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Density functional model of threshold voltage shifts at High-K/Metal gates 高-K/金属栅极阈值电压偏移的密度泛函模型
IF 1.7 4区 物理与天体物理 Q3 ENGINEERING, ELECTRICAL & ELECTRONIC Pub Date : 2024-05-03 DOI: 10.1016/j.sse.2024.108949
R. Cao , Z. Zhang , Y. Guo , J. Robertson

A density functional analysis of oxide dipole layers used to set the threshold voltages in high-K/metal CMOS gate stacks is given in terms of the band alignments and chemical trends of these component oxide layers. The oxides SrO, La2O3, HfO2 and Al2O3 are found to have similar band gaps and form a ‘staircase’ of band alignments, allowing them to shift the metal electrode Fermi level in both n-type and p-type directions. This analysis supersedes previous largely empirical models based on metal oxide ion densities or electronegativity scales.

根据这些成分氧化物层的能带排列和化学趋势,对用于设置高 K/金属 CMOS 栅极堆栈阈值电压的氧化物偶极层进行了密度泛函分析。研究发现,氧化物 SrO、La2O3、HfO2 和 Al2O3 具有相似的带隙,并形成 "阶梯 "带排列,使它们能够在 n 型和 p 型方向上移动金属电极费米级。这一分析取代了以往主要基于金属氧化物离子密度或电负性标度的经验模型。
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引用次数: 0
Threshold voltage in FD-SOI MOSFETs FD-SOI MOSFET 的阈值电压
IF 1.7 4区 物理与天体物理 Q3 ENGINEERING, ELECTRICAL & ELECTRONIC Pub Date : 2024-04-30 DOI: 10.1016/j.sse.2024.108947
Georges Pananakakis, Gérard Ghibaudo, Sorin Cristoloveanu

The threshold voltage definition and measurement in ultrathin FD-SOI MOS transistors are revisited by comparing theoretical and pragmatic extraction techniques, including novel approaches. The respective merits and limitations of methods based on the monitoring of the potential, mobile charge, gate-to-channel capacitance and drain current are emphasized. Back-gate biasing, thickness-induced quantization, potential fluctuations and surface roughness can enhance the disparity between various extraction methods. The origin of these deviations is clarified.

通过比较理论和实际提取技术(包括新方法),重新审视了超薄 FD-SOI MOS 晶体管中阈值电压的定义和测量。强调了基于监测电位、移动电荷、栅极到沟道电容和漏极电流的方法各自的优点和局限性。后栅偏压、厚度引起的量化、电位波动和表面粗糙度会加剧各种提取方法之间的差异。这些偏差的根源已得到澄清。
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引用次数: 0
Analysis of anomalous C-V behavior for extracting the traps density in the undoped polysilicon with a double-BOX structure 分析反常 C-V 行为以提取双 BOX 结构未掺杂多晶硅中的陷阱密度
IF 1.7 4区 物理与天体物理 Q3 ENGINEERING, ELECTRICAL & ELECTRONIC Pub Date : 2024-04-26 DOI: 10.1016/j.sse.2024.108946
Yang Huang , Yiyi Yan , Massinissa Nabet , Fanyu Liu , Bo Li , Binhong Li , Zhengsheng Han , Sorin Cristoloveanu , Jean-Pierre Raskin

A new Double-BOX structure is introduced to reveal the electrical properties of undoped polysilicon used to enhance the performance of radio frequency SOI substrates. A plateau is clearly observed in the capacitance–voltage (C-V) characteristics, which is due to the influence of the potential barrier formed at the grain boundary. A tangential approximation method based on a three-element circuit model is proposed for correcting the measured C-V curve. With the corrected C-V curve, the effective trap density distribution in polysilicon is determined for each frequency.

