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1.
利用直流脉冲磁控溅射法在室温下制备无氢SiNx薄膜.通过傅里叶变换红外光谱、台阶仪、紫外—可见分光光度计、接触角测量仪、透湿测试仪等表征技术,分析了N2流量、Si靶溅射功率等实验参数对SiNx薄膜成分、结构、及阻透性能、透光性能、接触角等性能的影响.研究结果表明,Si靶溅射功率固定时,在低N2流量条件下,或N2流量固定时,在高Si靶溅射功率条件下,制备的SiN 关键词x')" href="#">SiNx 磁控溅射 微观结构 阻透性能  相似文献   

2.
丁万昱  徐军  陆文琪  邓新绿  董闯 《物理学报》2008,57(8):5170-5175
利用微波电子回旋共振增强磁控反应溅射法在不同基片温度下制备无氢SiNx薄膜.通过傅里叶变换红外光谱、透射电子显微镜、台阶仪、纳米硬度仪等表征技术,研究了基片温度对SiNx薄膜结晶状态、晶粒尺寸、晶体取向等结晶性能以及薄膜的生长速率、硬度等机械性能的影响,并探讨了薄膜结晶性能与机械性能之间的关系.研究结果表明,在基片温度低于300℃时制备的SiNx薄膜以非晶状态存在,硬度值仅为18GPa左右;基片温度 关键词x')" href="#">SiNx 磁控溅射 微观结构 硬度  相似文献   

3.
在室温下,采用射频磁控溅射法制备了Cu/TiOx纳米晶复合薄膜.利用X射线粉末衍射(XRD)、X射线光电子能谱(XPS)对其结构进行表征,并研究了Cu/TiOx复合薄膜的UV-vis吸收谱和亲水性.结果表明,退火前后薄膜中钛元素皆以Ti3+形式存在.薄膜在可见区有吸收,吸收限为600 nm左右.Cu/TiOx复合薄膜具有良好的亲水性.这主要是由于Cu的掺杂,使得薄膜的性能的亲水性变好. 关键词x复合薄膜')" href="#">Cu/TiOx复合薄膜 射频磁控溅射 XPS 亲水性  相似文献   

4.
丁万昱  徐军  陆文琪  邓新绿  董闯 《物理学报》2009,58(6):4109-4116
利用微波电子回旋共振等离子体增强非平衡磁控溅射法在不同N2流量下制备无氢SiNx薄膜.通过X光电子能谱、纳米硬度仪等表征技术,研究了不同N2流量下制备的SiNx薄膜的化学键结构、化学键含量、元素配比及各元素沿深度分布.研究结果表明,N2流量是影响SiNx薄膜化学键结构、元素配比、元素延深度分布等性质的主要因素.在N2关键词: x')" href="#">SiNx 磁控溅射 XPS 化学键结构  相似文献   

5.
采用脉冲激光沉积方法在单晶Si(100)衬底上制备出c轴取向的Zn1-xMgxO单晶薄膜,通过荧光光谱仪研究了薄膜的光致发光特性.实验结果表明,Mg含量增加,Zn1-xMgxO单晶薄膜的紫外发光峰蓝移,发光峰强度减弱,缺陷发光强度增强.同时发现,由于Mg的掺杂,引入了一些束缚能较大的局域束缚态.对于氧气氛下制备的样品,实验发现紫外峰和绿光带发光峰同时增强,但是R值减小,紫外峰红移.对绿光发光机理研究发现,绿光发光带主要与锌空位、氧间隙(Oi)或锌位氧(OZn)等缺陷有关,它是由多个缺陷发光峰组成,各缺陷发光峰强度相对变化导致了绿光发光带的整体移动. 关键词: 1-xMgxO薄膜')" href="#">Zn1-xMgxO薄膜 光致发光 脉冲激光沉积  相似文献   

