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1.
李荣斌 《物理学报》2007,56(6):3428-3434
在不同实验条件下,用微波等离子体化学气相沉积(MPCVD)技术在Si基体上制备了S掺杂和B-S共掺杂CVD金刚石薄膜,利用X射线衍射仪和拉曼光谱仪研究掺杂对CVD金刚石薄膜的应力影响.研究结果发现,随着S掺杂浓度的增加,薄膜中sp2杂化碳含量和缺陷增多,CVD金刚石薄膜压应力增加;小尺寸的B原子与大尺寸的S原子共掺杂时,微量B的加入改变了CVD金刚石薄膜的应力状态,共掺杂形成B-S复合体进入金刚石晶体后降低金刚石晶体的晶格畸变程度,减少S原子在晶界上偏聚数量和晶体中非金刚石结构相含量,降低由于杂质、缺陷及sp2杂化碳含量产生的晶格畸变和薄膜压应力,提高晶格完整性. 关键词: 金刚石薄膜 掺杂 应力  相似文献   

2.
通过对Al2O3陶瓷衬底进行碳离子预注入,大大降低了Al2O3陶瓷衬底上金刚石薄膜的应力,且金刚石薄膜中的压应力随碳离子注入剂量的增加而线性下降.通过对Al2O3陶瓷衬底注入前后的对比分析表明,高能量的碳离子注入Al2O3陶瓷衬底以后,并没有产生过渡层性质的新相,而是大量累积在Al2O3晶格的间隙位,使Al2O3晶格发生畸变.而且,随着碳离子注入剂量的增加,Al2O3基体内晶格畸变加剧,注入层残余压应力也随之上升.当金刚石薄膜沉积以后,在降温的过程中衬底这部分残余应力得到释放,从而部分弛豫了金刚石薄膜中的 关键词: 金刚石薄膜 应力 离子注入 Al2O3陶瓷  相似文献   

3.
刘思宁  周艳文  沙天怡 《发光学报》2015,36(11):1300-1306
室温下在玻璃和聚酰亚胺两种不同衬底上, 采用射频磁控溅射法溅射掺铝氧化锌(AZO)粉末靶和固体Ag靶, 制备了两组AZO/Ag/AZO 3层透明导电薄膜, 研究了AZO层厚度对不同衬底3层膜结构和光电性能的影响.结果表明:不同衬底的两组AZO/Ag/AZO薄膜均为多晶膜.当Ag层厚度不变时, 随着AZO层厚度的增加, 两组薄膜电学性能变化不大, 透射峰向长波方向移动.玻璃和PI衬底上制备的AZO(30 nm)/Ag(14 nm)/AZO(30 nm)薄膜, 在550 nm处的透光率分别为85%和70%, 方块电阻分别为2.6 Ω/□和4.6 Ω/□.  相似文献   

4.
采用脉冲激光沉积技术制备了SrTiO3和SrNb0.2Ti0.8O3薄膜.X射线衍射分析表明在LaAlO3(100)单晶平衬底上生长的SrTiO3及SrNb0.2Ti0.8O3薄膜是沿[001]取向的近外延生长.随着氧压在一定范围内逐渐增大,SrTiO3薄膜的晶格参数减小,而SrNb0.2Ti0.8O3薄膜的晶格参数先减小后增大.同时摸索出制备具有二维电子气超晶格(SrTiO3/SrNb0.2Ti0.8O3).的最佳氧压为1.0×10-2Pa.另外在LaAlO3(100)倾斜衬底上制备的SrNb0.2Ti0.8O3薄膜中观察到激光感生热电电压效应.  相似文献   

5.
为研制真空紫外与极紫外波段Al基薄膜光学元件,详细研究了Al基薄膜的应力特性及其优化方法。利用应力实时测量装置对共溅射技术制备的5种不同Si掺杂质量分数(0、8.97%、16.49%、28.46%、45.73%)的Al-Si复合薄膜进行应力测试,并采用X射线衍射法表征薄膜的结晶状态。结果表明:Al薄膜中的应力表现为压应力,随着Si在Al中掺杂量的增加,Al中的压应力减小,并且Al的结晶度降低,Al(111)晶向的晶粒尺寸也减小,Al的结晶被抑制;当Si的掺杂质量分数从18.63%增大到31.57%时,Al中的压应力转变为张应力,且张应力随Si掺杂量的增加而进一步增大。本研究为制备Al基滤片、单层膜和多层膜元件提供了技术支撑,在极紫外光刻、同步辐射和天文观测领域具有重要的应用价值。  相似文献   

