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1.
The bias stress effect in pentacene thin-film transistors (TFTs) with and without MoOx interlayer was characterized. The device without MoOx interlayer showed a large threshold voltage shift of 5.1 V after stressing with a constant gate-source voltage of −40 V for 10000 s, while at the same condition, the device with MoOx interlayer showed a low threshold voltage shift of 1.9 V. The results can be attributed to the stable interface between MoOx/pentacene and small contact resistance change for the device with MoOx/Cu electrode. Pentacene-TFTs with MoOx interlayer showed a high field-effect mobility of 0.61 cm2/V s and excellent bias stability, which could be a significant step toward the commercialization of OTFT technology.  相似文献   

2.
《Current Applied Physics》2014,14(8):1036-1040
We have fabricated hafnium–indium–zinc-oxide (HfInZnO) thin film transistors (TFT) with indium–tin-oxide (ITO) interlayer. Compared with conventional HfInZnO-TFT, the electrical performance and bias stability of HfInZnO-TFTs with ITO interlayer are improved. HfInZnO-TFT with 4-nm-thick ITO interlayer shows a high mobility of 7.2 cm2/V s, a low threshold voltage of 0.13 V and a better bias stability. The performance enhancement is attributed to a decrease in interface trap state and an increase in carrier concentration. It suggests that introducing ITO interlayer at the ALD Al2O3/HfInZnO interface is an effective way to improve the electrical performance and bias stability.  相似文献   

3.
《Current Applied Physics》2010,10(5):1306-1308
Low-voltage-drive ZnO thin-film transistors (TFTs) with room-temperature radio frequency magnetron sputtering SiO2 as the gate insulator were fabricated successfully on the glass substrate. The ZnO-TFT operates in the enhancement mode with a threshold voltage of 4.2 V, a field effect mobility of 11.2 cm2/V s, an on/off ratio of 3.1 × 106 and a subthreshold swing of 0.61 V/dec. The drain current can reach to 1 mA while the gate voltage is only of 12 V and drain voltage of 8 V. The C–V characteristics of a MOS capacitor with the structure of ITO/SiO2/ZnO/Al was investigated. The carrier concentration ND in the ZnO active layer was determined, the calculated ND is 1.81 × 1016 cm−3, which is the typical value of undoped ZnO film used as the channel layer for ZnO-TFT devices. The experiment results show that SiO2 film is a promising insulator for the low voltage and high drive capability oxide TFTs.  相似文献   

4.
We demonstrated the tunable contact resistance in pentacene thin film transistor (TFT) by inserting an organic-inorganic hybrid interlayer between Au electrode and pentacene layer. The contact resistance of pentacene-TFT varies with concentration of pentacene-TFT varies with concentration of MoOx in organic-inorganic hybrid interlayer. MoOx in organic-inorganic hybrid interlayer. The contact resistance of the device with 55 wt% MoOx doped pentacene interlayer is about 7.8 times smaller than that of device without interlayer at the gate voltage of −20 V. Comparing the properties of pentacene-TFT without interlayer, the performance of the pentacene-TFT with 55 wt% MoOx doped pentacene was significantly improved: saturation mobility increased from 0.39 to 0.87 cm2/V s, threshold voltage reduced from −21.3 to −7.2 V, and threshold swing varied from 3.75 to 1.39 V/dec. Our results indicated that the organic-inorganic hybrid interlayer is an effective way to improve the performance of p-channel OTFTs.  相似文献   

5.
N2O Plasma表面处理对SiNx基IGZO-TFT性能的影响   总被引:1,自引:1,他引:0  
采用N2O plasma处理SiNx薄膜作为绝缘层,以室温下沉积的铟镓锌氧化物(IGZO)作为有源层制备了 IGZO薄膜晶体管。与常规的IGZO-TFT相比,N2O plasma处理过的IGZO-TFT的迁移率由原来的4.5 cm2·V-1·s-1增 加至8.1 cm2·V-1·s-1,阈值电压由原来的11.5 V减小至3.2 V,亚阈值摆由原来的1.25 V/decade减小至0.9 V/decade。采用C-V方法计算了两种器件的陷阱态,结果发现N2O plasma处理过的IGZO-TFT的陷阱态明显小于普通的IGZO-TFT的陷阱态,表明N2O plasma处理SiNx绝缘层是一种改善IGZO-TFT器件性能的有效方法。  相似文献   