6.
The formation of silicon nanoclusters embedded in amorphous silicon nitride (SiNx:H) can be of great interest for optoelectronic devices such as solar cells. Here amorphous SiNx:H layers have been deposited by remote microwave-assisted chemical vapor deposition at 300 °C substrate temperature and with different ammonia [NH3]/silane [SiH4] gas flow ratios (R=0.5−5). Post-thermal annealing was carried out at 700 °C during 30 min to form the silicon nanoclusters. The composition of the layers was determined by Rutherford back scattering (RBS) and elastic recoil detection analysis (ERDA). Fourier transform infrared spectroscopy (FTIR) showed that the densities of SiH (2160 cm−1) and NH (3330 cm−1) molecules are reduced after thermal annealing for SiN:H films deposited at flow gas ratio R>1.5. Breaking the SiH bonding provide Si atoms in excess in the bulk of the layer, which can nucleate and form Si nanostructures. The analysis of the photoluminescence (PL) spectra for different stoichiometric layers showed a strong dependence of the peak characteristics (position, intensity, etc.) on the gas flow ratio. On the other hand, transmission electron microscopy (TEM) analysis proves the presence of silicon nanoclusters embedded in the films deposited at a gas flow ratio of R=2 and annealed at 700 °C (30 min).  相似文献   

7.
袁贺  孙长征  徐建明  武庆  熊兵  罗毅 《物理学报》2010,59(10):7239-7244
针对光电子器件端面抗反镀膜的要求,研究了基于等离子体增强化学气相沉积(PECVD)技术的多层抗反膜的设计和制作.首先,对影响SiNx折射率的因素进行了实验研究,确定了具有大折射率差的SiO2/SiNx材料的PECVD沉积条件.根据理论计算分析,设计了四层SiO2/SiNx抗反膜结构,能够在70 nm的波长范围内实现低于10-4的反射率  相似文献   

8.
利用脉冲激光沉积方法制备出了具有室温铁磁性的Ni1-xFexO(x=0.02,0.05)稀磁半导体.X射线衍射(XRD)结果表明Ni1-xFexO的晶体结构为NaCl结构,并且在Fe含量较高的Ni0.95Fe0.05O中出现了少量的α-Fe2O3物相.X射线吸收近 关键词: 1-xFexO')" href="#">Ni1-xFexO XANES 脉冲激光沉积方法  相似文献   

9.
SiCxNy thin films with different nitrogen contents were deposited by way of incorporation of different amounts of nitrogen into SiC0.70 using unbalanced reactive dc magnetron sputtering method. Their phase configurations, nanostructures and mechanical behaviors were investigated by X-ray diffraction (XRD), X-ray photoelectron spectroscopy (XPS), Raman spectroscopy, high-resolution transmission electron microscopy (HRTEM) and microindentation methods. The result indicated SiC0.70 and all SiCxNy thin films exhibited amorphous irrespective of the nitrogen content. The phase configuration and mechanical behaviors of SiCxNy thin films strongly depended on nitrogen content. SiC0.70 exhibited a mixture consisting of SiC, Si and a small amount of C. Incorporated nitrogen, on one hand linked to Si, forming SiNx, on the other hand produced CNx and C at the expense of SiC. As a result, an amorphous mixture consisting of SiC, SiNx, C and CNx were produced. Such effects were enhanced with increase of nitrogen content. A low hardness of about 16.5 GPa was obtained at nitrogen-free SiC0.70. Incorporation of nitrogen or increase of nitrogen content increased the film hardness. A microhardness maximum of ∼29 GPa was obtained at a nitrogen content of 15.7 at.%. This value was decreased with further increase of N content, and finally a hardness value of ∼22 GPa was obtained at a N content of ∼25 at.%. The residual compressive stress was consistent with the hardness in the nitrogen content range of 8.6-25.3 at.%.  相似文献   

10.
李红凯  林国强  董闯 《物理学报》2008,57(10):6636-6642
用脉冲偏压电弧离子镀通过控制不同的氮流量在(100)单晶Si基片上制备了不同成分的CNx薄膜.用光学显微镜,XPS,XRD,激光Raman和Nanoindenter等方法研究了薄膜的形貌、成分、结构和性能.结果表明,薄膜表面平整致密、氮含量随着氮流量的降低而降低、结构为非晶且为类金刚石薄膜;随着氮含量从18.9%降低到5.3%(摩尔百分比,全文同),薄膜的硬度和弹性模量单调增加而且增幅较大,其中硬度从15.0 GPa成倍增加到30.0 GPa;通过氮流量的调整能够敏感地改变薄膜中的sp3键的含量,是CNx薄膜的硬度和弹性模量获得大幅度调整的本质原因. 关键词x薄膜')" href="#">CNx薄膜 脉冲偏压 电弧离子镀 硬度  相似文献   

