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1.
采用液氮冷却基片的气相沉积法,制备了 Cu-Ge 非晶薄膜。电阻测量及 TEM 形貌、电子衍射等分析表明,非晶态合金的形成能力及稳定性与成分密切相关。对 Cu_(100-x)Ge_x 合金膜,在x<25成分区,形成的非晶态稳定性差,晶化初期出现 fcc 结构的亚稳晶相;在 x>25成分区,有较高稳定性的非晶相形成,晶化后形成 Cu_3Ge 相。用合金化化学键效应观点解释了非晶态的形成、结构及结构转变行为。  相似文献   

2.
离子束混合制备非晶Sm-Fe-Zr合金薄膜   总被引:1,自引:0,他引:1  
采用离子束混合技术制备非晶Sm—Fe-Zr合金薄膜,在Sin的含量为x=400,300,200m/g的Sm—Fe多层薄膜中,注入能量为60KeV,剂量为1×1017ion/cm2的Zr+,研究非晶形成条件及合金薄膜的磁性能.实验发现:三种成分配比的样品在Zr+注入后磁性能皆发生明显的变化.X=400mg/g样品没有形成非晶,其主相为SmFe5;x=300,200mg/g样品形成非晶,且x=200mg/g样品晶化后形成一个面心结构未知相和α—Fe相  相似文献   

3.
一种富钛NiTi薄膜的晶化动力学   总被引:5,自引:0,他引:5  
本实验采用直流磁控溅射法制备了一种非晶的富TiNiTi薄膜,其成分为Ni46.34%(原子分数),Ti53.66%(原子分数)。采用变温方法研究了这种非晶薄膜的晶化动力学。测得非晶薄膜晶化的激活能为271kJ/mol,平均Avrami指数为1.17。采用以上获得的动力学参数计算了薄膜在773K的等温晶化动力学曲线。计算结果与实验结果吻合较好。在薄膜的晶化过程中伴随着Ti2Ni的析出。  相似文献   

4.
对非晶态 Li~+导体 B_2O_3—0.7Li_2O—0.7LiCl—0.1Al_2O_3在300℃温度下分相和晶化过程进行了扫描电镜(SEM)观察。结果表明;在等温处理的开始阶段,样品内首先发生分相,从母相中分离出均匀分布的新的非晶相粒子,随后长大和聚集;然后,新非晶相发生晶化长成晶粒,其成分为 Li_4B_7O_(12)Cl;最后,背景的非晶相中析出另一种晶粒,成分为 LiBO_2,并有较大的生长速度。  相似文献   

5.
综述了压力对非晶态合金的晶化行为的影响。首先介绍压力作用对不同类型晶化过程的作用,主要是晶化温度的变化,然后通过体积变化、原子扩散、界面和塑性变形几个方面分析压力如何影响非晶态固体晶化过程的。多数非晶合金体系表现出晶化温度随压力升高,热稳定性增加,说明原子扩散仍然是主要的影响因素。此外,少数非晶合金体系则需要考虑新生晶体/非晶界面的作用,在一定条件下,晶化温度反而随压力升高而下降。塑性变形也可以降低非晶的热稳定性。  相似文献   

6.
利用X射线衍射分析技术结合差示扫描量热仪,研究了Zr在Co-Si合金非晶薄膜晶化和相变过程中的作用.结果表明:溅射态非晶Co-Si薄膜和Co-Si-Zr薄膜在加热到950℃的过程中,均主要析出Co-Si和Co-Si2两种晶化相;Zr的加入增大了晶化激活能,抑制了晶化相的形核和长大,使薄膜能够在更高的温度范围保持稳定,但在高温800℃以上加热时,却使晶化相Co-Si向Co-Si2的转变加快.  相似文献   

7.
互不固溶系统的固态反应非晶化   总被引:2,自引:0,他引:2  
利用选区电子衍射和X射线衍射研究了互不固溶系统Cu-Ta和Cu-Nb纳米多层膜的固态反应非晶化的可能性,结果表明:当单层厚度减小到一定程度,成分为25~30%Cu的多层膜可以通过退火实现固态反应非晶化,从而获得具有正混合热系统的非晶薄膜,在Cu-Ta系统中还获得了厚0.8μm的非晶态薄膜,互不固溶系统多层膜固态反应非晶化的热力学驱动力主要源于多层膜界面自由能。  相似文献   