为了揭示用于提高射频 SOI 基底面性能的未掺杂多晶硅的电气特性,我们引入了一种新的双 BOX 结构。在电容-电压(C-V)特性中可以清楚地观察到高原现象,这是由于在晶界处形成的势垒的影响。我们提出了一种基于三元素电路模型的切向近似方法,用于修正测量到的 C-V 曲线。利用修正后的 C-V 曲线,可以确定多晶硅中每个频率的有效陷阱密度分布。
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引用次数: 0
Forward leakage currents in GaN p-i-n diodes GaN pi-n 二极管的正向漏电流
IF 1.7 4区 物理与天体物理 Q3 ENGINEERING, ELECTRICAL & ELECTRONIC Pub Date : 2024-04-22 DOI: 10.1016/j.sse.2024.108936
Ao Lu , Xiaofei Pan , Xinjie Zhou , Yang Li , Xiao Wang , Jinping Ao , Dawei Yan

Excessive forward leakage currents in GaN p-i-n diodes were investigated. Traditional diffusion mechanism dominates at VF > 2 V. The effective band gap is derived to be ∼2.21 eV, which is much lower than 3.4 eV and attributed to a band fluctuation caused by dislocations; At 1.35 V < VF < 2 V, a trap-assisted tunneling process becomes important, whose ideality factor is still larger than 4.1 at T = 400 K; Two distinct power-law relationships were observed at lower biases, separated at VF = 0.8 V, whose exponents are extracted to be ∼8 and ∼4, respectively. The behavior is in a good agreement with the space-charge-limited model, featuring an exponentially decaying distribution of trap states below the conduction band.

研究了 GaN pi-n 二极管中过大的正向漏电流。传统的扩散机制在 VF > 2 V 时占主导地位。在 1.35 V < VF < 2 V 时,阱辅助隧穿过程变得重要,其表意系数仍大于 4。在 T = 400 K 时,阱辅助隧道过程变得非常重要,其意念系数仍然大于 4;在 VF = 0.8 V 时,在较低偏压下观察到两个不同的幂律关系,其指数分别为 ∼8 和 ∼4。这种行为与空间电荷限制模型十分吻合,其特点是导带以下的阱态分布呈指数衰减。
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引用次数: 0
Impact of Gate Oxide Thickness on Flicker Noise (1/f) in PDSOI n-channel FETs 栅极氧化物厚度对 PDSOI n 沟道场效应晶体管闪烁噪声 (1/f) 的影响
IF 1.7 4区 物理与天体物理 Q3 ENGINEERING, ELECTRICAL & ELECTRONIC Pub Date : 2024-04-16 DOI: 10.1016/j.sse.2024.108935
Shruti Pathak , Sumreti Gupta , Aarti Rathi , P. Srinivasan , Abhisek Dixit

This work reports the impact of gate oxide thickness on flicker noise (1/f) in 45-nm RFSOI NFET devices. In addition, the effect of finger width scaling on 1/f noise parameters is studied in linear region. The dominant source of 1/f noise is also analyzed. It is observed that thin oxide devices show carrier number fluctuation; however, for thick oxide devices, correlated number-mobility govern the noise. Extracted trap densities using 1/f noise show higher volume trap densities in thin oxide devices. Moreover, trap distribution behavior is analyzed using frequency exponent. Further, GLOBALFOUNDRIES PDK is utilized to model 1/f noise behavior of the devices.

这项研究报告了栅极氧化物厚度对 45 纳米 RFSOI NFET 器件闪烁噪声 (1/f) 的影响。此外,还研究了线性区域中指宽缩放对 1/f 噪声参数的影响。还分析了 1/f 噪声的主要来源。研究发现,薄氧化物器件会出现载流子数量波动;但对于厚氧化物器件,相关的数量-流动性会控制噪声。利用 1/f 噪声提取的陷阱密度显示,薄氧化物器件的体积陷阱密度更高。此外,还利用频率指数分析了陷阱分布行为。此外,还利用 GLOBALFOUNDRIES PDK 对器件的 1/f 噪声行为进行了建模。
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引用次数: 0
Synthesis of α-Fe2O3 nanorod for sensitive and selective detection of the n-butanol 用于灵敏和选择性检测正丁醇的 α-Fe2O3 纳米棒的合成
IF 1.7 4区 物理与天体物理 Q3 ENGINEERING, ELECTRICAL & ELECTRONIC Pub Date : 2024-04-16 DOI: 10.1016/j.sse.2024.108934
Yina Yang , Yufeng Liu , Xiaohong Zheng , Xinfeng Qiao