6.
In this paper, top-gate thin-film transistors (TFTs) using amorphous In-Ga-Zn-O as the n-channel active layer and SiO2 as gate insulator were fabricated by radio frequency magnetron sputtering at room temperature. In this device, a SiO layer was used to be a buffer layer between active layer and gate insulator for preventing the damage of the InGaZnO surface by the process of sputtering SiO2 with relatively high sputtering power. The thickness of buffer layers was studied and optimized for enhancing the TFTs performances. Contrasting to the TFTs without buffer layer, the optimized thickness of 10 nm SiO buffer layer improved the top-gate TFTs performances greatly: mobility increases 30%, reached 1.29 cm2/V s, the Ion/Ioff ratio increases 3 orders, and the trap density at the interface of channel/insulator decreases about 1 order, indicated that the improvement of semiconductor/dielectric interface by buffering the sputtering power.  相似文献   

7.
Electrically pumped ultraviolet random lasing was achieved in metal-insulator-semiconductor (MIS) diodes based on ZnO films at room temperature. The ZnO films were grown by plasma assisted molecular beam epitaxy. Two different kinds of insulator layers, SiO x (0<x≤2) and AlO x (0<x≤1.5) were deposited by electron beam evaporation. X-ray diffraction experiments found these oxide layers were amorphous (or microcrystals), and X-ray photoelectron spectroscopy confirmed the Si and Al were fully oxidized. Compared with devices using SiO x as the insulator layer, diodes with evaporated AlO x layers showed a lower working threshold forward current (~20 mA to ~26 mA) and higher emission intensity. Periodic features indicating formation of closed-loop paths were deduced by the power Fourier transform of electroluminescence spectra. The cavity length of both devices increased as forward currents increased, while a larger cavity length was always obtained in the AlO x -involved device under the same working current. The improved performance was attributed to larger hole amount in AlO x layers. These results revealed that evaporated AlO x can serve as good electron blocking and hole supplying layers for hetero-structures.  相似文献   

8.
The impact of hydrogen desorption on the electrical properties of TiOx on crystalline silicon (c-Si) with SiOy interlayers is studied for the development of high-performance TiOx carrier-selective contacts. Compared with the TiOx/c-Si heterocontacts, a lower surface recombination velocity of 9.6 cm/s and lower contact resistivity of 7.1 mΩ cm2 are obtained by using SiOy interlayers formed by mixture (often called SC2). The hydrogen desorption peaks arising from silicon dihydride (α1) and silicon monohydride (α2) on the c-Si surface of the as-deposited samples are observed. The α1 peak pressure of as-deposited heterocontacts with SiOx interlayers is lower than that of heterocontacts without a SiOy interlayer. Furthermore, the hydrogen desorption energies are found to be 1.76 and 2.13 eV for the TiOx/c-Si and TiOx/SC2-SiOy/c-Si heterocontacts, respectively. Therefore, the excellent passivation of the TiOx/SC2-SiOy/c-Si heterocontacts is ascribed to the relatively high rupture energy of bonding between Si and H atoms.  相似文献   

9.
《Current Applied Physics》2015,15(4):452-455
We report on the optimization of the optical and electrical properties of IGZO/Ag/IGZO multilayer films as a function of IGZO thickness. The transmission window slightly widened and shifted toward lower energies with increasing IGZO thickness. The IGZO(39 nm)/Ag(19 nm)/IGZO(39 nm) showed transmittance 88.7% at 520 nm. The optical transmittance spectra were examined by finite-difference time-domain (FDTD) simulations. The carrier concentration decreased from 1.73 × 1022 to 4.99 × 1021 cm−3 with increasing the IGZO thickness, while the charge mobility insignificantly changed from 19.07 to 19.62 cm2/V. The samples had sheet resistances of 4.17–4.39 Ω/sq with increasing IGZO thickness, while the resistivity increased from 1.89 × 10−5 to 6.43 × 10−5 Ω cm. The 39 nm-thick IGZO multilayer sample had a smooth surface with a root mean square roughness of 0.63 nm. The IGZO(39 nm)/Ag(19 nm)/IGZO(39 nm) multilayer showed a Haacke's FOM of 49.94 × 10−3 Ω−1.  相似文献   

10.
An influence of electronic states at an insulator/GaN interface on the behavior of excess holes in an ultraviolet-illuminated metal/ SiO2/n-GaN structure has been studied by numerical simulations for weak (gate bias of −0.1 V ) and strong (−1 V ) depletion, in a wide range of excitation light intensities (from 1010 to 1020 photons cm−2 s−1) and for various bulk carrier lifetimes (from 1 to 100 ns). It has been found that the interface states with densities of 1012 eV −1 cm−2 dramatically reduce the total (integrated in the whole GaN layer) density of photogenerated holes and thus degrade the sensitivity of the metal/insulator/GaN-based photodetector.  相似文献   

