高分辨紫外电子轰击互补金属氧化物半导体器件的实验研究

基于真空紫外光电阴极和背照式互补金属氧化物半导体(CMOS)图像传感器研制了紫外光响应的电子轰击CMOS(EBCMOS)器件,实现了EBCMOS器件在40 mlx光照度环境下的高分辨探测,电子图像灰度随电子能量的变化呈现出极好的线性关系.对器件成像分辨率测试的结果表明,在电场强度为5000 V/mm时,器件的空间分辨率可以达到25 lp/mm,与国际相关报道水平相当.研制的EBCMOS器件可直接在紫外弱光探测领域应用,如天文观察、高能物理、遥感测绘等,同时也可为下一步研制可见光和近红外敏感的EBCMOS器件提供参考.     

质子辐射下互补金属氧化物半导体有源像素传感器暗信号退化机理研究

对某国产0.5 μm工艺制造的互补金属氧化物半导体有源像素传感器进行了10 MeV质子辐射试验, 当辐射注量达到预定注量点时, 采用离线的测试方法, 定量测试了器件暗信号的变化情况. 试验结果表明, 随着辐射注量的增加暗信号迅速增大. 采用MULASSIS (multi-layered shielding simulation software)软件计算了电离损伤剂量和位移损伤剂量, 在与γ辐射试验数据对比的基础上, 结合器件结构和工艺参数, 建立了分离质子辐射引起的电离效应和位移效应理论模型, 深入分析了器件暗信号的退化机理. 研究结果表明, 对该国产器件而言, 电离效应导致的表面暗信号和位移效应导致的体暗信号对整个器件暗信号退化的贡献大致相当.     

基于4晶体管像素结构的互补金属氧化物半导体图像传感器总剂量辐射效应研究

对基于4晶体管像素结构互补金属氧化物半导体图像传感器的电离总剂量效应进行了研究,着重分析了器件的满阱容量和暗电流随总剂量退化的物理机理.实验的总剂量为200 krad(Si),测试点分别为30 krad(Si),100 krad(Si),150 krad(Si)和200 krad(Si),剂量率为50 rad(Si)/s.实验结果发现随着辐照总剂量的增加,器件的满阱容量下降并且暗电流显著增加.其中辐照使得传输门沟道掺杂分布发生改变是满阱容量下降的主要原因,而暗电流退化则主要来自于浅槽隔离界面缺陷产生电流和传输门-光电二极管交叠区产生电流.实验还表明样品器件的转换增益在辐照前后未发生明显变化,并且与3晶体管像素结构不同,4晶体管像素结构的互补金属氧化物半导体图像传感器没有显著的总剂量辐照偏置效应.     

Speckles in laser Doppler perfusion imaging

We report on the quantitative influence of speckles in laser Doppler perfusion imaging. The influence of speckles on the signal amplitude and on the Doppler spectrum is demonstrated experimentally for particle suspensions with different scattering levels and various beam widths. It is shown that the type of tissue affects the instrumental response through the effect of lateral light diffusion on the number of speckles involved in the detection process. These effects are largest for narrow beams.     

Bistability in a complementary metal oxide semiconductor inverter circuit

Radiofrequency signals can disrupt the operation of low frequency circuits. A digital inverter circuit would seem to be immune to such disruption, because its output state usually jumps abruptly between 0 and 5 V. Nevertheless, when driven with a high frequency signal, the inverter can have two coexisting stable states (which are not at 0 and 5 V). Slow switching between these states (by changing the rf signal) will produce a low frequency signal. I demonstrate the bistability in a circuit experiment and in a simple model of the circuit.     

Low on-resistance high-voltage lateral double-diffused metal oxide semiconductor with a buried improved super-junction layer

A novel low specific on-resistance （Ron,sp） lateral double-diffused metal oxide semiconductor （LDMOS） with a buried improved super-junction （BISJ） layer is proposed. A super-junction layer is buried in the drift region and the P pillar is split into two parts with different doping concentrations. Firstly, the buried super-junction layer causes the multiple-direction assisted depletion effect. The drift region doping concentration of the BISJ LDMOS is therefore much higher than that of the conventional LDMOS. Secondly, the buried super-junction layer provides a bulk low on-resistance path. Both of them reduce Ron,sp greatly. Thirdly, the electric field modulation effect of the new electric field peak introduced by the step doped P pillar improves the breakdown voltage （BV）. The BISJ LDMOS exhibits a BV of 300 V and Ron,sp of 8.08 mΩ·cm2 which increases BV by 35% and reduces Ron,sp by 60% compared with those of a conventional LDMOS with a drift length of 15 μm, respectively.     

