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1.
A novel-channel MOS transistor with a silicon-germanium (SiGe) heterostructure embedded beneath the channel and silicon-carbon source/drain (Si:C S/D) stressors was demonstrated. The additional SiGe structure couples additional strain from the S/D stressors to the overlying Si channel, leading to enhanced strain effects in the channel region. We termed the SiGe region a strain-transfer structure due to its role in enhancing the transfer of strain from lattice-mismatched S/D stressors to the channel region. Numerical simulations were performed using the finite-element method to explain the strain-transfer mechanism. A significant drive current IDSAT improvement of 40% was achieved over the unstrained control devices, which is predominantly due to the strain-induced mobility enhancement. In addition, the impact of scaling the device design parameters on transistor drive current performance was investigated. Guidelines on further performance optimization in such a new device structure are provided.  相似文献   

2.
High-k gate dielectric La2O3 thin films have been deposited on Si(1 0 0) substrates by molecular beam epitaxy (MBE). Al/La2O3/Si metal-oxide–semiconductor capacitor structures were fabricated and measured. A leakage current of 3 × 10−9 A/cm2 and dielectric constant between 20 and 25 has been measured for samples having an equivalent oxide thickness (EOT) 2.2 nm. The estimated interface state density Dit is around 1 × 1011 eV−1 cm−2. EOT and flat-band voltage were calculated using the NCSU CVC program. The chemical composition of the La2O3 films was measured using X-ray photoelectron spectrometry and Rutherford backscattering. Current density vs. voltage curves show that the La2O3 films have a leakage current several orders of magnitude lower than SiO2 at the same EOT. Thin La2O3 layers survive anneals of up to 900 °C for 30 s with no degradation in electrical properties.  相似文献   

3.
A recessed gate AlGaN/GaN high-electron mobility transistor (HEMT) on sapphire (0 0 0 1), a GaN metal-semiconductor field-effect transistor (MESFET) and an InGaN multiple-quantum well green light-emitting diode (LED) on Si (1 1 1) substrates have been grown by metalorganic chemical vapor deposition. The AlGaN/GaN intermediate layers have been used for the growth of GaN MESFET and LED on Si substrates. A two-dimensional electron gas mobility as high as 9260 cm2/V s with a sheet carrier density of 4.8×1012 cm−2 was measured at 4.6 K for the AlGaN/GaN heterostructure on the sapphire substrate. The recessed gate device on sapphire showed a maximum extrinsic transconductance of 146 mS/mm and a drain–source current of 900 mA/mm for the AlGaN/GaN HEMT with a gate length of 2.1 μm at 25°C. The GaN MESFET on Si showed a maximum extrinsic transconductance of 25 mS/mm and a drain–source current of 169 mA/mm with a complete pinch-off for the 2.5-μm-gate length. The LED on Si exhibited an operating voltage of 18 V, a series resistance of 300 Ω, an optical output power of 10 μW and a peak emission wavelength of 505 nm with a full-width at half-maximum of 33 nm at 20 mA drive current.  相似文献   

4.
We report the fabrication of bottom-gate thin film transistors (TFTs) at various carrier concentrations of an amorphous InGaZnO (a-IGZO) active layer from ~1016 to ~1019 cm−3, which exceeds the limit of the concentration range for a conventional active layer in a TFT. Using the Schottky TFTs configuration yielded high TFT performance with saturation mobility (μsat), threshold voltage (VTH), and on off current ratio (ION/IOFF) of 16.1 cm2/V s, −1.22 V, and 1.3×108, respectively, at the highest carrier concentration active layer of 1019 cm−3. Other carrier concentrations (<1019 cm−3) of IGZO resulted in a decrease of its work function and increase in activation energy, which changes the source/drain (S/D) contact with the active layer behavior from Schottky to quasi Ohmic, resulting in achieving conventional TFT. Hence, we successfully manipulate the barrier height between the active layer and the S/D contact by changing the carrier concentration of the active layer. Since the performance of this Schottky type TFT yielded favorable results, it is feasible to explore other high carrier concentration ternary and quaternary materials as active layers.  相似文献   

5.
A novel SiGe-S/D structure for high performance pMOSFET called two-step recessed SiGe-source/drain (S/D) is developed with careful optimization of recessed SiGe-S/D structure. With this method, hole mobility, short channel effect and S/D resistance in pMOSFET are improved compared with conventional recessed SiGe-S/D structure. To enhance device performance such as drain current drivability, SiGe region has to be closer to channel region. Then, conventional deep SiGe-S/D region with carefully optimized shallow SiGe SDE region showed additional device performance improvement without SCE degradation. As a result, high performance 24 nm gate length pMOSFET was demonstrated with drive current of 451 μA/μm at Vdd of 0.9 V and Ioff of 100 nA/μm (552 μA/μm at Vdd of 1.0 V). Furthermore, by combining with Vdd scaling, we indicate the extendability of two-step recessed SiGe-S/D structure down to 15 nm node generation.  相似文献   