11.
In this letter, indium–titanium–zinc–oxide thin-film transistors with zirconium oxide (ZrOx) gate dielectric were fabricated at room temperature. In the devices, an ultra-thin ZrOx layer was formed as the gate dielectric by sol–gel process followed by ultraviolet (UV) irradiation. The devices can be operated under a voltage of 4 V. Enhancement mode operations with a high field-effect mobility of 48.9 cm2/V s, a threshold voltage of 1.4 V, a subthreshold swing of 0.2 V/decade, and an on/off current ratio of 106 were realized. Our results demonstrate that UV-irradiated ZrOx dielectric is a promising gate dielectric candidate for high-performance oxide devices.  相似文献   

12.
李俊  周帆  张建华  蒋雪茵  张志林 《发光学报》2012,33(11):1258-1263
制备了基于反应溅射SiOx绝缘层的InGaZnO-TFT,并系统地研究了InGaZnO-TFT在白光照射下的稳定性,主要涉及到光照、负偏压、正偏压、光照负偏压和光照正偏压5种情况。结果表明,器件在光照和负偏压光照下的阈值偏移较大,而在正偏压光照情况下的阈值偏移几乎可以忽略。采用C-V方法证明阈值电压漂移是源于绝缘层/有源层附近及界面处的缺陷。另外,采用指数模式计算了缺陷态的弛豫时间。本研究的目的就是揭示InGaZnO-TFT在白光照射和偏压下的不稳定的原因。  相似文献   

13.
由于铟镓锌氧化物(IGZO) 薄膜具有高迁移率和高透过率的特点, 它作为有源层被广泛的应用于薄膜晶体管(TFT). 本文利用磁控溅射方法制备了TFT的有源层IGZO和源漏电极, 用简单低成本的掩膜法控制沟道的尺寸, 制备了具有高迁移率、底栅结构的n型非晶铟镓锌氧化物薄膜晶体管 (IGZO-TFT). 利用X 射线衍射仪(XRD) 和紫外可见光分光光度计分别测试了IGZO薄膜的衍射图谱和透过率图谱, 研究了IGZO薄膜的结构和光学特性. 通过测试IGZO-TFT的输出特性和转移特性曲线, 讨论了IGZO有源层厚度对IGZO-TFT特性的影响. 制备的IGZO-TFT器件的场效应迁移率高达15.6 cm2·V-1·s-1, 开关比高于107. 关键词: 非晶铟镓锌氧化物 薄膜晶体管 有源层  相似文献   

14.
The samples of Cu1−xPtxFeO2 (0 ≤ x ≤ 0.05) delafossite have been synthesized by solid-state reaction method to investigate their optical and electrical properties. The properties of electrical resistivity and Seebeck coefficient were measured in the high temperature ranging from 300 to 960 K, and the Hall effect and the optical properties were measured at room temperature. The obtained results of Seebeck showed the samples are p-type conductor. The optical properties at room temperature exhibited the samples are transparent visible light material with optical direct gap 3.45 eV. The low electrical resistivity, hole mobility and carrier density at room temperature displayed value ranging from 0.29 to 0.08 Ω cm, 1.8 to 8.6 cm2/V s and 1.56 × 1018 to 4.04 × 1019 cm−3, respectively. The temperature range for transparent visible light is below 820 K because the direct energy gap contains value above 3.1 eV. Consequently, the Cu1−xPtxFeO2 delafossite enhance performance for materials of p-type transparent conducting oxide (TCO) with low electrical resistivity.  相似文献   

15.
A reliable surface treatment for the pentacene/gate dielectric interface was developed to enhance the electrical transport properties of organic thin-film transistors (OTFTs). Plasma-polymerized fluorocarbon (CFx) film was deposited onto the SiO2 gate dielectric prior to pentacene deposition, resulting in a dramatic increase of the field-effect mobility from 0.015 cm2/(V s) to 0.22 cm2/(V s), and a threshold voltage reduction from −14.0 V to −9.9 V. The observed carrier mobility increase by a factor of 10 in the resulting OTFTs is associated with various growth behaviors of polycrystalline pentacene thin films on different substrates, where a pronounced morphological change occurs in the first few molecular layers but the similar morphologies in the upper layers. The accompanying threshold voltage variation suggests that hole accumulation in the conduction channel-induced weak charge transfer between pentacene and CFx.  相似文献   