Capacitance analysis for a metal–insulator– semiconductor structure with an ultra-thin oxide layer

Applied Physics A - We have studied theoretically the capacitance characteristics of a metal–insulator–semiconductor structure with an ultra-thin oxide layer by self-consistently...     

Laser Doppler imaging through tissues phantoms by using self-mixing interferometry with a laser diode

Laser Doppler imaging has been widely used for the evaluation of cutaneous blood flow. We report on how the self-mixing interferometry configuration with a laser diode is explored for what is believed to be the first time to generate flow maps. The experiment was carried out by sensing the laser intensity power spectrum at each pixel as the laser was scanned over a model that mimics the properties of skin and circulating blood.     

Influence of oxygen adsorption on the surface potential of a metal oxide semiconductor

Analytical expressions describing dependences of the surface density of adsorbed oxygen ions and energy band bending in the subsurface region of a metal oxide semiconductor on the oxygen concentration that consider not only the process of neutral gas particle adsorption, but also their charge transfer at the expense of electron capture from the conduction band are presented. It is demonstrated that the heat of oxygen ion absorption is equal to the sum of the heat of neutral particle adsorption and the energy gap between the Fermi level and the level of the oxygen ion on the semiconductor surface. When the adsorption equilibrium is established, an analytical expression describing the time dependence of the energy band bending can be obtained only for small change of the oxygen concentration in the gas mixture.     

超深亚微米互补金属氧化物半导体器件的剂量率效应

对0.18 μm互补金属氧化物半导体(CMOS)工艺的N型金属氧化物半导体场效应晶体管(NMOSFET)及静态随机存储器(SRAM)开展了不同剂量率下的电离总剂量辐照试验研究. 结果表明: 在相同累积剂量, SRAM的低剂量率辐照损伤要略大于高剂量率辐照的损伤, 并且低剂量率辐照损伤要远大于高剂量率辐照加与低剂量率辐照时间相同的室温退火后的损伤. 虽然NMOSFET 低剂量率辐照损伤略小于高剂量率辐照损伤, 但室温退火后, 高剂量率辐照损伤同样要远小于低剂量率辐照损伤. 研究结果表明0.18 μm CMOS工艺器件的辐射损伤不是时间相关效应. 利用数值模拟的方法提出了解释CMOS器件剂量率效应的理论模型.     

Pseudo 2-transistor active pixel sensor using an n-well/gate-tied p-channel metal oxide semiconductor field eeffect transistor-type photodetector with built-in transfer gate

In this paper, a pseudo 2-transistor active pixel sensor (APS) has been designed and fabricated by using an n-well/gate-tied p-channel metal oxide semiconductor field effect transistor (PMOSFET)-type photodetector with built-in transfer gate. The proposed sensor has been fabricated using a 0.35 μm 2-poly 4-metal standard complementary metal oxide semiconductor (CMOS) logic process. The pseudo 2-transistor APS consists of two NMOSFETs and one photodetector which can amplify the generated photocurrent. The area of the pseudo 2-transistor APS is 7.1 × 6.2 μm². The sensitivity of the proposed pixel is 49 lux/(V·s). By using this pixel, a smaller pixel area and a higher level of sensitivity can be realized when compared with a conventional 3-transistor APS which uses a pn junction photodiode.     

