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1.
With the increase of magnetic storage density, the thickness of the protective diamond like carbon (DLC) film on the surfaces of head and disk is required as thin as possible. In this paper, the structure, mechanical properties and corrosion and oxidation resistance of ultra-thin DLC films are investigated. The ultra-thin DLC films were deposited by using filtered cathodic vacuum arc (FCVA) technique. The exact thickness of the ultra-thin DLC film was determined by high resolution transmission electron microscope (HRTEM). Raman analysis indicates that the ultra-thin DLC film presents ta-C structure with high sp3 fraction. In the wear test, a diamond tip was used to simulate a single-asperity contact with the film surface and the wear marks were produced on the film surface. The wear depths decrease with film thickness increasing. If the film thickness was 1.4 nm or above, the wear depth was much lower than that of Si substrate. This indicates that the ultra-thin DLC film with thickness of 1.4 nm shows excellent wear resistance. Corrosion tests in water and oxidation tests in air were carried out to investigate the diffusion barrier effect of the ultra-thin DLC films. The results show that the DLC film with thickness of 1.4 nm provides adequate coverage on the substrate and has good corrosion and oxidation resistance. 相似文献
2.
紫外光下纳米TiO2薄膜亲水性机理的电化学研究 总被引:6,自引:0,他引:6
利用溶胶 凝胶方法在透明导电玻璃ITO (SnO2 ∶In)表面制备纳米TiO2 薄膜 ,XRD谱图表明TiO2 是锐钛矿晶型 ,AFM (Atomic Force Microscope)测得薄膜表面粒子约为 10 0nm .研究了ITO表面纳米TiO2 薄膜的光致亲水性变化 .通过循环伏安技术测定TiO2 薄膜电极在 2 5 3.7nm的紫外光照射后的电化学行为推测光致亲水性机理 .发现在紫外光照射一定时间后 ,TiO2 薄膜电极的循环伏安图在 +0 .0 35V处出现新的氧化峰 ;且随光照时间的增加 ,氧化峰的峰电流增大 ,溶液中的溶解氧对峰电流的大小有明显影响 .实验表明 ,在紫外光照下电极表面有Ti3 + 产生 ,证实了TiO2 薄膜的光致亲水性转变过程与Ti3 + 的生成导致的表面结构变化有关 相似文献
3.
Qian Xinming Zhang Xintong Bai Yubai Li Tiejin Tang Xinyi Wang Erkang Dong Shaojun 《Journal of nanoparticle research》2000,2(2):191-198
-Fe2O3 single crystal thin films have been prepared from 45nm diameter colloid. These thin nanocrystalline films exhibit a typical behavior of n-type semiconductor material because of the anodic photocurrent generation. The anodic photocurrent response upon illumination and the reversal spike of cathodic current upon the light switched off suggests that the electrons can flow in both directions and no space charge layer exists at the thin film/electrolyte interface. The decreased photocurrent responses of thicker films can be explained by the electric resistance effect and recombination effect. Moreover, the thicker film will lead to a poor photocurrent response for short wavelength light. Considering the use of sunlight, the thin film thickness should be controlled to an optimal value. 相似文献
4.
水杨醛缩苯胺锌及其薄膜的谱学性能 总被引:2,自引:2,他引:0
合成了一种新型的发光材料水杨醛缩苯胺锌(SAZ),利用真空热蒸镀制备了高质量、纳米级薄膜,利用红外光谱、差热-热重谱、X射线衍射谱、UV-Vis吸收谱、荧光光谱研究了水杨醛缩苯胺锌及其薄膜的结构、晶态、热稳定性以及光学特性,并利用循环伏安法、UV-Vis吸收谱确定了该材料的能级结构。结果表明,水杨醛缩苯胺锌无定性薄膜具有较高的热稳定性,在紫外光激发下产生绿色荧光,色纯度高, 亮度高。水杨醛缩苯胺锌薄膜在大气环境下存放,荧光衰减比8-羟基喹啉铝快,但受紫外光照射时,荧光衰减比8-羟基喹啉铝慢。水杨醛缩苯胺锌的HOMO能级为-5.659 eV,LUMO能级为-3.054 eV,禁带宽度为2.604 eV。 相似文献
5.