In different environments, high concentration of n-butanol will have certain harm to the human senses and nervous system, meanwhile the electrochemical sensor limits its widespread use due to its high power consumption, so it is very meaningful to develop a semiconductor n-butanol sensor with low energy consumption. In this paper, α-Fe2O3 nanorods were prepared by one-step hydrothermal method and then assembled into a n-butanol sensor capable of detecting n-butanol, and the effects of two different calcination temperatures on the performance of the sensor were investigated. Due to its higher Fe3+ content, higher oxygen vacancy content and larger specific surface area, S1-250 provided more active sites for gas adsorption, which making the response of S1-250 to 100 ppm n-butanol at 215 °C reached to 88.4. Finally, the effect of the calcination temperature on the sensor and the response mechanism were discussed. This paper offers promising applications for low-energy n-butanol sensors assembled from a single material α −Fe2O3.

在不同的环境中,高浓度的正丁醇会对人的感官和神经系统产生一定的危害,而电化学传感器因耗电量大而限制了其广泛应用,因此开发一种低能耗的半导体正丁醇传感器非常有意义。本文采用一步水热法制备了α-Fe2O3纳米棒,然后将其组装成能够检测正丁醇的正丁醇传感器,并研究了两种不同煅烧温度对传感器性能的影响。由于 S1-250 具有较高的 Fe3+ 含量、较高的氧空位含量和较大的比表面积,为气体吸附提供了更多的活性位点,这使得 S1-250 在 215 ℃ 时对 100 ppm 正丁醇的响应达到了 88.4。最后,还讨论了煅烧温度对传感器的影响和响应机制。本文为由单一材料 α -Fe2O3 组装而成的低能正丁醇传感器提供了广阔的应用前景。
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引用次数: 0
High-performance uniform stepper-based InP double-heterojunction bipolar transistor (DHBT) on a 3-inch InP substrate 基于 3 英寸 InP 基底面的高性能均匀步进式 InP 双兼性双极晶体管 (DHBT)
IF 1.7 4区 物理与天体物理 Q3 ENGINEERING, ELECTRICAL & ELECTRONIC Pub Date : 2024-04-16 DOI: 10.1016/j.sse.2024.108933
Seung Heon Shin , Hyeon-Seok Jeong , Yong-Hyun Kim , Yong-Soo Jeon , Ji-Min Beak , Wan-Soo Park , In-Geun Lee , Jacob Yun , Ted Kim , Jae-Hak Lee , Hyuk-Min Kwon , Dae-Hyun Kim

In this paper, InP Double-Heterojunction Bipolar Transistors (DHBTs) on a 3-inch InP substrate is demonstrated through stepper-based photolithography. The performance of the fabricated InP DHBTs such as DC characteristics, high-frequency characteristics, and uniformity of the 3-inch wafer is investigated to verify the stepper-based fabrication process. To improve the high-frequency characteristics, the self-aligned base-emitter contact is realized by using the high height-to-width ratio and vertical sidewall emitter profile of the Au electroplating process. The fabricated DHBTs with WE = 0.6 μm and LE = 15 μm exhibits current gain (β) = 50 at VCE = 1.0 V and an open-base common-emitter breakdown voltage (BVCEO) of 5.7 V at JC = 0.01 mA/µm2 and 7.5 V at JC = 0.1 mA/µm2, respectively. Moreover, the fabricated DHBTs with WE = 0.6 μm and LE = 15 μm show excellent fT of 244 GHz and fmax of 221 GHz at JC = 4.4 mA/μm2 and VCE = 1.6 V. In order to evaluate the uniformity of the fabricated DHBTs, we measure current gain (β) and high-frequency characteristics with WE = 0.6 μm and LE = 15 μm and the average values and standard deviation of the β, fT, and fmax are β = 49.3 ± 1.9, fT = 241.4 ± 3.8 GHz, and fmax = 221.5 ± 4.0 GHz, respectively. Thanks to the optimized stepper-based fabrication process, the fabricated InP DHBTs exhibit well-balanced high-frequency characteristics and excellent uniformity.