6.
超导薄膜所受的应力对其临界转变温度Tc具有重要的影响,研究应力对超导薄膜Tc的影响对获得更高Tc材料具有重要意义.本文采用溶胶-凝胶法,在LAO单晶基板上制备了Y2O3/YBCO薄膜,并研究了Y2O3缓冲层对不同厚度YBCO超导薄膜的临界转变温度的影响.研究发现,当YBCO薄膜厚度为90nm时,由于Y2O3和YBCO薄膜的晶格错配,在YBCO/Y2O3薄膜的a-b面内引入了压应力,增加了c轴的晶格常数,结果提高了YBCO薄膜的临界转变温度.当YBCO薄膜的厚度较大时(如230nm),由晶格错配引起的应力通过位错的形式得以释放,YBCO薄膜的Tc变化不大.  相似文献   

7.
采用射频磁控溅射的方法在SrTiO3(001,基片上制备了(La0.7Sr0.3MnO3)m(BiFeO3)n超晶格间隔的La0.7Sr0.3MnO3三明治结构.X射线衍射分析证明(La0.7Sr0.3MnO3)m(BiFeO3)n具有明显的超晶格结构.电流垂直于薄膜表面测得的电阻-温度关系表明.La0.7Sr0.3MnO3)m(BiFeO3)n超晶格薄膜在290 K有金属-绝缘体转变,略低于单层La0.7Sr0.3MnO3薄膜的转变温度.电流在0.01-10 mA范围内,观察到薄膜的峰值电阻随电流增大而减小,峰值变化率远大于单层La0.7Sr0.3MnO3薄膜,且随着超晶格周期厚度的增加而增大.低温下,电流-电压曲线表明其导电机制应主要为空间载子限制,且显示较大的电压偏置,表现出肖特基结的特性.  相似文献   

8.
通过x射线衍射方法研究了聚晶金刚石复合片中金刚石层内的宏观残余应力以及微观残余应力.宏观残余应力通过测量x射线衍射的峰值移动可以计算出来,微观残余应力由x射线衍射的峰形宽化决定.本文研究结果表明:我们研究的三种型号聚晶金刚石复合片中存在着宏观残余压应力和微观残余张应力,并且发现宏观残余压应力和微观残余张应力的大小随着金刚石平均粒径的增大而减小,根据x射线衍射研究表明这可能是由于随着金刚石粒径的增大,聚晶金刚石复合片中金刚石相的减少而非金刚石相的增加造成的.x射线衍射技术可以非破坏性的测量宏观和微观残余应力的大小,因此,这是一种很好的检测聚晶金刚石复合片中残余应力的方法,并可以通过应力的大小来优化聚晶金刚石复合片的最佳组分和工艺,同时也可以给出聚晶金刚石复合片的最佳工作条件.  相似文献   

9.
分别采用溶胶-凝胶法和脉冲激光沉积的方法制备了La0.67Sr0.33FexMn1-xO3(x=0, 0.05, 0.10, 0.15)系列块材和薄膜,研究了Fe部分替代对La0.67Sr0.33FexMn1-xO3薄膜输运和光诱导特性的影响.研究表明,随着Fe含量的增加,薄膜的峰值转变温度下降,导电性降低.在激光作用下,薄膜在TTP)则减小,随着Fe掺杂量的增加,光致电阻相对变化极值增加,当x=0.15时,光致电阻变化率极大值达到38%.并从晶格效应的角度讨论了光诱导薄膜电阻率变化的内在机理.  相似文献   

10.
沉积温度对氧化钇稳定氧化锆薄膜残余应力的影响   总被引:5,自引:3,他引:2  
采用自制掺摩尔分数12%的YzO2的ZrO2混合颗粒料为原料,在不同的沉积温度下用电子束蒸发方法沉积氧化钇稳定氧化锆(YSZ)薄膜样品.利用ZYGO MarkⅢ-GPI数字波面干涉仪对氧化钇稳定氧化锆薄膜的残余应力进行了研究,讨论了沉积温度对残余应力的影响.实验结果表明:随沉积温度升高,氧化钇稳定氧化锆薄膜中残余应力状态由张应力变为压应力.且压应力值随着沉积温度升高而增大;用X射线衍射仪表征了不同沉积温度下氧化钇稳定氧化锆薄膜的微观结构,探讨了薄膜微观结构与其应力的对应关系,并对比了纯ZrO2薄膜表现出的应力状念.  相似文献   