11.
采用化学共沉淀法制备了不同Ba2+掺杂浓度、 不同煅烧温度的Sr0.8-xBaxEu0.2WO4红色荧光粉. 研究了样品的晶体取向和晶格 畸变对发光性质的影响, 实验结果表明: 合成的Sr0.8-xBaxEu0.2WO4红色荧光粉为四方相, 样品中Eu3+5D07F2跃迁的红光能被近紫外光和蓝光有效激发. 适量的Ba2+离子取代部分的Sr2+提高了Sr0.8Eu0.2WO4荧光粉的发光强度, Ba2+掺杂浓度的改变对基质的晶格参数、晶体对称性和发光性能影响较大, Ba2+的最佳掺杂量为30%.  相似文献   

12.
利用X射线衍射(XRD)和X射线吸收近边结构(XANES)方法研究了在Si(100)衬底上及600℃温度条件下用分子束外延(MBE)共蒸发方法生长的MnxSi1-x磁性薄膜的结构.由XRD结果表明,只有在高Mn含量(8%和17%)样品中存在着Mn4Si7化合物物相.而XANES结果则显示,对于Mn浓度在0.7%到17%之间的MnxSi1-x样品,其Mn原子的XANES谱表现出了一致的谱线特征.基于多重散射的XANES理论计算进一步表明,只有根据Mn4Si7模型计算出的理论XANES谱才能够很好的重构出MnxSi1-x样品的实验XANES谱.这些研究结果说明在MnxSi1-x样品中,Mn原子主要是以镶嵌式的Mn4Si7化合物纳米晶颗粒存在于Si薄膜介质中,几乎不存在间隙位和替代位的Mn原子. 关键词xSi1-x磁性薄膜')" href="#">MnxSi1-x磁性薄膜 分子束外延 XRD XANES  相似文献   

13.
We have developed a terahertz time-domain spectroscopy (THz-TDS) system for reflectivity measurement with a temperature-controllable cryostat. For emission and detection of THz radiation, a Ti:Sapphire pulsed laser and photoconductive antennas are used. Two wire-grid polarizers enable us to carry out the polarized reflectivity measurements. Using our THz-TDS system, we measured the c-axis polarized reflectivity spectra for La2−xSrxCuO4 single crystals (x = 0.10 and 0.13) and observed sharp Josephson plasma edges for both samples below Tc. The reflectivity spectra of the x = 0.10 sample were in good agreement with those reported previously, which confirms the validity of the system. For the x = 0.13 sample, we discuss the anomolous features of the optical spectra.  相似文献   

14.
利用倾斜衬底沉积法在无织构的金属衬底上生长了MgO双轴织构的模板层,在这一模板层上实现了YBa2Cu3O7-x薄膜的外延生长.在外延YBa2Cu3O7-x薄膜前,依次沉积了钇稳定的立方氧化锆和CeO2作为缓冲层.利用X射线衍射2θ扫描、扫描、Ω扫描和极图分析测定了这些膜的结构和双轴织 关键词: 2Cu3O7-x镀膜导体')" href="#">YBa2Cu3O7-x镀膜导体 2缓冲层')" href="#">CeO2缓冲层 厚度依赖性 外延生长  相似文献   

15.
纳元元  王聪  褚立华  丁磊  闫君 《物理学报》2012,61(3):36801-036801
采用对靶磁控溅射方法在单晶Si(100)基片上制备了反钙钛矿结构的Mn3CuNx薄膜.通过控制制备过程中的反应气体氮气(N2) 流量(N2/Ar+N2), 研究了氮含量对Mn3CuNx薄膜结构及物理性能的影响.分别利用X射线衍射仪、俄歇电子能谱、 原子力显微镜、X射线光电子能谱、物理性能测试系统和超导量子干涉仪, 对所制备薄膜的晶体结构、成分、表面形貌和电、磁输运性质进行了测试.结果表明:制备的薄膜均为反钙钛矿立方结构,且沿 (200) 晶面择优生长.随着氮含量的增大,薄膜表面粗糙度和颗粒度尺寸逐渐增大, 导致电阻率增加.氮含量对薄膜的电输运性质没有影响,所有薄膜电阻率均随着温度的降低逐渐增大, 呈现半导体型导电行为,这与对应的块体材料结果相反.Mn3CuNx薄膜随着测试温度的增大发生了 亚铁磁到顺磁的磁转变,且N含量的增大降低了磁有序转变温度,主要是由于N缺陷对Mn6N八面体结构中 磁交换作用的影响所致.  相似文献   