本文通过步进式光刻技术,在 3 英寸 InP 基底面上演示了 InP 双异质结双极晶体管 (DHBT)。研究了所制造的 InP DHBT 的性能,如直流特性、高频特性和 3 英寸晶片的均匀性,以验证步进式制造工艺。为了改善高频特性,利用金电镀工艺的高高宽比和垂直侧壁发射极轮廓实现了自对准基极-发射极接触。制成的 DHBT 的 WE = 0.6 μm 和 LE = 15 μm 在 VCE = 1.0 V 时的电流增益 (β) = 50,在 JC = 0.01 mA/µm2 和 JC = 0.1 mA/µm2 时的开基共发射极击穿电压 (BVCEO) 分别为 5.7 V 和 7.5 V。此外,在 JC = 4.4 mA/µm2 和 VCE = 1.6 V 条件下,WE = 0.6 μm 和 LE = 15 μm 的 DHBT 具有出色的 fT(244 GHz)和 fmax(221 GHz)。β = 49.3 ± 1.9,fT = 241.4 ± 3.8 GHz,fmax = 221.5 ± 4.0 GHz。由于采用了优化的步进式制造工艺,制造出的 InP DHBT 具有均衡的高频特性和出色的均匀性。
{"title":"High-performance uniform stepper-based InP double-heterojunction bipolar transistor (DHBT) on a 3-inch InP substrate","authors":"Seung Heon Shin ,&nbsp;Hyeon-Seok Jeong ,&nbsp;Yong-Hyun Kim ,&nbsp;Yong-Soo Jeon ,&nbsp;Ji-Min Beak ,&nbsp;Wan-Soo Park ,&nbsp;In-Geun Lee ,&nbsp;Jacob Yun ,&nbsp;Ted Kim ,&nbsp;Jae-Hak Lee ,&nbsp;Hyuk-Min Kwon ,&nbsp;Dae-Hyun Kim","doi":"10.1016/j.sse.2024.108933","DOIUrl":"10.1016/j.sse.2024.108933","url":null,"abstract":"<div><p>In this paper, InP Double-Heterojunction Bipolar Transistors (DHBTs) on a 3-inch InP substrate is demonstrated through stepper-based photolithography. The performance of the fabricated InP DHBTs such as DC characteristics, high-frequency characteristics, and uniformity of the 3-inch wafer is investigated to verify the stepper-based fabrication process. To improve the high-frequency characteristics, the self-aligned base-emitter contact is realized by using the high height-to-width ratio and vertical sidewall emitter profile of the Au electroplating process. The fabricated DHBTs with <em>W<sub>E</sub></em> = 0.6 μm and <em>L<sub>E</sub></em> = 15 μm exhibits current gain (<em>β</em>) = 50 at <em>V<sub>CE</sub></em> = 1.0 V and an open-base common-emitter breakdown voltage (<em>BV<sub>CEO</sub></em>) of 5.7 V at <em>J<sub>C</sub></em> = 0.01 mA/µm<sup>2</sup> and 7.5 V at <em>J<sub>C</sub></em> = 0.1 mA/µm<sup>2</sup>, respectively. Moreover, the fabricated DHBTs with <em>W<sub>E</sub></em> = 0.6 μm and <em>L<sub>E</sub></em> = 15 μm show excellent <em>f<sub>T</sub></em> of 244 GHz and <em>f<sub>max</sub></em> of 221 GHz at <em>J<sub>C</sub></em> = 4.4 mA/μm<sup>2</sup> and <em>V<sub>CE</sub></em> = 1.6 V. In order to evaluate the uniformity of the fabricated DHBTs, we measure current gain (<em>β</em>) and high-frequency characteristics with <em>W<sub>E</sub></em> = 0.6 μm and <em>L<sub>E</sub></em> = 15 μm and the average values and standard deviation of <em>the β, f<sub>T</sub></em>, and <em>f<sub>max</sub> are β</em> = 49.3 ± 1.9, <em>f<sub>T</sub></em> = 241.4 ± 3.8 GHz, and <em>f<sub>max</sub></em> = 221.5 ± 4.0 GHz, respectively. Thanks to the optimized stepper-based fabrication process, the fabricated InP DHBTs exhibit well-balanced high-frequency characteristics and excellent uniformity.</p></div>","PeriodicalId":21909,"journal":{"name":"Solid-state Electronics","volume":"217 ","pages":"Article 108933"},"PeriodicalIF":1.7,"publicationDate":"2024-04-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140781826","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
Neural Network-Based prediction for Cross-Temperature induced VT distribution shift in 3D NAND flash memory 基于神经网络的 3D NAND 闪存跨温度诱导 VT 分布偏移预测
IF 1.7 4区 物理与天体物理 Q3 ENGINEERING, ELECTRICAL & ELECTRONIC Pub Date : 2024-04-12 DOI: 10.1016/j.sse.2024.108925
Kyeongrae Cho , Chanyang Park , Hyundong Jang , Hyeok Yun , Seungjoon Eom , Min Sang Park , Rock-Hyun Baek

