Characteristics of high-quality HfSiON gate dielectric prepared by physical vapour deposition

This paper presents a method using simple physical vapour deposition to form high-quality hafnium silicon oxynitride (HfSiON) on ultrathin SiO₂ buffer layer. The gate dielectric with 10? (1?= 0.1 nm) equivalent oxide thickness is obtained. The experimental results indicate that the prepared HfSiON gate dielectric exhibits good physical and electrical characteristics, including very good thermal stability up to 1000℃, excellent interface properties, high dielectric constant (k=14) and low gate-leakage current (I_g=1.9×10^-3A/cm² @V_g=V_fb-1V for EOT of 10?). TaN metal gate electrode is integrated with the HfSiON gate dielectric.The effective work function of TaN on HfSiON is 4.3eV, meeting the requirements of NMOS for the metal gate. And, the impacts of sputtering ambient and annealing temperature on the electrical properties of HfSiON gate dielectric are investigated.     

高$lt;i$gt;k$lt;/i$gt;栅介质小尺寸全耗尽绝缘体上锗p型金属氧化物半导体场效应晶体管漏源电流模型

通过求解沟道的二维泊松方程得到沟道表面势和沟道反型层电荷, 建立了高k栅介质小尺寸绝缘体上锗(GeOI) p型金属氧化物半导体场效应晶体管(PMOSFET)的漏源电流解析模型. 模型包括了速度饱和效应、迁移率调制效应和沟长调制效应, 同时考虑了栅氧化层和埋氧层与沟道界面处的界面陷阱电荷、氧化层固定电荷对漏源电流的影响. 在饱和区和非饱和区, 漏源电流模拟结果与实验数据符合得较好, 证实了模型的正确性和实用性. 利用建立的漏源电流模型模拟分析了器件主要结构和物理参数对跨导、漏导、截止频率和电压增益的影响, 对GeOI PMOSFET的设计具有一定的指导作用. 关键词： 绝缘体上锗p型金属氧化物半导体场效应晶体管 漏源电流模型 跨导 截止频率     

具有poly-Si$lt;sub$gt;1-$lt;i$gt;x$lt;/i$gt;$lt;/sub$gt;Ge$lt;sub$gt;$lt;i$gt;x$lt;/i$gt;$lt;/sub$gt;栅的应变SiGep型金属氧化物半导体场效应晶体管阈值电压漂移模型研究

针对具有poly-Si_1-xGe_x栅的应变SiGe p型金属氧化物半导体场效应晶体管(PMOSFET), 研究了其垂直电势与电场分布, 建立了考虑栅耗尽的poly-Si_1-xGe_x栅情况下该器件的等效栅氧化层厚度模型, 并利用该模型分析了poly-Si_1-xGe_x栅及应变SiGe层中Ge组分对等效氧化层厚度的影响. 研究了应变SiGe PMOSFET热载流子产生的机理及其对器件性能的影响, 以及引起应变SiGe PMOSFET阈值电压漂移的机理, 并建立了该器件阈值电压漂移模型, 揭示了器件阈值电压漂移随电应力施加时间、栅极电压、poly-Si_1-xGe_x栅及应变SiGe层中Ge组分的变化关系. 并在此基础上进行了实验验证, 在电应力施加10000 s时, 阈值电压漂移0.032 V, 与模拟结果基本一致, 为应变SiGe PMOSFET及相关电路的设计与制造提供了重要的理论与实践基础. 关键词： 应变SiGep型金属氧化物半导体场效应晶体管 1-xGe_x栅')" href="#">poly-Si_1-xGe_x栅 热载流子 阈值电压     

压应变Ge/(001)Si1-xGex空穴散射与迁移率模型

应变Ge材料因其载流子迁移率高, 且与硅工艺兼容等优点, 已成为硅基CMOS研究发展的重点和热点. 本文基于压应变Ge/(001)Si_1-xGe_x价带结构模型, 研究了压应变Ge/(001)Si_1-xGe_x空穴各散射概率、空穴迁移率与Ge组分(x)的关系, 包括空穴离化杂质散射概率、声学声子散射、非极性光学声子散射、总散射概率以及空穴各向同性、各向异性迁移率, 获得了有实用价值的相关结论. 本文量化模型可为应力致Ge改性半导体物理的理解及相关器件的研究设计提供有重要的理论参考.     