M. Skibowski B. Feuerbacher Dr. W. Steinmann R. P. Godwin 《Zeitschrift für Physik A Hadrons and Nuclei》1968,211(4):342-351
Measurements of the photocurrent from thin Al cathodes in a windowless electron multiplier as a function of wavelength, polarization, angle of incidence, and film thickness have been carried out in the extreme vacuum ultraviolet. A normal incidence monochromator utilizing synchrotron radiation provided highly polarized light. A marked difference is found between the photocurrent measured during irradiation of thin films with “s” and “p” polarized light at wavelengths near the Al plasma wavelength (835 Å). For films thicker than about 500 Å pronounced interference effects are found in both “p” and “s” light at wavelengths less than the plasma wavelength. The observations can be explained by assuming the photocurrent is related to the photon density (electromagnetic energy density) in the photocathode. Calculations of the energy density in films irradiated with light give the structure found in the measured photocurrent. The measurements indicate our monochromator yields light with a degree of polarization consistent with the calculated polarization of the synchrotron radiation incident upon our grating (about 85%). 相似文献
6.
《中国物理快报》2016,(10)
Silver films(Ag) and silver-gold films(Ag-Au) with thickness ~15nm are coated on Bk7 glasses through thermal evaporation.After doping gold of 5.2%,the grain size of the Ag film reduces from 13.6nm to 9.1nm,also the surface roughness decreases from 1.45 nm to 0.94 nm.A UV lamp is used as the irradiation light source to accelerate the corrosion process in the atmosphere.After 17 h irradiation,the pure silver film surface turns dark,and the transmittances reduce from 350 nm to 500 nm,while the Ag-Au film degrades much less,almost negligibly after UV radiation.Additional x-ray photoelectron spectroscopy and atomic force micrographs data are provided to show atomic content of Sims and their surface morphologies.It is suggested that small grain size and high packing density of alloy film prevent reaction of silver with oxygen in the atmosphere,which leads to high stability of the Ag-Au Elm. 相似文献
7.
Tin oxide (non-doped) films have been prepared by a photochemical vapour deposition (photo-CVD) from Tetramethyltin (TMT) (Sn(CH3)4) and O2 (containing O3). A low-pressure mercury lamp was used as the light source. The effect of the UV light irradiation on the film thickness distribution along 5 cm×5 cm area was examined. By piling Teflon films on the surface of the suprasil window, the light intensity of 184.9 nm UV wavelength of the low-pressure mercury lamp was controlled, while that of 253.7 nm wavelength through the Teflon hardly changed. As a result, the uniformity of the film thickness distribution was improved as the light intensity (184.9 nm) increased. The UV 184.9 nm light irradiation may have improved the uniformity of the reactive species distribution in the vapour phase, which may result in the formation of the uniform thickness distribution. 相似文献
8.
The effect of substrate roughness on growth of ultra thin diamond-like carbon (DLC) films has been studied. The ultra thin DLC films have been deposited on silicon substrates with initial surface roughness of 0.15, 0.46 and 1.08 nm using a filted cathodic vacuum arc (FCVA) system. The films were characterized by Raman spectroscope, transmission electron microscope (TEM) and atomic force microscopy (AFM) to investigate the evolution of the surface roughness as a function of the film thickness. The experimental results show that the evolution of the surface morphology in an atomic scale depends on the initial surface morphology of the silicon substrate. For smooth silicon substrate (initial surface roughness of 0.15 nm), the surface roughness decreased with DLC thickness. However, for silicon substrate with initial surface roughness of 0.46 and 1.08 nm, the film surface roughness decreased first and then increased to a maximum and subsequently decreased again. The preferred growth of the valley and the island growth of DLC were employed to interpret the influence of substrate morphology on the evolution of DLC film roughness. 相似文献
9.