In this study, a neural network (NN) was proposed for predicting the VT characteristics of NAND flash memories under cross-temperature conditions. The training data were obtained from commercial NAND flash memory chip measurements at various temperatures. The VT distribution shift caused by cross-temperature was accurately predicted by investigating the optimum data dimensions while minimizing the data generation process. Two types of NNs were used to achieve an accurate VT distribution prediction, and each network was optimized using specific parameters based on the data characteristics at various program verify levels. Finally, quantitative and visual evaluations were conducted to verify the performance of the trained NNs. When the program-measured temperature varied from low to high, the NNs achieved mean errors of 1.87%, 1.41% at low and 0.34%, 0.77% at high for the average and width of the VT distribution, respectively. Similarly, when the temperature varied from high to low, the corresponding mean errors were 2.01%, 0.74% at high and 0.23%, 1.59% at low. These findings demonstrate that NNs can minimize the procedures for detecting the VT distribution shift caused by cross-temperature, thereby offering a promising approach to enhance reliability in the presence of such effects.

本研究提出了一种神经网络 (NN),用于预测 NAND 闪存在跨温度条件下的 VT 特性。训练数据来自商用 NAND 闪存芯片在不同温度下的测量结果。在最小化数据生成过程的同时,通过研究最佳数据尺寸,准确预测了交叉温度引起的 VT 分布偏移。为了实现准确的 VT 分布预测,使用了两种类型的 NN,并根据不同程序验证级别的数据特征,使用特定参数对每个网络进行了优化。最后,进行了定量和可视化评估,以验证训练有素的 NN 的性能。当程序测量的温度从低到高变化时,NN 对于 VT 分布的平均值和宽度的平均误差分别为:低时 1.87%、1.41%,高时 0.34%、0.77%。同样,当温度从高到低变化时,相应的平均误差分别为:高为 2.01%、0.74%;低为 0.23%、1.59%。这些研究结果表明,NN 可以最大限度地减少检测交叉温度引起的 VT 分布偏移的程序,从而为在这种效应下提高可靠性提供了一种可行的方法。
{"title":"Neural Network-Based prediction for Cross-Temperature induced VT distribution shift in 3D NAND flash memory","authors":"Kyeongrae Cho ,&nbsp;Chanyang Park ,&nbsp;Hyundong Jang ,&nbsp;Hyeok Yun ,&nbsp;Seungjoon Eom ,&nbsp;Min Sang Park ,&nbsp;Rock-Hyun Baek","doi":"10.1016/j.sse.2024.108925","DOIUrl":"10.1016/j.sse.2024.108925","url":null,"abstract":"<div><p>In this study, a neural network (NN) was proposed for predicting the V<sub>T</sub> characteristics of NAND flash memories under cross-temperature conditions. The training data were obtained from commercial NAND flash memory chip measurements at various temperatures. The V<sub>T</sub> distribution shift caused by cross-temperature was accurately predicted by investigating the optimum data dimensions while minimizing the data generation process. Two types of NNs were used to achieve an accurate V<sub>T</sub> distribution prediction, and each network was optimized using specific parameters based on the data characteristics at various program verify levels. Finally, quantitative and visual evaluations were conducted to verify the performance of the trained NNs. When the program-measured temperature varied from low to high, the NNs achieved mean errors of 1.87%, 1.41% at low and 0.34%, 0.77% at high for the average and width of the V<sub>T</sub> distribution, respectively. Similarly, when the temperature varied from high to low, the corresponding mean errors were 2.01%, 0.74% at high and 0.23%, 1.59% at low. These findings demonstrate that NNs can minimize the procedures for detecting the V<sub>T</sub> distribution shift caused by cross-temperature, thereby offering a promising approach to enhance reliability in the presence of such effects.</p></div>","PeriodicalId":21909,"journal":{"name":"Solid-state Electronics","volume":"217 ","pages":"Article 108925"},"PeriodicalIF":1.7,"publicationDate":"2024-04-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140756730","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
BCl3/Cl2 plasma etching process to fabricate a ferroelectric gate structure for device integration 利用 BCl3/Cl2 等离子体蚀刻工艺制造用于器件集成的铁电栅极结构
IF 1.7 4区 物理与天体物理 Q3 ENGINEERING, ELECTRICAL & ELECTRONIC Pub Date : 2024-04-06 DOI: 10.1016/j.sse.2024.108918
Bohyeon Kang, Sung-min Ahn, Jongseo Park, Jehyun An, Giryun Hong, Beomjoo Ham, Rock-Hyun Baek