Ge metal oxide semiconductor field effect transistors with optimized Si cap and HfSiO2 high-k metal gate stacks

High mobility metal-oxide-semiconductor-field-effect-transistors (MOSFETs) are demonstrated on high quality epitaxial Si_0.75Ge_0.25 films selectively grown on Si (100) substrates. With a Si cap processed on Si_0.75Ge_0.25 channels, HfSiO₂ high-k gate dielectrics exhibited low C–V hysteresis (<10 mV), interface trap density (7.5 × 10¹⁰), and gate leakage current (∼10⁻²A/cm² at an EOT of 13.4 Å), which are comparable to gate stack on Si channels. The mobility enhancement afforded intrinsically by the Si_0.75Ge_0.25 channel (60%) is further increased by a Si cap (40%) process, resulting in a combined ∼100% enhancement over Si channels. The Si cap process also mitigates the low potential barrier issues of Si_0.75Ge_0.25 channels, which are major causes of the high off-state current of small band gap energy Si_0.75Ge_0.25 pMOSFETs, by improving gate control over the channel.     

n型金属氧化物半导体场效应晶体管噪声非高斯性研究

基于n型金属氧化物半导体场效应晶体管（nMOSFET）噪声的数涨落模型,采用高阶统计量双相干系数平方和研究了nMOSFET噪声的非高斯性.通过对nMOSFET实际测试噪声的分析,发现nMOSFET器件噪声存在非高斯性;小尺寸器件噪声的非高斯性强于大尺寸器件;在器件的强反型线性区,其非高斯性随着漏压的增加而增加.文中还通过蒙特卡罗模拟和中心极限定理理论对nMOSFET噪声的非高斯性作了深入的探讨. 关键词： 噪声 非高斯性 n型金属氧化物半导体场效应晶体管 氧化层陷阱     

高迁移率Ge沟道器件研究进展

高迁移率Ge沟道器件由于其较高而且更对称的载流子迁移率, 成为未来互补型金属-氧化物-半导体(CMOS) 器件极有潜力的候选材料. 然而, 对于Ge基MOS器件, 其栅、源漏方面面临的挑战严重影响了Ge基MOS 器件性能的提升, 尤其是Ge NMOS器件. 本文重点分析了Ge基器件在栅、源漏方面面临的问题, 综述了国内外研究者们提出的不同解决方案, 在此基础上提出了新的技术方案. 研究结果为Ge基MOS 器件性能的进一步提升奠定了基础.     

太赫兹互补金属氧化物半导体场效应管探测器理论模型中扩散效应研究

针对基于经典动力学理论传统模型中忽略扩散效应的问题,通过对基于玻尔兹曼理论的场效应管传输线模型的理论分析,建立了包含扩散效应的太赫兹互补金属氧化物半导体(CMOS)场效应管探测器理论模型,研究扩散效应对场效应管电导及响应度的影响.同时,将此模型与忽略了扩散效应的传统模型进行了对比仿真模拟,给出了两种模型下的电流响应度随温度及频率变化的差别.依据仿真结果,并结合3σ原则明确了场效应管传输线模型中扩散部分省略的依据和条件.研究结果表明:扩散部分引起的响应度差异大小主要由场效应管的工作温度及工作频率决定.其中工作频率起主要作用,温度变化对差异大小影响较为微弱;而对于工作频率而言,当场效应管工作频率小于1 THz时,模型中的扩散部分可以忽略不计;而当工作频率大于1 THz时,扩散部分不可省略,此时场效应管模型需同时包含漂移、散射及扩散三个物理过程.本文的研究结果为太赫兹CMOS场效应管理论模型的精确建立及模拟提供了理论支持.     

Parameter analysis for gate metal-oxide-semiconductor structures of ion-implanted 4H silicon carbide metal-semiconductor field-effect transistors

From the theoretical analysis of the thermionic emission model of current-voltage characteristics, this paper extracts the parameters for the gate Schottky contact of two ion-implanted 4H-SiC metal-semiconductor field-effect transistors (sample A and sample B for three and four times multiple ion-implantation channel region respectively) fabricated in the experiment, including the ideality factor, the series resistance, the zero-field barrier height, the interface oxide capacitance, the interface state density distribution, the neutral level of interface states and the fixed space charge density. The methods to improve the interface of the ion-implanted Schottky contact are given at last.     