6.
A novel strained-silicon (Si) n-MOSFET with 50-nm gate length is reported. The strained n-MOSFET features silicon-carbon (Si1-yCy) source and drain (S/D) regions formed by a Si recess etch and a selective epitaxy of Si1-yCy in the S/D regions. The carbon mole fraction incorporated is 0.013. Lattice mismatch of ~0.56% between Si 0.987C0.013 and Si results in lateral tensile strain and vertical compressive strain in the Si channel region, both contributing to substantial electron-mobility enhancement. The conduction-band offset DeltaEc between the Si0.987 C0.013 source and the strained Si channel could also contribute to an increased electron injection velocity nuinj from the source. Implementation of the Si0.987 C0.013 S/D regions for n-MOSFET provides significant drive current IDsat enhancement of up to 50% at a gate length of 50 nm  相似文献   

7.
A simple technique leading to the measurement of minority carrier lifetimes of UHV compatible LPCVD Si and SiGe by Ct depth profiling of Metal:Oxide:Si:SiGe:Si structures is reported. A high quality gate oxide is realised by low temperature (<100°C) plasma anodisation thereby reducing any oxidation effects on the underlying epitaxial layer quality. Capacitance response times were observed for an impurity concentration of 2.5×1017 cm−3, giving rise to generation lifetimes of the Si and Si0.9Ge0.1 of >0.55 and 2.6 μs respectively, reflective of very high quality epitaxial semiconductor material.  相似文献   

8.
刘艳  颜静  王洪娟  韩根全 《半导体学报》2014,35(2):024001-4
在Si(110)衬底上制备了Ge源n型Si沟道隧穿场效应晶体管(TFET)。本文研究了温度对Ge源Si TFET器件的电学性能的影响。温度相关性研究显示器件漏电流主要由漏区的Shockley - Read - Hall (SRH) 产生于复合电流决定。器件开态电流随温度升高而增加,这是因为温度升高材料禁带宽度减小,隧穿几率增大。界面缺陷引起的隧穿电流的亚阈值摆幅随温度升高而变差,但是带间隧穿电流的亚阈值摆幅不随温度变化而变化。  相似文献   

9.
There are several advanced processes which are being actively studied as candidates for sub-0.25 μm technology. This paper studies the effects on NMOS hot carrier reliability from remote plasma nitrided oxide (RPNO), deuterium anneal and pocket implant. It is found that RPNO will not affect the SiO2/Si interface. The hot carrier reliability is better for the same device channel current. This is due to making the effective oxide thickness thinner and achieving the same drive current with longer channel length. The deuterium anneal can improve the hot carrier reliability, even with nitride sidewall, if proper annealing is done. While the pocket implant can reduce short channel effects, the hot carrier lifetime is degraded unless optimization is done.  相似文献   

10.
In this paper we investigate and develop models for partially-depleted silicon-on-insulator (SOI) (PD–SOI) device failure under EOS/ESD stress. The model and experimental data show that due to increased device self-heating, the second-breakdown current per micron width (It2) for salicided PD-SOI metal-oxide semiconductor field effect transistor (MOSFET)s with Si film thickness of 100 nm is about 50% of that in their bulk counterparts under human body model (HBM–ESD) stress pulses. Furthermore, It2 did not scale with device width. Therefore, ESD protection devices with non-silicided S/D diffusions and source-body tied MOSFETs are investigated for improved ESD protection levels. Compact ESD protection networks using the source-body tied device may have been shown to achieve HBM–ESD protection levels of ±3.75 kV (Smith JC, Lien M, Veeraghaven S. An ESD protection circuit for TFSOI technology. International SOI Conf. Proc. 1996. pp. 170–71).  相似文献   