硅(001)图形衬底上锗硅纳米线的定位生长

纳米线的定位生长是实现纳米线量子器件寻址和集成的前提.结合自上而下的纳米加工和自下而上的自组装技术,通过分子束外延生长方法,在具有周期性凹槽结构的硅(001)图形衬底上首先低温生长硅锗薄膜然后升温退火,实现了有序锗硅纳米线在凹槽中的定位生长,锗硅纳米线的表面晶面为(105)晶面.详细研究了退火温度、硅锗的比例及图形周期对纳米线形成与否,以及纳米线尺寸的影响.     

LaTiO高k栅介质Ge MOS电容电特性及Ti含量优化

采用共反应溅射法将Ti添加到La_2O_3中,制备了LaTiO/Ge金属-氧化物-半导体电容,并就Ti含量对器件电特性的影响进行了仔细研究.由于Ti-基氧化物具有极高的介电常数,LaTiO栅介质能够获得高k值;然而由于界面/近界面缺陷随着Ti含量的升高而增加,添加Ti使界面质量恶化,进而使栅极漏电流增大、器件可靠性降低.因此,为了在器件电特性之间实现协调,对Ti含量进行优化显得尤为重要.就所研究的Ti/La_2O_3比率而言,18.4%的Ti/La_2O_3比率最合适.该比率导致器件呈现出高k值(22.7)、低D_(it)(5.5×10~(11)eV~(-1)·cm~(-2))、可接受的J_g(V_g=1V,J_g=7.1×10~(-3)A·cm~(-2))和良好的器件可靠性.     

Hole mobility enhancement in uniaxial stressed Ge dependence on stress and transport direction

Utilizing a six-band k.p valence band calculations that considered a strained perturbation Hamiltonian, uniaxial stress-induced valence band structure parameters for Ge such as band edge energy shift, split, and effective mass were quantitatively evaluated. Based on these valence band parameters, the dependence of hole mobility on uniaxial stress (direction, type, and magnitude) and hole transport direction was theoretical studied. The results show that the hole mobility had a strong dependence on the transport direction and uniaxial stress. The hole mobility enhancement can be found for all transport directions and uniaxial stess configurations, and the hole transport along the [110] direction under the uniaxial [110] compressive stress had the highest mobility compared to other transport directions and stress configurations.     

采用Al/TaN叠层电极提高Si基Ge PIN光电探测器的性能

金属与Ge材料接触由于存在强烈的费米钉扎效应, 导致金属电极与n型Ge接触引入较大的接触电阻, 限制了Si基Ge探测器响应带宽. 本文报道了在SOI衬底上外延Ge单晶薄膜并制备了不同台面尺度的Ge PIN光电探测器. 对比了电极分别为金属Al和Al/TaN叠层的具有相同器件结构的SOI基Ge PIN光电探测器的暗电流、响应度以及响应带宽等参数. 发现在Al与Ge之间增加一薄层TaN可有效减小n型Ge的接触电阻, 将台面直径为24 μ的探测器在1.55 μ的波 长和-1 V偏压下的3 dB响应带宽提高了4倍. 同时, 器件暗电流减小一个数量级, 而响应度提高了2倍. 结果表明, 采用TaN薄层制作金属与Ge接触电极, 可有效钝化金属与Ge界面, 减轻费米钉扎效应, 降低金属与n-Ge接触的势垒高度, 因而减小接触电阻和界面复合电流, 提高探测器的光电性能.     

采用AI／TaN叠层电极提高Si基GePIN光电探测器的性能

金属与Ge材料接触由于存在强烈的费米钉扎效应,导致金属电极与n型Ge接触引入较大的接触电阻,限制了si基Ge探测器响应带宽．本文报道了在SOI衬底上外延Ge单晶薄膜并制备了不同台面尺度的GePIN光电探测器．对比了电极分别为金属Al和A1／TaN叠层的具有相同器件结构的SOI基GePIN光电探测器的暗电流、响应度以及响应带宽等参数．发现在Al与Ge之间增加一薄层TaN可有效减小n型Ge的接触电阻,将台面直径为24um的探测器在1．55um的波长和-1V偏压下的3dB响应带宽提高了4倍．同时,器件暗电流减小一个数量级,而响应度提高了2倍．结果表明,采用TaN薄层制作金属与Ge接触电极,可有效钝化金属与Ge界面,减轻费米钉扎效应,降低金属与n-Ge接触的势垒高度,因而减小接触电阻和界面复合电流,提高探测器的光电性能．     