Despite the significant potential of ferroelectric devices in overcoming the challenges faced by conventional high-k-based CMOS devices owing to the scaling of CMOS processes, most ferroelectric devices are not implemented in practical circuits yet. For practical application, integrating them into a circuit is essential, and the development of a reliable etching process is crucial for the integration of individual devices into circuits. Therefore, this study proposes a process for etching hafnium zirconium oxide (HZO)-based gate stacks to fabricate a gate structure and integrate HZO-based devices into circuits. First, poly-Si/TiN/HZO/TiN/SiO2 was deposited on a Si substrate and etched via Cl2 and BCl3/Cl2 plasma etchings. Cl2 plasma etching was found to be less effective, whereas BCl3/Cl2 plasma etching exhibited a higher etching rate. The optimal etching time for the BCl3/Cl2 plasma at which the entire stack was successfully removed was 50 s. Furthermore, the optimal ratio of Ar:Cl2:BCl3 that resulted in minimal damage to the Si surface was determined to be 1:1:3. These results led to the successful formation of an HZO-based gate structure and provided the potential to integrate ferroelectric devices into the circuit, thereby enabling their practical utilization.

尽管铁电器件在克服传统基于高 K 值的 CMOS 器件因 CMOS 工艺缩放而面临的挑战方面具有巨大潜力,但大多数铁电器件尚未应用于实际电路中。在实际应用中,将它们集成到电路中至关重要,而开发可靠的蚀刻工艺对于将单个器件集成到电路中至关重要。因此,本研究提出了一种蚀刻基于氧化铪锆(HZO)的栅极堆栈的工艺,以制造栅极结构并将基于 HZO 的器件集成到电路中。首先,在硅衬底上沉积聚硅/TiN/HZO/TiN/SiO2,并通过 Cl2 和 BCl3/Cl2 等离子体蚀刻进行蚀刻。结果发现 Cl2 等离子刻蚀的效果较差,而 BCl3/Cl2 等离子刻蚀的刻蚀率较高。此外,Ar:Cl2:BCl3 的最佳比例为 1:1:3,对硅表面的损害最小。这些结果成功地形成了基于 HZO 的栅极结构,并为将铁电器件集成到电路中提供了可能性,从而实现了铁电器件的实际应用。
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引用次数: 0
Analysis of breakdown voltage for GaN MIS-HEMT with various composite field plate configurations and passivation layers 采用不同复合场板配置和钝化层的 GaN MIS-HEMT 击穿电压分析
IF 1.7 4区 物理与天体物理 Q3 ENGINEERING, ELECTRICAL & ELECTRONIC Pub Date : 2024-04-03 DOI: 10.1016/j.sse.2024.108930
Catherine Langpoklakpam , Yi-Kai Hsiao , Edward Yi Chang , Chun-Hsiung Lin , Hao-Chung Kuo