8.
采用聚焦脉冲激光研究了Ge2Sb2Te5薄膜在沉积和激光淬火两种非晶态下反射率与激光脉冲宽度变化的关系,发现沉积态的Ge2Sb2Te5薄膜在晶化触发阶段内的反射率随激光脉冲宽度增加而减小,经过激光淬火的非晶态Ge2Sb2Te5薄膜在晶化触发阶段内的反射率随激光脉冲宽度增加而变化平缓。本文借用气-液体系中过饱和度分析液滴形成的原理,从统计物理学角度详细研究了两种非晶态Ge2Sb2Te5薄膜在脉冲激光作用下的晶化过程及机理,结果表明,当Ge2Sb2Te5的非晶态程度处于未饱和或饱和状态时不形成晶核;当Ge2Sb2Te5的非晶态程度处于过饱和状态时,此时的Ge2Sb2Te5为亚稳态,可能形成大小不等的晶核,但只有半径大于临界晶核尺寸时才可能长大成晶粒,而应力降低晶化能垒,增加非晶态Ge2Sb2Te5的过饱和度是导致沉积态与激光淬火态的Ge2Sb2Te5薄膜在晶化触发阶段内反射率随激光脉冲宽度变化规律不一致的根本原因,并据此解释了Ge2Sb2Te5薄膜在这两种状态下的反射率随激光脉冲宽度的变化特点及规律。  相似文献   

9.
Zr对Pr-Fe-B非晶合金晶化形成纳米晶合金的作用   总被引:2,自引:0,他引:2  
从非晶合金化激活能的角度,分析了Pr-Fe-B非晶合金在退火过程中晶粒粗大的原因,揭示了Zr元素在其晶化过程中的作用,结果表明,Zr能改变Pr-Fe-B非晶合金中α-Fe相的晶化行为,有助于形成尺寸细小的α-Fe相。  相似文献   

10.
采用磁控溅射法制备TiNi非晶薄膜.通过X射线衍射(XRD)、透射电子显微镜(TEM)等方法研究了TiNi合金薄膜的组织形貌、电子衍射花样,并对其相变过程进行了动态观察.结果表明:态薄膜为非晶态,对其在515℃进行1 h的晶化处理后,薄膜中析出了TiNi3相;晶化处理后的TiNi合金薄膜加热到100℃时,薄膜中R相和马氏体相以切变方式完全转变为奥氏体;当冷却至室温时,是以R相、马氏体相以及少量的奥氏体相存在.其加热过程中的相变顺序为:马氏体相→R相→奥氏体相.冷却过程中的相变顺序为:奥氏体相→R相→马氏体相.  相似文献   

11.
CoSi2 thin films were prepared by annealing the amorphous Co-Si thin films. Zr was added into the amorphous thin film in order to investigate its effect on formation of CoSi2 thin film. It was found that Zr increased the crystallization nucleation barrier and accelerated the complete transformation of CoSi to CoSi2.  相似文献   

12.
Hsin CL  Yu SY  Wu WW 《Nanotechnology》2010,21(48):485602
Single-crystalline cobalt silicide/SiO(x) nanocables have been grown on Co thin films on an SiO(2) layer by a self-catalysis process via vapor-liquid-solid mechanism. The nanocables consist of a core of CoSi nanowires and a silicon oxide shell with a length of several tens of micrometers. In the confined space in the oxide shell, the CoSi phase is stable and free from agglomeration in samples annealed in air ambient at 900?°C for 1?h. The nanocable structure came to a clear conclusion that the thermal stability of the silicide nanowires can be resolved by the shell encapsulation. Cobalt silicide nanowires were obtained from the nanocable structure. The electrical properties of the CoSi nanowires have been found to be compatible with their thin film counterpart and a high maximum current density of the nanowires has been measured. One way to obtain silicate nanowires has been demonstrated. The silicate compound, which is composed of cobalt, silicon and oxygen, was achieved. The Co silicide/oxide nanocables are potentially useful as a key component of silicate nanowires, interconnects and magnetic units in nanoelectronics.  相似文献   

13.
采用射频磁控溅射法溅射CoSi2合金靶材制备CoSi2薄膜,研究了制备参数对薄膜织构的影响。结果表明,CoSi2薄膜中存在(111)或(220)织构。织构的形成受溅射参数的影响。溅射功率越大,溅射气压越低,(111)织构越强烈。当基底温度增加时,织构经历了先增强后减弱的过程。  相似文献   

14.
Cobalt silicide (CoSi) nanocrystal (NC) layer distributed within narrow spatial region is synthesized by thermal annealing of a sandwich structure comprised of a thin cobalt (Co) film sandwiched between two silicon-rich oxide (SiO(x)) layers. It is shown that the size of the CoSi NCs can be controlled by varying the Co film thickness, an increase in the size with increasing thickness. Capacitance-voltage (C-V) measurements on a test metal/oxide/semiconductor (MOS) structure with floating gate based on CoSi NCs of 3.8 nm in diameter and 1.4 x 10(12) cm2 in density are shown to have C-V characteristics suitable for nonvolatile memory applications, including a C-V memory window of about 9.5 V for sweep voltages between -15 V and +8, a retention time >10(8) s, and an endurance > 10(6) program/erase cycles.  相似文献   