16.
利用磁控溅射方法沉积双势垒磁性隧道结多层膜, 其中Al-O势垒层由等离子体氧化1 nm厚的 金属铝膜方式制备,然后采用深紫外光曝光和Ar离子刻蚀技术、微加工制备出长短轴分别为 6和3 μm大小的椭圆形双势垒磁性隧道结(DBMTJ),并在室温和低温下对其自旋电子输运 特性进行了研究. DBMTJ的隧穿磁电阻(TMR)比值在室温和42 K分别达到27%和423%, 结电阻分别为136 kΩ·μm2和175 kΩ·μm2,并在实验中观 察到平行状 态下存在低电阻态及共振隧穿效应,反平行态下呈现高电阻态以及TMR随外加偏压或直流电 流的增加而发生振荡现象. 由此,设计了一种基于这种双势垒磁性隧道结隧穿特性的自旋晶 体管. 关键词: 双势垒磁性隧道结 隧穿磁电阻 共振隧穿效应 自旋晶体管  相似文献   

17.
An intrinsic, carbon-rich a-SiC x :H thin film, prepared by the plasma-enhanced chemical vapour deposition (PECVD) technique, has been studied mainly by AC admittance and small-pulse deep-level transient spectroscopy (DLTS) measurements on an Al/a-SiC x :H/p-Si metal–insulator–semiconductor (MIS) structure. The effects of measurement temperature, voltage and small-signal AC modulation frequency on the MIS capacitor are qualitatively and quantitatively described. The kinetics of charge injection from the silicon substrate into the a-SiC x :H film, as a function of temperature and voltage bias stresses, are reported. Nearest-neighbour and variable-range hopping mechanisms are considered. An activation energy of ~?0.09?eV, and a density of states (DOS) of about 1019?cm?3/eV were found. The value of the DOS is in agreement with the effective interface DOS of above 1012?cm?2/eV assessed by both capacitance and DLTS measurements. The frequency (or temperature) dependence of the MIS capacitor over the whole DC voltage range is considered in detail. Single- and double-step carrier exchange mechanisms between the a-SiC x :H film and the silicon substrate, in the accumulation and depletion voltage regimes, respectively, are proposed.  相似文献   

18.
《Current Applied Physics》2015,15(4):535-540
Carrier injection and charge loss characteristics of nonvolatile memories with chemically-synthesized (CS) and vacuum-deposited (VD) gold nanoparticles (Au-NPs) have been investigated. Compared to CS counterparts, the memories with VD Au-NPs exhibit a higher dot density of 3.77 × 1011 cm−2, leading to a larger memory window. Further, the energy from valence-band edge to vacuum level (EVB_vac) of tunneling oxide for the samples with CS and VD Au-NPs is found to be 9.04 and 9.85 eV respectively. The small EVB_vac value of the memories with CS Au-NPs is resulted from the formation of a thin chemical oxide (SiOx) on thermally-grown SiO2 tunneling layer during the chemically synthesized process, contributing to a slow erasing behavior. Besides, the programming of the memories with VD Au-NPs is saturated at high gate bias, which has been well-explained by the electrons induced potential coupling between Au-NPs. Superior data retention property and high temperature dependence of charge loss are observed for the memories with CS Au-NPs, which can be ascribed to the thick tunneling oxide layer by the additional SiOx film.  相似文献   

19.
D* (Detectivity), an important figure of merit for photodetectors, is limited by zero bias resistance-area product (R0A). R0A is determined by Auger recombination mechanism, depending on the composition, temperature, carrier concentration and other parameters of the photodetectors. To investigate R0A of In1−xGaxAs infrared photodetectors, in this paper, theoretical analysis of Auger recombination mechanism was carried out in the room temperature, by taking CCCH, CHHL and CHHS into account. The calculated results show that there are significant influences on R0A for various parameters in both p- and n-type regions of the devices. With carrier concentration around 1017 to 1018 cm−3, R0A of 108 Ω cm2 (n-region) and 106 Ω cm2 (p-region) are obtained for x=0.47, when thickness and surface recombination velocity of the sample are 5 μm and 100 m/s, respectively.  相似文献   

20.
We investigate the ablation of SiO x thin films on fused silica substrates using single-pulse exposures at 193 nm and 248 nm. Two ablation modes are considered: front side (the surface of a film is irradiated from above) and rear side (a film is irradiated through its supporting substrate). Fluence is varied from below 200 mJ/cm2 to above 3 J/cm2. SiO x films of thickness 200 nm, 400 nm, and 600 nm are ablated. In the case of rear-side illumination, at moderate fluences (around 0.5 mJ/cm2) the ablation depth corresponds roughly to the film thickness, above 1 J/cm2 part of the substrate is ablated as well. In the case of front-side ablation the single-pulse ablation depth is limited for all film thicknesses to less than 200 nm even at fluences up to 4 J/cm2. Experimental results are discussed in relation to film thickness, fluence, and ablation mode. Simple numerical calculations are performed to clarify the influence of heat transport on the ablation process.  相似文献   

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