11.
Aluminum-doped ZnO(AZO) thin films with thin film metallic glass of Zr(50)Cu(50) as buffer are prepared on glass substrates by the pulsed laser deposition. The influence of buffer thickness and substrate temperature on structural, optical, and electrical properties of AZO thin film are investigated. Increasing the thickness of buffer layer and substrate temperature can both promote the transformation of AZO from amorphous to crystalline structure, while they show(100)and(002) unique preferential orientations, respectively. After inserting Zr(50)Cu(50) layer between the glass substrate and AZO film, the sheet resistance and visible transmittance decrease, but the infrared transmittance increases. With substrate temperature increasing from 25℃ to 520℃, the sheet resistance of AZO(100 nm)/Zr(50)Cu(50)(4 nm) film first increases and then decreases, and the infrared transmittance is improved. The AZO(100 nm)/Zr(50)Cu(50)(4 nm) film deposited at a substrate temperature of 360℃ exhibits a low sheet resistance of 26.7 ?/, high transmittance of 82.1% in the visible light region, 81.6% in near-infrared region, and low surface roughness of 0.85 nm, which are useful properties for their potential applications in tandem solar cell and infrared technology.  相似文献   

12.
赵显伟  郜小勇  陈先梅  陈超  赵孟珂 《中国物理 B》2013,22(2):24202-024202
The nitrogen doping of ZnO film deposited by the magnetron sputtering method is subsequently realized by the hydrothermal synthesis method.The nitrogen-doped ZnO film is preferably(002) oriented.With the increase of hexamethylenetetramine(HMT) solution concentration,the average grain size of the film along the 002 direction almost immediately decreases and then monotonously increases,conversely,the lattice strain first increases and then decreases.The structural evolution of the film surface from compact and even to sparse and rough is attributed to the enhanced nitrogen doping content in the hydrothermal process.The transmission and photoluminescence properties of the film are closely related to grain size,lattice strain,and nitrogen-related defect arising from the enhanced nitrogen doping content with HMT concentration increasing.  相似文献   

13.
用直流磁控溅射技术在石英基片上制备不同厚度(5nm~114nm之间)的铬膜.使用X射线衍射仪和分光光度计分别检测薄膜的结构和光学性质,利用德鲁特模型和薄膜的透射、反射光谱计算铬膜的厚度和光学常量,并采用Van der Pauw方法测量薄膜电学性质.结果表明:制备的铬薄膜为体心立方的多晶态,随着膜厚的增加,薄膜的结晶性能提高,晶粒尺寸增大;在可见光区域,当膜厚小于32nm时,随着膜厚的增加,折射率快速减小,消光系数快速增大,当膜厚大于32nm时,折射率和消光系数均缓慢减小并逐渐趋于稳定;薄膜电阻率随膜厚的增加为一次指数衰减.  相似文献   

14.
用直流磁控溅射技术在石英基片上制备不同厚度(5 nm~114 nm之间)的铬膜.使用X射线衍射仪和分光光度计分别检测薄膜的结构和光学性质,利用德鲁特模型和薄膜的透射、反射光谱计算铬膜的厚度和光学常量,并采用Van der Pauw方法测量薄膜电学性质.结果表明:制备的铬薄膜为体心立方的多晶态,随着膜厚的增加,薄膜的结晶性能提高,晶粒尺寸增大;在可见光区域,当膜厚小于32 nm时,随着膜厚的增加,折射率快速减小,消光系数快速增大,当膜厚大于32 nm时,折射率和消光系数均缓慢减小并逐渐趋于稳定;薄膜电阻率随膜厚的增加为一次指数衰减.  相似文献   

15.
张传军  邬云骅  曹鸿  高艳卿  赵守仁  王善力  褚君浩 《物理学报》2013,62(15):158107-158107
在科宁7059玻璃, FTO, ITO, AZO四种衬底上磁控溅射CdS薄膜, 并在CdCl2+干燥空气380 ℃退火, 分别研究了不同衬底和退火工艺对CdS薄膜形貌、结构和光学性能的影响. 扫描电子显微镜形貌表明: 不同衬底原位溅射CdS薄膜的形貌不同, 退火后相应CdS薄膜的晶粒度和表面粗糙度明显增大. XRD衍射图谱表明: 不同衬底原位溅射和退火CdS薄膜均为六角相和立方相的混相结构, 退火前后科宁7059玻璃, FTO, AZO衬底上CdS薄膜有 H(002)/C(111) 最强衍射峰, ITO衬底原位溅射CdS薄膜没有明显的最强衍射峰, 退火后出现 H(002)/(111) 最强衍射峰. 紫外-可见分光光度计分析表明: AZO, FTO, ITO, 科宁7059玻璃衬底CdS薄膜的可见光平均透过率依次减小, 退火后相应衬底CdS薄膜的可见光平均透过率增大, 光学吸收系数降低; 退火显著增大了不同衬底CdS薄膜的光学带隙. 分析得出: 上述结果是由于不同衬底类型和退火工艺对CdS多晶薄膜的形貌、结构和带尾态掺杂浓度改变的结果. 关键词: CdS薄膜 磁控溅射 退火再结晶 带尾态  相似文献   