15.
Epitaxial CoSi2 (001) layers, deposited on Si (001) substrate by molecular beam allotaxy (MBA), were used as substrate for diamond deposition in order to realise new applications. The results indicate that, in a microwave plasma chamber, diamond can be nucleated with a higher density on CoSi2 at lower temperatures using a bias enhanced method. High quality, [001]-textured diamond films can be synthesized on CoSi2 (001) using the [001] textured growth conditions. So far an epitaxial growth of diamond on CoSi2 cannot be observed. Statistically, a rotating angle distribution of diamond grains around the [001] axis in an [001]-textured film shows, however, preferred in-plane orientations of 13°, 22°, 45° and 77° relative to the CoSi2 [011]axis. The structural and chemical analyses show that no Co and Si element diffusion from the CoSi2 substrate into the diamond film can be detected.  相似文献   

16.
Reduced melting temperature of nanoparticles is utilized to deposit thin polycrystalline silicon (c-Si) films on plastic substrates by using a laser beam without damaging the substrate. An aqueous dispersion of 5 nm silicon nanoparticles was used as precursor. A Nd:YAG (1064 nm wavelength) laser operating in continuous wave (CW) mode was used for thin film formation. Polycrystalline Si films were deposited on flexible as well as rigid plastic substrates in both air and argon ambients. The films were analyzed by optical microscopy for film formation, scanning electron microscopy (SEM) for microstructural features, energy dispersive spectroscopy (EDS) for impurities, X-ray photoelectron spectroscopy (XPS) for composition and bond information of the recrystallized film and Raman spectroscopy for estimating shift from amorphous to more crystalline phase. Raman spectroscopy showed a shift from amorphous to more crystalline phases with increasing both the laser power and irradiation time during laser recrystallization step.  相似文献   

17.
The crystallization of amorphous, Si-rich, Au28Si72/glass thin film was studied in real-time synchrotron X-ray scattering experiments. The amorphous film crystallizes first into Au and Si phases at a low temperature of 206 degrees C. At annealing temperatures above eutectic temperature (T(E) = 360 degrees C), the Au phase melts while the Si phase rapidly grows further. The crystallized Au28Si72 thin film has nanowire-type grains with 1000-nm-length and 10-nm-diameter. We confirm that the Au liquid phase contributes to the low-temperature crystallization of the Si solid phase for Si-nanowire growth.  相似文献   

18.
In situ experiments on the Co/SiC interface reaction were carried out with a high temperature X-ray diffractometer capable of measuring the X-ray diffraction pattern in 1–4s using an imaging plate. The kinetic formation processes of the interface reaction layer were measured in short-period exposure experiments with the apparatus. The time-temperature phase diagram of Co/SiC in N2was determined. Co2Si and CoSi were formed at the Co/SiC interface between 921 and 1573 K in N2. The formation of CoSi obeyed the parabolic rate law. The value of the activation energy was 95 kJ/mol. The results of thermal expansion coefficient measurements suggest that when a sample is cooled to room temperature, compressive strain caused by CoSi occurs on SiC.  相似文献   

19.
We have investigated the stress behaviors and a mechanism of void formation in TiSix films during annealing. TiSix thin films were prepared by DC magnetron sputtering using a TiSi2.1 target in the substrate temperature range of 200–500 °C. The as-deposited TiSix films at low substrate temperature (<300 °C) have an amorphous structure with low stress of 1×108 dynes/cm2. When the substrate temperature increases to 500 °C, the as-deposited TiSix film has a mixture of C49 and C54 TiSi2 phase with stress of 8×109 dynes/cm2. No void was observed in the as-deposited TiSix film. Amorphous TiSix film transforms to C54 TiSi2 phase with a random orientation of (311) and (040) after annealing at 750 °C. The C49 and C54 TiSi2 mixture phase transforms to (040) preferred C54 TiSi2 phase after annealing over 650 °C. By increasing substrate temperature, the transformation temperature for C54 TiSi2 can be reduced, resulting in relieved stress of TiSi2 film. The easy nucleation of the C54 phase was attributed to an avoidance of amorphous TiSix phase. We found that amorphous TiSix→C54 TiSi2 transformation caused higher tensile stress of 2×1010 dynes/cm2, resulting in more voids in the films, than C49→C54 transformation. It was observed that void formation was increased with thermal treatment. The high tensile stress caused by volume decreases in the silicide must be relieved to retard voids and cracks during C54 TiSi2 formation.  相似文献   

20.
Kim HM  Jeong JW  Kwak CH  Lee SS 《Applied optics》1995,34(26):6008-6011
We present a method for binary phase spatial modulation that uses photoinduced anisotropy in a chalcogenide amorphous As(2)S(3) thin film and its application to binary phase-only filters in a VanderLugt optical correlator. The time-dependent light-transmission properties of the photoilluminated As(2)S(3) thin film are analytically examined by use of third-order nonlinear polarization theory. Experimental results on optical correlation are discussed.  相似文献   

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