Study on changes in the structure of HfSiO and HfSiON dielectrics with different annealing temperature by photoelectron spectroscopy

We have investigated changes of the structure for HfSiO and HfSiON film with different annealing temperature by photoelectron spectroscopy. Core level photoelectron spectra have revealed the mechanism of metallization reaction at the bottom interface between the HfSiO(N) film and Si substrate under vacuum annealing. Silicidation action occurs by annealing at 850 and 900 °C for HfSiO and HfSiON film, respectively, indicating the incorporation of nitrogen enhances the thermal stability. By annealing at 900 °C, metallization reaction is rapidly promoted for the HfSiO film. For HfSiON film, Hf-nitride clusters or Hf-nitride layer and metal-silicide are formed at the bottom and upper interface, respectively, upon annealing at 950 °C.     

Structural and electrical properties of laser-crystallized nanocrystalline Ge films and nanocrystalline Ge/SiN_x multilayers

Nanocrystalline Ge （nc-Ge） single layers and nc-Ge/SiNx multilayers are prepared by laser annealing amorphous Ge （a-Ge） films and a-Ge/SiNx multilayers. The microstructures as well as the electrical properties of laser-crystallized samples are systematically studied by using various techniques. It is found that the optical band gap of nc-Ge film is reduced compared with its amorphous counterpart. The formed nc-Ge film is of p-type, and the dark conductivity is enhanced by 6 orders for an nc-Ge single layer and 4 orders for a multilayer. It is suggested that the carrier transport mechanism is dominant by the thermally activation process via the nanocrystal, which is different from the thermally annealed nc-Ge sample at an intermediate temperature. The carrier mobility of nc-Ge film can reach as high as about 39.4 cm2.V ^-1 .s^-1, which indicates their potential applications in future nano-devices.     

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.     

堆叠栅介质对称双栅单Halo应变Si金属氧化物半导体场效应管二维模型

提出了一种堆叠栅介质对称双栅单Halo应变Si金属氧化物半导体场效应管(metal-oxide semiconductor field effect transistor,MOSFET)新器件结构.采用分区的抛物线电势近似法和通用边界条件求解二维泊松方程,建立了全耗尽条件下的表面势和阈值电压的解析模型.该结构的应变硅沟道有两个掺杂区域,和常规双栅器件(均匀掺杂沟道)比较,沟道表面势呈阶梯电势分布,能进一步提高载流子迁移率;探讨了漏源电压对短沟道效应的影响;分析得到阈值电压随缓冲层Ge组分的提高而降低,随堆叠栅介质高k层介电常数的增大而增大,随源端应变硅沟道掺杂浓度的升高而增大,并解释了其物理机理.分析结果表明:该新结构器件能够更好地减小阈值电压漂移,抑制短沟道效应,为纳米领域MOSFET器件设计提供了指导.     

Raman modes of metastable phases of Si and Ge

Abstract

We have measured Raman spectra of metastable phases of Si and Ge prepared in a diamond anvil cell for pressures up to 12 GPa. For Si we observe eight Raman lines with mode Grüneisen parameters varying between -0.3 and 1.5. These lines can be assigned to the zone-center phonons of the cubic BC8-structure (Z = 8) by assuming a violation of Raman selection rules presumably due to disorder. In the case or Ge we observe two phases with different Raman spectra. The spectrum of the first phase is strikingly similar to that of BC8-Si. Below about 5 GPa this phase transforms into a second phase, which can be identified as Ge in the hexagonal diamond structure.     

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.     

Shape, facet evolution and photoluminescence of Ge islands capped with Si at different temperatures

We investigate the embedding of Ge islands in a Si matrix by means of atomic force microscopy and photoluminescence (PL) spectroscopy. The Ge islands were grown between 360°C and 840°C and subsequently capped with Si at different temperatures. For the highest Ge growth temperature (840°C), we show that the surface flattens at high Si capping temperatures while new facets can be identified at the island base for intermediate capping temperatures (650–450°C). At low capping temperatures (300–350°C), the island morphology is preserved. In contrast to the observed island shape changes, the decreasing Si capping temperature causes only a small redshift of the island related PL signal for islands grown on high temperatures. This redshift increases for Ge islands grown at lower temperatures due to an increased Ge content in the islands. By applying low-temperature capping (300°C) on the different island types, we show that the emission wavelength can be extended up to 2.06 μm for hut clusters grown at 400°C. Further decreasing of the island growth temperature to 360°C leads to a PL blueshift, which is explained by charge carrier confinement in Ge quantum dots.     