基于环形栅和半环形栅N沟道金属氧化物半导体晶体管的总剂量辐射效应研究

在商用0.35 μm互补金属氧化物半导体工艺上制备了两种栅氧化层厚度(t_ox)的条形栅、环形栅和半环形栅N沟道金属氧化物半导体 (n-channel metal oxide semiconductor, 简记为NMOS) 晶体管, 并进行了2000 Gy(Si)的总剂量辐射效应实验. 实验结果显示, 栅氧厚度对阈值电压漂移的影响大于栅氧厚度的3次方. 对于t_ox为11 nm的低压NMOS晶体管, 通过环形栅或半环形栅的加固方式能将其抗总剂量辐射能力从300 Gy(Si)提高到2000 Gy(Si)以上; 而对于t_ox为26 nm的高压NMOS晶体管, 通过环栅或半环栅的加固方式, 则只能在低于1000 Gy(Si)的总剂量下, 一定程度地抑制截止漏电流的增加. 作为两种不同的版图加固方式, 环形栅和半环形栅对同一t_ox的NMOS器件加固效果类似, 环形栅的加固效果略优于半环形栅. 对于上述实验结果, 进行了理论分析并阐释了产生这些现象的原因. 关键词： 环形栅 半环形栅 总剂量 辐射效应     

Mobility enhancement of strained GaSb p-channel metal oxide semiconductor field-effect transistors with biaxial compressive strain

Various biaxial compressive strained GaSb p-channel metal–oxide–semiconductor field-effect transistors(MOSFETs)are experimentally and theoretically investigated. The biaxial compressive strained GaSb MOSFETs show a high peak mobility of 638 cm~2/V·s, which is 3.86 times of the extracted mobility of the fabricated GaSb MOSFETs without strain.Meanwhile, first principles calculations show that the hole effective mass of Ga Sb depends on the biaxial compressive strain.The biaxial compressive strain brings a remarkable enhancement of the hole mobility caused by a significant reduction in the hole effective mass due to the modulation of the valence bands.     

具有纵向漏极场板的低导通电阻绝缘体上硅横向双扩散金属氧化物半导体器件新结构

为降低绝缘体上硅(SOI)横向双扩散金属氧化物半导体(LDMOS)器件的导通电阻,同时提高器件击穿电压,提出了一种具有纵向漏极场板的低导通电阻槽栅槽漏SOI-LDMOS器件新结构.该结构特征为采用了槽栅槽漏结构,在纵向上扩展了电流传导区域,在横向上缩短了电流传导路径,降低了器件导通电阻;漏端采用了纵向漏极场板,该场板对漏端下方的电场进行了调制,从而减弱了漏极末端的高电场,提高了器件的击穿电压.利用二维数值仿真软件MEDICI对新结构与具有相同器件尺寸的传统SOI结构、槽栅SOI结构、槽栅槽漏SOI结构进行了比较.结果表明:在保证各自最高优值的条件下,与这三种结构相比,新结构的比导通电阻分别降低了53%,23%和提高了87%,击穿电压则分别提高了4%、降低了9%、提高了45%.比较四种结构的优值,具有纵向漏极场板的槽栅槽漏SOI结构优值最高,这表明在四种结构中新结构保持了较低导通电阻,同时又具有较高的击穿电压.     

0.18 μm部分耗尽绝缘体上硅互补金属氧化物半导体电路单粒子瞬态特性研究

利用脉冲激光入射技术研究100级0.18 μm部分耗尽绝缘体上硅互补金属氧化物半导体反相器链的单粒子瞬态效应, 分析了激光入射器件类型及入射位置对单粒子瞬态脉冲传输特性的影响. 实验结果表明, 单粒子瞬态脉冲在反相器链中的传输与激光入射位置有关, 当激光入射第100级到第2级的n型金属-氧化物-半导体器件, 得到的脉冲宽度从287.4 ps增加到427.5 ps; 当激光入射第99级到第1级的p型金属-氧化物-半导体器件, 得到的脉冲宽度从150.5 ps增加到295.9 ps. 激光入射点靠近输出则得到的瞬态波形窄; 靠近输入则得到的瞬态波形较宽, 单粒子瞬态脉冲随着反相器链的传输而展宽. 入射器件的类型对单粒子瞬态脉冲展宽无影响. 通过理论分析得到, 部分耗尽绝缘体上硅器件浮体效应导致的阈值电压迟滞是反相器链单粒子瞬态脉冲展宽的主要原因. 而示波器观察到的与预期结果幅值相反的正输出脉冲, 是输出节点电容充放电的结果.