首页 | 本学科首页   官方微博 | 高级检索  
相似文献
 共查询到20条相似文献,搜索用时 31 毫秒
1.
M. Tao  J. Zhu 《Solid-state electronics》2004,48(12):2351-2352
The measurement of a negative or low Schottky barrier is complicated by several factors, including series resistance. With these factors in mind and additional experimental results, we reaffirm that the barrier height between Ti and Se-passivated n-type Si(0 0 1) is negative or nearly negative.  相似文献   

2.
Schottky barrier diodes (SBDs) were prepared by evaporation on H-terminated p-Si(1 0 0) surfaces. The Si(1 0 0)-H surfaces were obtained by wet chemical etching in diluted hydrofluoric acid. The current–voltage (IV) characteristics of real SBDs are described by using two fitting parameters that are the effective barrier height (EBH) and ideality factor n. They were determined from IV characteristics of SBDs (30 diodes) fabricated under experimentally identical conditions. The obtained values of EBHs varied from 0.729 to 0.749 eV, and the values of ideality factors varied from 1.083 to 1.119. The results showed that both parameters of SBDs differ from one diode to another even if they are identically prepared. The EBH distributions were fitted by two Gaussian distribution functions, and their mean values were found to be 0.739 ± 0.003 eV and 0.733 ± 0.001 eV, respectively. The homogeneous barrier height of SBDs was found to be 0.770 eV from the linear relationship between EBHs () and ideality factors (n).  相似文献   

3.
In this study, we investigated fabrication and characteristics of germanides Schottky contacts on germanium. Ti- and Ni-germanides were fabricated on n-Ge(1 0 0) substrates by sputtering metal Ti or Ni on Ge followed by a furnace annealing. The influence of annealing temperature on the electrical properties of Ti- and Ni-germanide on n-Ge(1 0 0) substrates was investigated. The low temperature ∼300 °C annealing helped to obtain the optimized Schottky contact characteristics in both Ti-germanide/Ge and Ni-germanide/Ge substrates contacts. The well-behaved Ti-germanides/n-Ge Schottky contact with 0.34 eV barrier height was obtained by using a 300 °C annealing process.  相似文献   

4.
By minimizing surface states with sulfur passivation, a record-high Schottky barrier is achieved with nickel on n-type Si(1 0 0) surface. Capacitance–voltage measurements yield a flat-band barrier height of 0.97 eV. Activation-energy and current–voltage measurements indicate ~0.2-eV lower barriers for the Ni/Si(1 0 0) junction. These results accompany a previously-reported record-high Schottky barrier of 1.1 eV between aluminum and S-passivated p-type Si(1 0 0) surface. The operation of these metal/Si(1 0 0) junctions changes from majority-carrier conduction, i.e., a Schottky junction, to minority-carrier conduction, i.e., a p–n junction, with the increase in barrier height from 0.97 eV to 1.1 eV. Temperature-dependent current–voltage measurements reveal that the Ni/S-passivated n-type Si(1 0 0) junction is stable up to 110 °C.  相似文献   

5.
氮气氛下衬底负偏压预溅射对GaAs肖特基势垒性能的改善   总被引:1,自引:1,他引:0  
本文研究了不同气氛下衬底负偏压预溅射对GaAs肖特基势垒特性的影响。我们发现,采用氮气氛下衬底负偏压预溅射新工艺能明显改善GaAs肖特基势垒特性:势垒高度增高,势垒电容减小和二极管反向击穿电压增大。这种新工艺对于GaAs肖特基势垒特性改善和GaAs MESFETs性能提高是一个非常有用的技术。  相似文献   

6.
This paper reports on estimating the Schottky barrier height of small contacts using a thermionic‐field emission model. Our results indicate that the logarithmic plot of the current as a function of bias voltage across the Schottky diode gives a linear relationship, while the plot as a function of the total applied voltage across a metal‐silicon contact gives a parabolic relationship. The Schottky barrier height is extracted from the slope of the linear line resulting from the logarithmic plot of current versus bias voltage across the Schottky diode. The result reveals that the barrier height decreases from 0.6 eV to 0.49 eV when the thickness of the barrier metal is increased from 500 Å to 900 Å. The extracted impurity concentration at the contact interface changes slightly with different Ti thicknesses with its maximum value at about 2.9×1020 cm?3, which agrees well with the results from secondary ion mass spectroscopy (SIMS) measurements.  相似文献   

7.
The transition from Schottky to ohmic contact in the nickel silicide/SiC system during annealing from 600 to 950 °C was investigated by measuring the electrical properties of the contact and by analyzing the microstructure of the silicide/SiC interface. The graphite clusters formed by carbon atoms during silicidation are uniformly distributed into the silicide layer after annealing at 600 °C and they agglomerate into a thin layer far from the silicide/SiC interface after annealing at 950 °C. At this temperature an increase of the Schottky barrier height was measured, while deep level transient spectroscopy evidences the absence of the 0.5 eV peak related to the carbon vacancies.  相似文献   