碘化铯膜层对紫外光以及X射线具有很高的光电转换效率,但在空气中容易发生潮解。介绍了微通道板碘化铯膜层抗潮解超薄保护膜层的制备与保护效果。使用扫描式电子显微镜(scanning electron microscope,SEM)对碘化铯薄膜光阴极微通道板的镀膜深度和厚度进行测试,采用氧化铝作为碘化铯薄膜光阴极的保护膜层,并分别制备了厚度为2 nm、5 nm和10 nm的氧化铝保护膜层。在空气中存放不同时间后,碘化铯薄膜光阴极微通道板表面未发生明显潮解变化,其增益约为8800,暗计数率约为4.1 counts·s^(−1)·cm^(−2)。试验证明,氧化铝能够作为微通道板碘化铯膜层抗潮解超薄保护膜层。 相似文献
10.
金属有机化学气相沉积(MOCVD)法生长的掺硼氧化锌(BZO)薄膜,具有天然的"类金字塔"绒面结构,作为硅基薄膜太阳电池的前电极具有良好的陷光效果.但直接获得的BZO薄膜表面形貌过于尖锐,影响后续硅基薄膜材料生长质量及太阳电池的光电转换效率.本文设计了以一层超薄In2O3:Sn(ITO)薄膜(~4 nm厚度)作为中间层的多层膜,并通过对顶层BZO薄膜的厚度调制,改善BZO薄膜的表面特性,薄膜结构为:glass/底层BZO/ITO/顶层BZO.合适厚度的顶层BZO薄膜有助于获得类似"菜花状"形貌特征,尖锐的表面趋于"柔和",而较厚的顶层BZO薄膜仍然保持"类金字塔状"结构."柔和"的BZO薄膜表面结构有助于提高后续生长薄膜电池的结晶质量.将获得的新型"三明治"结构多层膜应用于p-i-n型氢化微晶硅(μc-Si:H)薄膜太阳电池,相比传统的BZO薄膜,电池的量子效率QE在500—800 nm波长范围提高了~10%,并且电池的Jsc和Voc均有所提高. 相似文献
11.
《Current Applied Physics》2015,15(3):194-200
BiFeO3 (BFO) thin films with thickness increasing from 40 to 480 nm were successfully grown on LaNiO3 (LNO) buffered Pt/Ti/SiO2/Si(100) substrate and the effects of thickness evolution on magnetic and ferroelectric properties are investigated. The LNO buffer layer promotes the growth and crystallization of BFO thin films. Highly (100) orientation is induced for all BFO films regardless of the film thickness together with the dense microstructure. All BFO films exhibited weak ferromagnetic response at room temperature and saturation magnetization is found to decrease with increase in film thickness. Well saturated ferroelectric hysteresis loops were obtained for thicker films; however, the leakage current dominated the ferroelectric properties in thinner films. The leakage current density decreased by three orders of magnitude for 335 nm film compared to 40 nm film, giving rise to enhanced ferroelectric properties for thicker films. The mechanisms for the evolution of ferromagnetic and ferroelectric characteristics are discussed. 相似文献
12.
Solid-state effects in the creation and decay of K 2p core excitations in thin KF films on Cu(1 0 0) surface have been studied in resonant Auger spectra, excited using synchrotron radiation. The spectra of films of various thickness starting from a single monolayer were measured.The photoabsorption spectra reveal crystal field splitting already at film thickness of about 1 monolayer. The Auger decay spectra of the K 2p−13d core excitations in films of thickness up to 2 monolayers exhibit a band characteristic of the decay of core ionised states, showing that the excited electron delocalises into substrate before the core hole decays. In thicker films the coexistence of the decay of excited states in the bulk of the KF crystalline film and of ionised states at the KF-metal interface is observed, indicating that the charge transfer probability from the upper layers of the film into the metallic substrate is strongly reduced. 相似文献
13.