11.
1/f noise was measured on lateral bipolar PNP transistors over a temperature range of 220<T<450 K. Noise power spectral density measurements were performed simultaneously across two resistors connected in series with base and collector. The equivalent base current noise source SIB has two dominant components. One is SIBE that is between the base and the emitter, in parallel with rπ. The other is SIBC coming from the surface recombination current at the neutral base, between the base and the collector. The extracted SIB exhibited a near square law dependence on base current IB. The noise remained nearly constant when the temperature was below 310 K. However, it presented strong temperature dependence when the temperature was beyond 310 K. Two different models are proposed for the noise in different temperature regions. For the high temperature region, the surface recombination velocity fluctuation model is proposed, which indicates that the noise is coming from the fluctuations in the surface recombination velocity at the neutral base surface. The tunneling assistant trapping model is responsible for the low temperature region, where the noise source is the carrier trapping–detrapping by the defects in the spacer oxide covering the surface of the depletion layer.  相似文献   

12.
A thin body (fully depleted) strained SGOI device structure (FDSGOI), and a strained SiGe channel layer on SOI, were fabricated using scaled high-κ gate dielectrics and metal gate technology. The uniaxial strain effect and corresponding drive current enhancement reported by Irisawa et al. [1] for narrow-width devices was investigated on these structures. Although the strained FDSGOI device structure exhibited reduced off-state leakage compared to thicker body devices, and long-channel drive current enhancement under uniaxial strain, the loss of drive current enhancement at short channel length led to uncompetitive ION-IOFF characteristics. The SiGe on SOI structure showed the highest long-channel drive current enhancement (nearly 3×) in the narrowest devices, and also showed a significant reduction in off-state current. This trend was maintained down to the shortest channel lengths studied here and resulted in ION-IOFF characteristics that were competitive with contemporary uniaxial strained Si channel devices.  相似文献   

13.
All of the major acceptor (Mg, C, Be) and donor (Si, S, Se and Te) dopants have been implanted into GaN films grown on Al2O3 substrates. Annealing was performed at 1100–1500°C, using AlN encapsulation. Activation percentages of ≥90% were obtained for Si+ implantation annealed at 1400°C, while higher temperatures led to a decrease in both carrier concentration and electron mobility. No measurable redistribution of any of the implanted dopants was observed at 1450°C.  相似文献   

14.
Heterojunction solar cells of p‐type cupric oxide (CuO) and n‐type silicon (Si), p‐CuO/n‐Si, have been fabricated using conventional sputter and rapid thermal annealing techniques. Photovoltaic properties with an open‐circuit voltage (Voc) of 380 mV, short circuit current (Jsc) of 1.2 mA/cm2, and a photocurrent of 2.9 mA/cm2 were observed for the solar cell annealed at 300 °C for 1 min. When the annealing duration was increased, the photocurrent increased, but the Voc was found to reduce because of the degradation of interface quality. An improvement in the Voc resulting to a record value of 509 mV and Jsc of 4 mA/cm2 with a high photocurrent of ~12 mA/cm2 was achieved through interface engineering and controlling the phase transformation of CuO film. X‐ray diffraction, X‐ray photoelectron spectroscopy, and high‐resolution transmission electron microscopy analysis have been used to investigate the interface properties and crystal quality of sputter‐deposited CuO thin film. The improvement in Voc is mainly due to the enhancement of crystal quality of CuO thin film and interface properties between p‐CuO and n‐Si substrate. The enhancement of photocurrent is found to be due to the reduction of carrier recombination rate as revealed by transient photovoltage spectroscopy analysis. Copyright © 2014 John Wiley & Sons, Ltd.  相似文献   

15.
The distribution of hydrogen in Si and SiC following high-temperature proton irradiation (T irr=20–700 °C) is studied by secondary-ion mass spectrometry. It is shown that the hydrogen concentration profile in SiC depends weakly on irradiation temperature. In Si appreciable alteration of the concentration profile is observed already at T irr⋍300 °C, and the profile completely loses its concentration gradient at T irr⋍700 °C. Fiz. Tekh. Poluprovodn. 33, 1409–1410 (December 1999)  相似文献   

16.
The carrier conduction and the degradation mechanism in n+gate p-channel metal-insulator-semiconductor field-effect-transistors with HfAlOX (Hf: 60 at.%, Al: 40 at.%)/SiO2 dielectric layers have been investigated using carrier separation method. Since gate current depends on substrate bias and both electron and hole currents are independent of temperature over the range of 25–150 °C, the conduction mechanism for both currents is controlled by a tunneling process. As the interfacial SiO2 layer (IL) thickness increases in a fixed high-k layer thickness (Thigh-k), a dominant carrier in the leakage current changes from hole to electron around 2.2-nm-thick IL. This is due to an asymmetric barrier height for electrons and holes at the SiO2/Si interface. On the contrary, in the case of a fixed IL thickness of 1.3 nm, the hole current is dominant in the leakage current, regardless of Thigh-k. It is shown that the dominant carrier in the leakage current depends on the structure of the high-k stack. Both electron and hole currents for the stress-induced-leakage-current (SILC) state increase slightly relative to the initial currents, which means that the trap generation in the high-k stack occurs near both the conduction band edge of n+poly-Si gate and the valence band edge of Si substrate. The electron current at soft breakdown (SBD) state dramatically increases over that for the SILC state, while the hole currents for both the SILC state and SBD are almost the same. This indicates that the defect sites generated in the high-k stack after SBD are located at energies near the conduction band edge of n+poly-Si gate. Both the defect generation rate and the defect size in the HfAlOX/SiO2 stacks are large compared with those in SiO2. It is inferred that, in high-k dielectric stack, the defect generation mainly occurs in the high-k side rather than the IL side, and the defect size larger than the case of SiO2 could be related to a larger dielectric constant of the high-k layer.  相似文献   