8.
Barrier height engineering of n-GaAs-based millimeter-wave Schottky diodes using strained InGaAs/GaAs and InGaP/GaAs heterostructures and a high doping surface layer is presented. The Schottky barrier height can be varied between Φfb=0.52 eV and Φfb=1.0 eV. The use of a pseudomorphic InGaAs layer and/or a thin high doping layer at the surface significantly reduces the Schottky barrier height. This is advantageous for low-drive zero bias mixing applications, A full quantum mechanical numerical calculation is presented to simulate the influence of different high doping layer thicknesses on the diode's dc characteristic. The theoretical results are compared with experimental results, For reverse bias applications (e.g., varactors) a barrier height and breakdown voltage enhancement is realized with a lattice matched InGaP/GaAs heterostructure. The barrier height value is determined by temperature dependent dc-measurements. The epitaxial layered structures are grown by molecular beam epitaxy. The diode devices are fabricated in a fully planar technology using selective oxygen implantation for lateral isolation. The diode's cut-off frequencies are in the THz-range  相似文献   

9.
The electrical characteristics of swift heavy ion (SHI) irradiated Au/n-Si (1 0 0) structure has been investigated in a wide temperature range (50–300 K). The forward bias current–voltage (IV) measurements have been used to extract the diode parameters as a function of temperature. The Zero-bias Schottky barrier height decreases with decreasing temperature. However, the flat-band barrier height is almost independent of the temperature. These results are interpreted using the models of Fermi level pinning. The behavior of Schottky diode parameters is explained by taking into account the role of the irradiation induced defects at Au/n-Si (1 0 0) interface.  相似文献   

10.
采用弹道电子发射显微术 ( BEEM)技术对超薄 Pt Si/Si、Co Si2 /Si肖特基接触特性进行了研究 ,并与电流 -电压 ( I- V)及电容 -电压 ( C- V)测试结果进行了对比 .研究了 Ar离子轰击对超薄Pt Si/n- Si肖特基接触特性的影响 .BEEM、I- V/C- V技术对多种样品的研究结果表明 ,I- V/C- V测试会由于超薄硅化物层串联电阻的影响而使测试结果产生严重误差 ;BEEM测试则不受影响 .随着离子轰击能量增大 ,肖特基势垒高度降低 ,且其不均匀性也越大 .用 BEEM和变温 I- V对超薄 Co Si2 /n- Si肖特基二极管的研究结果表明 ,变温 I- V测试可在一定程度上获得肖特基势垒  相似文献   

11.
We have investigated the crystalline orientation dependence of the electrical properties of Mn germanide/Ge(1 1 1) and (0 0 1) Schottky contacts. We prepared epitaxial and polycrystalline Mn5Ge3 layers on Ge(1 1 1) and (0 0 1) substrates, respectively. The Schottky barrier height (SBH) estimated from the current density-voltage characteristics for epitaxial Mn5Ge3/Ge(1 1 1) is as low as 0.30 eV, while the SBH of polycrystalline Mn5Ge3/Ge(0 0 1) is higher than 0.56 eV. On the other hand, the SBH estimated from capacitance-voltage characteristics are higher than 0.6 eV for both samples. The difference of these SBHs can be explained by the local carrier conduction through the small area with the low SBH regions in the epitaxial Mn5Ge3/Ge(1 1 1) contact. This result suggests the possibility that the lowering SBH takes place due to Fermi level depinning in epitaxial germanide/Ge(1 1 1) contacts.  相似文献   

12.
本文采用衬底负偏压溅射方法对比研究了ZrN薄膜及其与GaAs的肖特基势垒特性,结果表明,该法不仅能降低ZrN薄膜电阻率,而且能增高GaAs肖特基势垒高度.文中还用不同剂量的氮离子对GaAs衬底进行注入实验,可以看出,氮注入明显地改善了Ti/n-GaAs肖特基势垒特性.  相似文献   

13.
The characteristics of Ni/Si(1 0 0) solid-state reaction with yttrium (Y) addition are studied in this paper. Film stacks of Ti(20 nm)/TiN(40 nm)/Ni(8 nm)/Y(4 nm)/Ni(8 nm)/Si(1 0 0) and Ti(20 nm)/TiN(40 nm)/Ni(7 nm)/Y(6 nm)/Ni(7 nm)/Si(1 0 0) were prepared by physical vapor deposition. After solid-state reaction between metal films and Si was performed by rapid thermal annealing, various material analyses show that NiSi forms even with the addition of Y, and Ni silicidation is accompanied with Y diffusion in Ni film toward its top surface. The electrical characteristic measurements reveal that no significant Schottky barrier height modulation with the addition of Y occurs.  相似文献   

14.
The thermal stability of two commercially available silicon carbide Schottky diode types has been evaluated following a 1000 h non-biased storage test under vacuum at 350 °C. The Ti-based Schottky (Anode) contact shows excellent stability over the duration of the test with less than 5% change in either extracted Schottky barrier height or ideality values. The Al die attach metalisation on the anode also shows no evidence of degradation after the test. However, a considerable change in series resistance was observed for both diode types, with up to a factor of 100 measured for one of the diodes. The primary early failure mode is related to degradation of the NiAg Ohmic (cathode) die attach metalisation. Demixing of the NiAg alloy, leading to Ag agglomeration is proposed to be the underlying degradation mechanism involved resulting in delamination of the die attach metalisation and the corresponding series resistance increase.  相似文献   