Experimental clarification of orientation dependence of germanium PMOSFETs with AlzO3/GeOx/Ge gate stack

An extensive and complete experimental investigation with a full layout design of the channel direction was carried out for the first time to clarify the orientation dependence of germanium p-channel metal-oxide-semiconductor field-effect transistors （PMOSFETs）. By comparison of gate trans-conductance, drive current, and hole mobility, we found that the performance trend with the substrate orientation for Ge PMOSFET is （110）〉（111） ~ （100）, and the best channel direction is （110）/[110]. Moreover, the （110） device performance was found to be easily degraded as the channel direction got off from the [ 110] orientation, while （100） and （111） devices exhibited less channel orientation dependence. This experimental result shows good matching with the simulation reports to give a credible and significant guidance for Ge PMOSFET design.     

A study of GaN MOSFETs with atomic-layer-deposited A1203 as the gate dielectric

Accumulation-type GaN metal-oxide-semiconductor field-effect transistors （MOSFETs） with atomic-layerdeposited Al₂O₃ gate dielectrics are fabricated.The device,with atomic-layer-deposited Al₂O₃ as the gate dielectric,presents a drain current of 260 mA/mm and a broad maximum transconductance of 34 mS/mm,which are better than those reported previously with Al₂O₃ as the gate dielectric.Furthermore,the device shows negligible current collapse in a wide range of bias voltages,owing to the effective passivation of the GaN surface by the Al₂O₃ film.The gate drain breakdown voltage is found to be about 59.5 V,and in addition the channel mobility of the n-GaN layer is about 380 cm2 /Vs,which is consistent with the Hall result,and it is not degraded by atomic-layer-deposition Al₂O₃ growth and device fabrication.     

金属与半导体Ge欧姆接触制备、性质及其机理分析

金属与Ge材料接触时界面处存在着强烈的费米钉扎效应, 尤其与n型Ge形成的欧姆接触的比接触电阻率高, 是制约Si基Ge器件性能的关键因素之一. 本文对比了分别采用金属Al和Ni 与Si衬底上外延生长的p型Ge和n型Ge材料的接触特性. 发现在相同的较高掺杂条件下, NiGe与n型Ge可形成良好的欧姆接触, 其比接触电阻率 较 Al接触降低了一个数量级, 掺P浓度为2×10¹⁹ cm^-3时达到1.43×10^-5 Ω·cm². NiGe与p型Ge接触和Al接触的比接触电阻率相当, 掺B浓度为4.2×10¹⁸ cm^-3时达到1.68×10^-5 Ω·cm². NiGe与n型Ge接触和Al电极相比较, 在形成NiGe过程中, P杂质在界面处的偏析是其接触电阻率降低的主要原因. 采用NiGe作为Ge的接触电极在目前是合适的选择. 关键词： 金属与Ge接触性质 NiGe 比接触电阻率     

Influence of defects on the optical and structural properties of Ge dots embedded in an Si/Ge superlattice

In this work we studied the influence of high-energy proton irradiation on the optical and structural properties of an Si/Ge superlattice (SL) with embedded Ge quantum dots (QDs). The presence of QDs in the as-grown samples was established by transmission electron microscopy and photoluminescence (PL). The samples were irradiated with 2.0 MeV protons to fluences in the range 2×10¹²-2×10¹⁴ cm^-2. The structural characterization made by X-ray reciprocal space mapping, X-ray reflection and Rutherford backscattering/channelling has shown no changes in the as-grown heterostructure due to the irradiation. In spite of the expected high concentration of nonradiative recombination centres caused by the proton-induced damage, the PL emission from the Ge dots has been observed even for the highest irradiation fluence. The studied QD-in-SL structure has shown an extraordinarily high radiation hardness when compared with previously studied QD heterostructures.