The effects of different field plate designs on the breakdown voltage of GaN Metal-insulator-semiconductor high electron mobility transistors (MIS-HEMTs) were examined in this study. The study's primary goal was to determine the dependence of breakdown voltage with respective to composite field plate designs using TCAD simulation. For devices featuring only G-FP, with a fixed gate to drain distance of 15 μm and a fixed G-FP to drain distance of 15 μm, the maximum breakdown voltage was achieved 1 μm G-FP. Breakdown voltage trends were also determined for composite field plate configurations, such as adding a source field plate (S-FP) or a drain field plate (D-FP) with a fixed 1 μm G-FP length. A further enhancement in device breakdown performance was demonstrated by employing a novel D-FP structure. A single D-FP improves the breakdown voltage from 1.4 kV (conventional breakdown voltage with 1um G-FP) to 1.6 kV when combined with 1 μm G-FP, while the novel two-step D-FP achieves a breakdown voltage of about 1.7 kV when combined with 1 μm G-FP. We also investigated the influence of high-k dielectric passivation layers on the breakdown voltage. The breakdown voltage of the devices with optimized G-FP can be further improved by using high-k dielectric material as a passivation layer. The thorough investigations contribute to a better understanding of GaN MIS-HEMT breakdown characteristics and prospective pathways for improving their performance via unique field plate designs and superior dielectric materials.

本研究探讨了不同场板设计对氮化镓金属绝缘体-半导体高电子迁移率晶体管(MIS-HEMT)击穿电压的影响。研究的主要目标是利用 TCAD 仿真确定击穿电压与复合场板设计的关系。对于仅采用 G-FP 的器件,栅极到漏极的固定距离为 15 μm,G-FP 到漏极的固定距离为 15 μm,1 μm G-FP 可达到最大击穿电压。此外,还确定了复合场板配置的击穿电压趋势,例如增加一个源场板(S-FP)或一个漏场板(D-FP),G-FP 长度固定为 1 μm。通过采用新型 D-FP 结构,器件的击穿性能得到了进一步提高。当结合 1 μm G-FP 时,单个 D-FP 可将击穿电压从 1.4 kV(使用 1um G-FP 的传统击穿电压)提高到 1.6 kV,而当结合 1 μm G-FP 时,新型两步式 D-FP 可实现约 1.7 kV 的击穿电压。我们还研究了高介电钝化层对击穿电压的影响。通过使用高介电材料作为钝化层,使用优化 G-FP 的器件的击穿电压可以进一步提高。这些深入研究有助于更好地了解 GaN MIS-HEMT 的击穿特性,以及通过独特的场板设计和优质介电材料提高其性能的前景。
{"title":"Analysis of breakdown voltage for GaN MIS-HEMT with various composite field plate configurations and passivation layers","authors":"Catherine Langpoklakpam ,&nbsp;Yi-Kai Hsiao ,&nbsp;Edward Yi Chang ,&nbsp;Chun-Hsiung Lin ,&nbsp;Hao-Chung Kuo","doi":"10.1016/j.sse.2024.108930","DOIUrl":"https://doi.org/10.1016/j.sse.2024.108930","url":null,"abstract":"<div><p>The effects of different field plate designs on the breakdown voltage of GaN Metal-insulator-semiconductor high electron mobility transistors (MIS-HEMTs) were examined in this study. The study's primary goal was to determine the dependence of breakdown voltage with respective to composite field plate designs using TCAD simulation. For devices featuring only G-FP, with a fixed gate to drain distance of 15 μm and a fixed G-FP to drain distance of 15 μm, the maximum breakdown voltage was achieved 1 μm G-FP. Breakdown voltage trends were also determined for composite field plate configurations, such as adding a source field plate (S-FP) or a drain field plate (D-FP) with a fixed 1 μm G-FP length. A further enhancement in device breakdown performance was demonstrated by employing a novel D-FP structure. A single D-FP improves the breakdown voltage from 1.4 kV (conventional breakdown voltage with 1um G-FP) to 1.6 kV when combined with 1 μm G-FP, while the novel two-step D-FP achieves a breakdown voltage of about 1.7 kV when combined with 1 μm G-FP. We also investigated the influence of high-k dielectric passivation layers on the breakdown voltage. The breakdown voltage of the devices with optimized G-FP can be further improved by using high-k dielectric material as a passivation layer. The thorough investigations contribute to a better understanding of GaN MIS-HEMT breakdown characteristics and prospective pathways for improving their performance via unique field plate designs and superior dielectric materials.</p></div>","PeriodicalId":21909,"journal":{"name":"Solid-state Electronics","volume":"216 ","pages":"Article 108930"},"PeriodicalIF":1.7,"publicationDate":"2024-04-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140557630","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
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Solid-state Electronics
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