15.
Theoretical models for the generation-recombination noise and trapping noise in metal-semiconductor Schottky barrier diodes are developed. Low-frequency excess noise in Schottky barrier diodes is found to be dominated by the modulation of the barrier height φB caused by fluctuation in the charge state of traps or generation-recombination centers. This noise mechanism does not occur in p-n junctions. The bias and the temperature dependence of the generation-recombination noise is critically compared with the experimental data for forward diode current ranges from 3 to 300 µA and operating temperatures from -25° to 100°C. Trapping noise in Schottky barrier diodes is observed at low temperatures in diodes not intentionally doped with deep level impurities. The experimental results on trapping noise can be described by assuming that the trap states have a constant capture cross section and are uniformly distributed in space, as well as in energy. The surface potential at the diode periphery also has an important effect on the Schottky barrier diode noise. The best low-frequency noise behavior is found when the surface is at the flat-band condition. An accumulated surface is always associated with a large amount of low-frequency excess noise.  相似文献   

16.
Mn/p-Si Schottky barrier diode (SBD) electrical parameters and interface state density have been investigated with current–voltage (IV) characteristics and Cheung's functions employing hydrostatic pressure. The interface state density of the diodes has an exponential growth with bias from the midgap towards the top of the valance band. We have seen that the Schottky barrier height (SBH) for Mn/p-Si SBD has a pressure coefficient of 1.61 meV/kbar (16.1 meV/GPa). We have reported that the p-type barrier height exhibited a weak pressure dependence, accepting that the Fermi level at the interface do not shift as a function of the pressure.  相似文献   

17.
提出了一种考虑Schottky结势垒不均匀性和界面层作用的Si C Schottky二极管( SBD)正向特性模型,势垒的不均匀性来自于Si C外延层上的各种缺陷,而界面层上的压降会使正向Schottky结的有效势垒增高.该模型能够对不同温度下Si C Schottky结正向特性很好地进行模拟,模拟结果和测量数据相符.它更适用于考虑器件温度变化的场合,从机理上说明了理想因子、有效势垒和温度的关系.  相似文献   

18.
To improve the Schottky contact performance and carrier confinement of GaAs metal-semiconductor-metal photodetectors (MSM-PDs), we employed the wide bandgap material, In/sub 0.5/(Al/sub 0.66/Ga/sub 0.34/)/sub 0.5/P, for the capping and buffer layers. We directly evaluated the Schottky contact parameters on the MSM-PD structure. The reverse characteristics of the Schottky contacts were examined by taking into account the Schottky barrier height depended on the electric field in the depletion region, and hence on the applied bias. The ideality factor and Schottky barrier height of Ti-Pt-Au contacts to In/sub 0.5/(Al/sub 0.66/Ga/sub 0.34/)/sub 0.5/P are 1.02 and 1.05 eV, respectively. Extremely low dark currents of 70 and 620 pA were obtained for these MSM-PDs when they were operated at a reverse bias of -10 V at room temperature and at 70/spl deg/C, respectively.  相似文献   

19.
In this study, the current-voltage characteristics of the AlCdO/unpolished p-type Si and AlCdO/polished p-type Si Schottky diodes with and without light illumination were examined. It is found that the Schottky barrier height (the series resistance) of the AlCdO/unpolished p-type Si Schottky diode is higher (lower) than that of the AlCdO/polished p-type Si Schottky diode. The power conversion efficiency of the AlCdO/p-type Si devices in the light (AM 1.5 G, 100 mW/cm2) was improved by increasing built-in potential at the AlCdO/p-type Si interfaces and reducing the device series resistance and surface reflectivity. It is shown that the device surface roughness plays an essential role in improving the device performance.  相似文献   

20.
Electron irradiation of the Au/n-Si/Al Schottky diode was performed by using 6 MeV electrons and 3 × 1012 e/cm2 fluency. The current-voltage (I-V), capacitance-voltage (C-V) and capacitance-frequency (C-f) characteristics of the unirradiated and irradiated Schottky diode were analyzed. It was seen that the values of the barrier height, the series resistance, and the ideality factor increased after electron irradiation. However, there was a decrease in the leakage current with electron irradiation. The increase in the barrier height and in the series resistance values was attributed to the dopant deactivation in the near-interface region. The interface states, Nss, have been decreased significantly after electron irradiation. This was attributed to the decrease in recombination centre and the existence of an interfacial layer. A decrease in the capacitance was observed after electron irradiation. This was attributed to decrease in the net ionized dopant concentration with electron irradiation.  相似文献   

设为首页 | 免责声明 | 关于勤云 | 加入收藏

Copyright©北京勤云科技发展有限公司  京ICP备09084417号