16.
采用脉冲激光沉积(PLD)方法在单晶Si(100)衬底上沿c轴方向生长单晶Zn1-xMgxO薄膜,通过X射线衍射(XRD)、原子力显微镜(AFM)、扫描电镜(SEM)和荧光光谱(PL)研究了膜厚、Mg含量、退火温度及氧气氛等制备工艺对Zn1-xMgxO薄膜的结构、形貌和光学性质的影响.实验结果表明,Mg含量x≤0.15时, Zn关键词: 1-xMgxO薄膜')" href="#">Zn1-xMgxO薄膜 制备工艺 结构 光学性质  相似文献   

17.
利用X射线吸收精细结构、X射线衍射和磁性测量等技术研究脉冲激光气相沉积法制备的Zn1-xCoxO (x=0.01,0.02)稀磁半导体薄膜的结构和磁性.磁性测量结果表明Zn1-xCoxO样品都具有室温铁磁性.X射线衍射结果显示其薄膜样品具有结晶良好的纤锌矿结构.荧光X射线吸收精细结构测试结果表明,脉冲激光气相沉积法制备的样品中的Co离子全部进入ZnO晶格中替代了部分Zn的格点位置,生成单一相的Zn1-xCoxO 稀磁半导体.通过对X射线吸收近边结构谱的分析,确定Zn1-xCoxO薄膜中存在O空位,表明Co离子与O空位的相互作用是诱导Zn1-xCoxO产生室温铁磁性的主要原因. 关键词: 1-xCoxO稀磁半导体')" href="#">Zn1-xCoxO稀磁半导体 X射线吸收精细结构谱 脉冲激光气相沉积法  相似文献   

18.
Ba(Ti1−x,Nix)O3 thin films were prepared on fused quartz substrates by a sol–gel process. X-ray diffraction and Raman scattering measurements showed that the films are of pseudo-cubic perovskite structure with random orientation and the change of lattice constant caused by Ni-doping with different concentrations is very small. Optical transmittance spectra indicated that Ni-doping has an obvious effect on the energy band structure. The energy gap of Ba(Ti1−x,Nix)O3 decreased linearly with the increase of Ni concentration. It indicates that the adjusting of band gap can be achieved by controlling the Ni-doping content accurately in Ba(Ti1−x,Nix)O3 thin films. This has potential application in devices based on ferroelectric thin films.  相似文献   

19.
樊继斌  刘红侠  马飞  卓青青  郝跃 《中国物理 B》2013,22(2):27702-027702
A comparative study of two kinds of oxidants(H2O and O3) with the combinations of two metal precursors [trimethylaluminum(TMA) and tetrakis(ethylmethylamino) hafnium(TEMAH)] for atomic layer deposition(ALD) hafnium aluminum oxide(HfAlOx) films is carried out.The effects of different oxidants on the physical properties and electrical characteristics of HfAlOx films are studied.The preliminary testing results indicate that the impurity level of HfAlOx films grown with both H2O and O3 used as oxidants can be well controlled,which has significant effects on the dielectric constant,valence band,electrical properties,and stability of HfAlOx film.Additional thermal annealing effects on the properties of HfAlOx films grown with different oxidants are also investigated.  相似文献   

20.
Aligned CNx nanotubes were fabricated by pyrolyzing ethylenediamine on p-type Si(1 1 1) substrates using iron as the catalyst. Scanning electron microscopy (SEM), high-resolution transmission electron microscopy (HRTEM), X-ray photoelectron spectrum (XPS) and Raman spectroscopy were used to characterize the CNx nanotubes. The CNx nanotubes with the average length of 20 μm and diameters in the range of 50–100 nm have the “bamboo-like” structure and worse crystalline order. The low-field emission measurements of the CNx nanotubes indicated that 20 μA/cm2 current densities were observed at an electric field of 1.4 V/μm and 1.280 mA/cm2 were obtained at 2.54 V/μm. The CNx nanotubes exhibit better field emission properties than the carbon nanotubes and the BCN nanotubes. The emission mechanism of CNx nanotubes is also discussed.  相似文献   

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