Chien-Chon Chen Jin-Shyong Lin Eric Wei-Guang Diau Tzeng-Feng Liu 《Applied Physics A: Materials Science & Processing》2008,92(3):615-620
Self-cleaning of a surface of nanotube arrays of anodic titanium oxide (ATO) is demonstrated. The ATO was prepared in fluoride
ion containing sulfate electrolytes with a structure of 0.4 μm length, 100 nm pores diameter, 120 nm interpore distance, 25 nm
pore wall thickness, a 8×109 pores cm−2 pore density, and 68.2% porosity. Prepared as thin films either directly from a Ti foil or on a glass substrate, these arrays
have the property that water drops spread quickly over the surface of the films without irradiation. In contrast, a flat anatase
TiO2 film requires irradiation with UV light for several minutes before the contact angle decreases to zero. The observed self-cleaning
behavior of the ATO thin films is due to the capillary effect of the nanochannel structure and the superhydrophilic property
of the anatase TiO2 surface inside the tube. 相似文献
14.
本文报导了利用混合物理化学气相沉积法(Hybrid physical-chemical vapor deposition,HPCVD)在SiC(0001)衬底上制备干净的MgB2超薄膜.在背景气体压强、载气H2流量等条件一定的情况下,改变B2H6流量及沉积时间,制备不同厚度的MgB2超薄膜样品,并研究了超导转变温度Tc、剩余电阻率ρ(42K)、上临界场Hc2等与膜厚的关系.这系列超薄膜生长沿c轴外延,随膜厚度的变小Tc(0)降低,ρ(42K)升高.膜在衬底上的生长遵循Volmer-Weber岛状生长模式.对于10nm厚的膜,Tc(0)~32.4K,ρ(42K)~124.92μΩ·cm,其表面连接性良好,平均粗糙度为2.72nm,上临界磁场Hc2(0K)~12T,零场4K时的临界电流密度Jc~107A/cm2,为迄今为止所观测到的10nm厚MgB2超薄膜的最高Jc值,这也证明了10nm厚的MgB2膜在超导纳米器件上具有很强的应用潜力. 相似文献
15.
利用混合物理化学气相沉积法在6H-SiC(001)衬底上制备干净的MgB2超导超薄膜.在本底气体压强、载气氢气流量等条件一定的情况下,改变B2H6流量及沉积时间,制备得到不同厚度的系列MgB2超薄膜样品,并研究了超导转变温度Tc、剩余电阻率ρ(42K)、上临界磁场Hc2等与膜厚的关系.该系列超薄膜沿c轴外延生长,随膜厚度的变小,Tc(0)降低,ρ(42K)升高.膜在衬底上的生长遵循Volmer-Weber岛状生长模式.对于厚度为7.5 nm的MgB2超薄膜,Tc(0) =32.8 K,ρ(42K) =118 μΩcm,是迄今为止所观测到的厚度为7.5 nm的MgB2超薄膜最高的Tc值;对于厚度为10 nm的MgB2膜,Tc(0)=35.5 K,ρ(42K)=17.7 μΩcm,上临界磁场μ0Hc2估算为12 T左右,零磁场、4 K时的临界电流密度Jc=1.0×107 A/cm2,是迄今为止10 nm厚MgB2超薄膜的最高Jc值,且其表面连接性良好,均方根粗糙度为0.731 nm.这预示MgB2超薄膜在超导纳米器件上具有广阔的应用前景.
关键词:
2超薄膜')" href="#">MgB2超薄膜
薄膜生长
氢气流量
混合物理化学气相沉积 相似文献
16.
银薄膜对光学基底表面粗糙度及光散射的影响 总被引:1,自引:1,他引:0
为了研究金属银薄膜与光学基底表面粗糙度和光散射的关系,提出了通过对光学薄膜矢量散射公式积分来获得界面粗糙度完全相关模型和完全非相关模型下其表面的总反射散射的方法.理论计算了光学基底上两种模型在不同厚度银膜下的总反射散射和双向反射分布函数.结果表明,当沉积在光学基底上的银薄膜的厚度大于80 nm后,两种模型下计算的银薄膜的表面总反射散射都等于基底的总积分散射,银薄膜能较好地复现出基底的粗糙度轮廓.实验研究表明为了复现基底的粗糙度,银薄膜的最佳厚度应在80~160 nm之间. 相似文献
17.