16.
Al-doped ZnO (AZO) films prepared at different substrate temperature and AZO films with intentional Zn addition (ZAZO) during deposition at elevated substrate temperature were fabricated by radio frequency magnetron sputtering on glass substrate, and the resulting structural, electrical, optical properties together with the etching characteristics and annealing behavior were comparatively examined. AZO films deposited at 150 °C showed the optimum electrical properties and the largest grain size. XPS analysis revealed that AZO films deposited at elevated temperature of 450 °C contained large amount of Al content due to Zn deficiency, and that intentional Zn addition during deposition could compensate the deficiency of Zn to some extent. It was shown that the electrical, optical and structural properties of ZAZO films were almost comparable to those of AZO film deposited at 150 °C, and that ZAZO films had much smaller etching rate together with better stability in severe annealing conditions than AZO films due possibly to formation of dense structure.  相似文献   

17.
Bismuth films with different thicknesses have been grown by do sputtering on substrates held at room temperature. The films are always formed by columnar crystals with a grain size comparable to the film thickness which lead to surface roughness. It increases with the thickness of the films and has a strong influence on the film optical properties. The films have been irradiated with nanosecond laser pulses, and real-time reflectivity measurements during the irradiation were used to follow the changes in the film optical properties. It will be shown that pulsed-laser irradiation of films thinner than 100 nm improves substantially their surface roughness and their crystalline quality by increasing the grain size at least one order of magnitude.  相似文献   

18.
ZnO thin films were grown on c-plane sapphire and GaAs (001) substrates by metalorganic chemical vapor deposition. Atomic force microscopy and double-crystal X-ray diffractometry were utilized to investigate the structural properties of the ZnO films. The optical properties of ZnO films were also investigated in terms of time integrated and resolved photoluminescence (TIPL and TRPL). Large hexagonal crystallites and better crystalline quality were observed from the ZnO film on sapphire. Also, both the TIPL and TRPL showed a significant difference as the substrate changed. In particular, a detected sharp contrast in the result of TRPL measurement is due to the different defect structure and the lattice strain and stress of ZnO films on different substrates.  相似文献   

19.
功率密度对中频磁控溅射制备 AZO薄膜性能的影向   总被引:1,自引:0,他引:1  
利用中频磁控溅射法在普通玻璃衬底上沉积掺铝氧化锌(ZnO ∶ Al,简称AZO)薄膜,通过调整溅射功率密度参数得到沉积速率与功率密度之间的关系,制备了不同厚度的AZO薄膜.利用台阶仪、XRD、XPS、紫外可见分光光度计和Hall测试系统等方法研究了功率密度与厚度对AZO薄膜结构、组分、光学和电学性能的影响.实验结果表明...  相似文献   

20.
氢稀释对多晶硅薄膜结构特性和光学特性的影响   总被引:2,自引:0,他引:2       下载免费PDF全文
以SiCl4和H2为气源,用等离子体增强化学气相沉积技术,在250℃的低温下,研究氢稀释度对多晶硅薄膜结构特性的影响.实验结果表明,对于以SiCl4和H2组成的反应源气体,氢对薄膜生长特性的影响有异于SiH4/H2,在一定功率下,薄膜的晶化率随氢稀释度的减小而增加,在一定的氢稀释度下薄膜晶化度达到最大值85%;随着氢稀释度的继续减小,薄膜晶化度迅速下降,并逐渐向非晶态结构转变.随氢稀释度的减小,薄膜的光学带隙由 1.5eV减小至约1.2eV,而后增大至1.8eV.沉积速率则随氢稀释度的减小先增加后减小,在无氢条件下,无薄膜形成.在最佳氢稀释度条件下,Cl基是促进晶化度提高,晶粒长大的一个主要因素. 关键词: 多晶硅薄膜 微结构 氢稀释 4')" href="#">SiCl4  相似文献   

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