17.
High-κ oxides such as ZrO2 and HfO2 have attracted great interest, due to their physical properties, suitable to replacement of SiO2 as gate dielectric materials. In this work, we investigate the tunneling properties of ZrO2 and HfO2 high-κ oxides, by applying quantum mechanical methods that include the full-band structure of Si and oxide materials. Semiempirical sp3s*d tight-binding parameters have been determined to reproduce ab initio band dispersions. Transmission coefficients and tunneling current have been calculated for Si/ZrO2/Si and Si/HfO2/Si MOS structures, showing a very low gate leakage current in comparison to SiO2-based structures with equivalent oxide thickness.  相似文献   

18.
This paper reports comparative reliability of the hot carrier induced electrical performance degradation in power RF LDMOS transistors after RF life-tests and novel methods for accelerated ageing tests under various conditions (electrical and/or thermal stress): thermal shock tests (TST, air–air test) and thermal cycling tests (TCT, air–air test) under various conditions (with and without DC bias, TST cold and hot, different channel current IDS and different extremes temperatures ΔT values). It is important to understand the effects of the reliability degradation mechanisms on the S-parameters and in turn on static and dynamic parameters. The analysis of the experimental results is presented and the physical processes responsible for the observed degradation at different stress conditions are studied by means of 2D ATLAS-SILVACO simulations. The RF performance degradation of hot-carrier effects power RF LDMOS transistors can be explained by the transconductance and miller capacitance shifts, which are resulted from the interface state generation and trapped electrons, thereafter results in a build up of negative charge at Si/SiO2 interface.  相似文献   

19.
Ga doped ZnO (GZO) films prepared by sputtering at room temperature were rapid thermal annealed (RTA) at elevated temperatures. With increasing annealing temperature up to 570°C, film transmission enhanced significantly over wide spectral range especially in infrared region. Hall effect measurements revealed that carrier density decreased from ∼8 × 1020 to ∼ 3 × 1020 cm−3 while carrier mobility increased from ∼15 to ∼28 cm2/Vs after the annealing, and consequently low film resistivity was preserved. Hydrogenated microcrystalline Si (µc‐Si:H) and microcrystalline Si1‐xGex (µc‐Si1‐xGex:H, x = 0.1) thin film solar cells fabricated on textured RTA‐treated GZO substrates demonstrated strong enhancement in short‐circuit current density due to improved spectral response, exhibiting quite high conversion efficiencies of 9.5% and 8.2% for µc‐Si:H and µc‐Si0.9Ge0.1:H solar cells, respectively. Copyright © 2011 John Wiley & Sons, Ltd.  相似文献   

20.
Deposition of Ag films by direct liquid injection-metal organic chemical vapor deposition (DLI-MOCVD) was chosen because this preparation method allows precise control of precursor flow and prevents early decomposition of the precursor as compared to the bubbler-delivery. Silver(I)-2,2-dimethyl-6,6,7,7,8,8,8-heptafluoro-3,5-octanedionato-triethylphosphine [Ag(fod)(PEt3)] as the precursor for Ag CVD was studied, which is liquid at 30 °C. Ag films were grown on different substrates of SiO2/Si and TiN/Si. Argon and nitrogen/hydrogen carrier gas was used in a cold wall reactor at a pressure of 50–500 Pa with deposition temperature ranging between 220 °C and 350 °C. Ag films deposited on a TiN/Si diffusion barrier layer have favorable properties over films deposited on SiO2/Si substrate. At lower temperature (220 °C), film growth is essentially reaction-limited on SiO2 substrate. Significant dependence of the surface morphology on the deposition conditions exists in our experiments. According to XPS analysis pure Ag films are deposited by DLI-MOCVD at 250 °C by using argon as carrier gas.  相似文献   

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