用磁控溅射方法在单晶Si衬底上沉积膜厚为15—250nm的Ta膜.基于原子力显微镜获得的薄膜表面形貌,用动力学标度理论量化表征薄膜表面动态演化行为.结果表明:当膜厚d<50nm时,薄膜生长指数β≈0.17,而d>50nm后β≈0.45;随着d增加,粗糙度指数α由0.24逐渐增加到0.69,且在d>50nm后趋于稳定.Ta膜的表面动态演化行为揭示了其由小岛聚合结构向连续膜演化的生长过程.与自阴影等非局域效应引起的非稳定行为不同的是,当d<50nm时,薄膜表面动态演化的非稳定行为来源于生长初期的小岛聚合,表面小岛沿膜面切向的生长优于沿法向的生长.随着d继续增加,薄膜以连续膜形式生长,表面动态演化趋于稳定. 相似文献
18.
Dependence of photoconductivity on the crystallite orientations and porosity of polycrystalline ZnO films 总被引:1,自引:0,他引:1
Hexagonal ZnO films deposited on quartz glass, sapphire and glass substrates by sol–gel coating are found to be randomly oriented; maximum randomness is found in the film on quartz glass substrate. All the films are ultra-violet (UV) sensitive at around 360 nm sensitivity being maximum for the film with maximum randomness in the crystallite orientations. The film on quartz showed the lowest dark current and maximum photoresponse, which is related to the lowering of the barrier heights, introduced by the adsorbed oxygen at the grain boundaries. Faster decay in photocurrent is observed for the film deposited on glass, which is attributed due to the smaller crystallite sizes with porous microstructure of the film. PACS 73.61.Ga; 68.55.Jk; 73.50.Pz 相似文献
19.
极薄银在滤光片、高反射镜等中有广泛的应用,其光学常数严重影响着膜系的特性。在室温条件下,采用电阻热蒸发技术分别在硅和玻璃基底上沉积5.3 nm~26 nm不同厚度的极薄银薄膜,用TalySurfCCI非接触式轮廓仪测量了薄膜的厚度,研究了不同厚度银薄膜的光学常数n和k。镀制厚度5.3 nm、7.9 nm、14.1 nm、26.0 nm的银薄膜,结果显示极薄银的光学常数与块状银光学常数不同,当膜厚小于14.1 nm时,折射率n在380 nm~600 nm随波长增加而增加,在600 nm~1 600 nm随波长增加缓慢减小至趋于稳定值2.6;消光系数k在380 nm~500 nm随着波长增加而增加,在500 nm~1 600 nm随波长增加而缓慢减小至趋于0不变;当膜厚大于14.1 nm时,折射率随波长增加而增加,消光系数随波长近似呈线性增加。整体上,膜厚增加时折射率减小且趋于块状银的折射率,k随厚度增加而增加并最终趋于块状膜。用此拟合的光学常数代入TFc膜系设计软件计算其透射率,发现与分光光度计测得的透射率吻合较好。 相似文献
20.
超薄银薄膜具有高柔韧性和优良的光电性能,是用于透明导电电极的潜在材料。通过电阻热蒸发技术以金属铝作为浸润层制备超薄银透明导电薄膜。引入铝浸润层降低银薄膜的阈值厚度,使银薄膜在K9玻璃基底上以尽可能低的厚度达到连续。对不同厚度铝浸润层上银薄膜方块电阻进行测试,经SEM图像验证后得出,1 nm铝浸润层对银薄膜具有较好的浸润效果。随后采用相同的工艺在1 nm铝浸润层上制备了不同厚度的银薄膜,透过率和方阻测试结果表明,1 nm铝浸润层上制备的10 nm银薄膜方阻值可达到13Ω/,其在0.4μm~2.5μm波段内透过率可达到50%以上。 相似文献