and in Extreme Environments Made of Flexible Ultrawide‐Bandgap Single‐Crystalline AlN Thin Films

... Zhao et al analyzed thermal blistering at the Al 2 O 3 /Si, attributing it to hydrogen impurities from incomplete ALD and the gas barrier nature of Al 2 O 3 films, which can be reduced by three means [27]. Furthermore, Wang et al studied the sources of negative charges at the Al 2 O 3 /Si, identifying nonstoichiometric atomic ratios as the primary cause [28]. Kim and Agrawal et al have proposed using SiO 2 as an interfacial buffer layer and (NH 4 ) 2 S for passivation to effectively to tackle the high defect density at Al 2 O 3 /Si [29,30]. ...

Origin of interfacial charges of Al2O3/Si and Al2O3/GaN heterogeneous heterostructures
  • Citing Article
  • October 2022

Applied Surface Science

... The limited solubility of boron in the lattice makes it challenging to incorporate into III-nitride. This can result in cluster formation or phase separation, which deteriorates the material's optical and structural qualities [23][24][25]. However, these BNcontaining layers can be grown practically using metal-organic chemical vapor deposition and other epitaxial layer growing techniques [26,27]. ...

Demonstration of MOCVD-grown BGaN with over 10% boron composition

... Consequently, the significance of soliton waves and other applied topics are growing across multiple domains, including account service network [65], an improved particle swarm optimization algorithm [66], multilegged robot smooth motion [67], impulse switched singular systems [68], a fuzzy logic path planning algorithm [69], a lightweight method for intelligent detection [70], the nonlinear descriptor systems [71], the generalized matrix completion [72], accurate circle detection algorithm [73], the tangential force effect on electro-magnetic vibration [74], conformal micro/nano-scale [75], an improved back propagation neural network method [76], virtual multiple quasi-notch-flters impedance [77], deep learning method [78,79], the nonlinear optics [80], a multimodal hybrid parallel network intrusion [81], the network traffic detection model [82], a hydroxyethyl group [83], a novel fiber-supported superbase [84], the optimization strategies from the data, network [85], excellent microwave absorption [86], a machine learning study on superlattice electron [87], low resistance asymmetric by machine learning [88], the maturation of engineered cardiac tissues [89], the magnetic porous media [90], a neural architecture and multiscale attention [91]. A few of the latest findings on soliton waves in different fields have been examined in [92][93][94][95]. Through gaining a more profound comprehension of soliton waves, scientists can progress these domains and investigate novel applications. ...

Origin of Interfacial Charges of Al2o3/Si and Al2o3/Gan Heterogeneous Heterostructures
  • Citing Article
  • January 2022

SSRN Electronic Journal

... Due to the non-centrosymmetric crystal structure of wurtzite III-nitride, distinguishable gallium and nitrogen polarities with opposite, spontaneous, and piezoelectric polarizations have been revealed along the c-axis of GaN thin films [11,12]. In the pursuit of high-performance GaN electronic devices over the past decade, Ga-polar thin films have been widely utilized as a mature growth technology with a smoother surface morphology and better crystalline quality. ...

Polarization modulation of 2DEG toward plasma-damage-free GaN HEMT isolation

... 层大气的物理化学过程,为航空航天活动提供数据支持[75] 。 在环境监测方面,某些特殊的大气现象或者污染物 会在日盲紫外波段有特征辐射。 β-Ga 2 O 3 日盲紫外探测器可以对这些微弱的信号进行探测,辅助监测大气中的 臭氧空洞、火山活动等情况[76] 。 然而,β-Ga 2 O 3 在日盲紫外探测器的应用也面临一些挑战。 例如,材料的生长工 艺还不够成熟,导致晶体质量有待提高;探测器的制备工艺复杂,使制造成本较高[77] 。 但随着材料科学和半导 体技术的不断发展,这些问题有望逐步得到解决,β-Ga 2 O 3 在日盲紫外探测器中的应用前景十分广阔。 Si) 或砷化镓( GaAs) 器件由于击穿电场强度较低,在处理高功率信号时容易达到极限。 例如,在相同 的器件尺寸下,Si 基功率放大器可能在功率达到一定程度时就会发生击穿现象,而氧化镓器件由于其高击 穿电场强度,可以承受更高的电压,从而能够将射频信号放大到更高的功率。 理论计算表明,在毫米波频段, 氧化镓功率放大器能够实现数瓦甚至数十瓦的功率输出,这是传统材料难以企及的。 在卫星通信的高功率 发射机中,信号需要远距离传输,要求发射机具有高功率输出能力。 氧化镓射频器件能够满足这一要求,在 保证信号强度的同时,减少信号在传输过程中的衰减,提高通信的可靠性。 氧化镓具有合适的电子迁移率, 并且材料结构使其在高频下具有较低的寄生电容和电感。 在射频信号处理中,寄生电容和电感会影响信号 的传输速度和带宽。 对于 5G 及未来的 6G 通信技术,射频器件需要在毫米波频段(30~300 GHz) 工作。 在 这个频段下,传统材料的寄生参数会对信号产生较大的干扰。 在过去的几十年里,许多研究人员探索了 β-Ga 2 O 3 在射频应用中的适用性 [78-84] 。 Green 等 [78] 首次演示了 β-Ga 2 O 3 MOSFET 用于射频应用。 在这项工作中,观察到跨导 g m (约 21 mS / mm)和截止频率 f T (约 3. 3 GHz)的 高值,还展示了 0. 8 GHz 下的大信号连续波 RF 分析。 输出功率 P OUT ≈0. 23 W / mm, 功率增益G P ≈5. 1 dB和 功率附加效应 PAE≈6. ...

Quasi-Epitaxial Growth of β‑Ga2O3‑Coated Wide Band Gap Semiconductor Tape for Flexible UV Photodetectors
  • Citing Article
  • January 2022

ACS Applied Materials & Interfaces