溅射PZT薄膜的晶体结构和快速热处理

采用常温射频（ＲＦ）溅射法和快速热处理相结合的技术，在Ｐｔ／Ｔｉ／ＳｉＯ２／Ｓｉ衬底上，制备出具有铁电性的ＰＺＴ薄膜。研究了快速热处理工艺条件对ＰＺＴ薄膜性能的影响。通过Ｚ射线衍射法、ＳＥＭ和ＡＥＳ等方法，分析了ＰＺＴ薄膜的晶体结构、微结构、薄膜和电极间的界面效应。     

快速热处理对PZT薄膜的微结构及电性能的影响

采用改进的溶胶一凝胶技术,在Ｐｔ／Ｔｉ／ＴｉＯ２／ＳｉＯ２／Ｓｉ（１００）基片上制备了太电ＰＺＴ薄膜,用ＸＲＤ和ＡＦＭ技术分析了不同热处理工艺条件下ＰＺＴ薄膜的微观形貌变化及相结构演化,系统测试了ＰＺＴ薄膜的铁电性能。工艺－结构－性能研究结果表明：快速热处理工艺（ＲＴＡ）有利于ＰＺＴ薄膜保持较低的漏电流密度,热处理温度是影响晶粒大小的主要因素,而保温时间则对ＰＺＴ薄膜的致密性、晶粒均匀度和晶界结合     

Pt扩散阻挡层对PZT／Si薄膜化学结构和性能的影响

运用ＸＰＳ和ＡＥＳ研究了Ｐｔ扩散阻挡层对ＰＺＴ薄膜／Ｓｉ界面休学结构和性能的影响：在ＰＺＴ薄膜和Ｓｉ工间增加Ｐｔ扩散阻挡层，可以抑制ＴｉＣｘ物种和ＴｉＳｉｘ物种的形成，促进ＰＺＴ薄膜的形成反应。Ｐｔ扩散阻挡层的存在阻断了氧和Ｓｉ的相互扩散反应，促进ＰＺＴ物种形成钙钛矿型晶体结构，使得形成的ＰＴ薄膜具有和体相材料相摈 电常数和铁电性能。     

脉冲激光淀积法在Pt/TiO_2/SiO_2/Si(001)衬底上制备Pb(Ta_(0.05)Zr_(0.45)Ti_(0.50))O_3薄膜的铁电性质研究

用脉冲激光淀积方法在Ｐｔ／ＴｉＯ２／ ＳｉＯ２／ Ｓｉ（００１） 衬底上制备了掺Ｔａ 的ＰＺＴ 薄膜。此薄膜显示了理想的铁电性。漏电流特性表明这种异质结构中Ｓｃｈｏｔｔｋｙ 场发射机制起主要作用。扫描电镜形貌照片表明ＰＺＴ 薄膜结晶很好并且异质结构界面无明显扩散。     

脉冲激光淀积法在Pt／TiO2／SiO2／Si（001）衬底上制备Pb（Ta0.05Zr0.45T …

用脉冲激光淀积方法在Ｐｔ／ＴｉＯ２／ＳｉＯ２／Ｓｉ（００１）衬底上制备了掺Ｔａ的ＰＺＴ薄膜,此薄膜显示了理想的铁电性。漏电流特性表明这种异质结构中Ｓｃｈｏｔｔｋｙ场发射机制起主要作用。扫描电镜形貌照射表明ＰＺＴ薄膜结晶很好并且异质结构界面无明显扩散。     

锆钛酸铅(PZT)薄膜的自发极化与压电响应

用溶胶－凝胶法在Ｐｔ／Ｔｉ／ＳｉＯ２／Ｓｉ（１００）基片上制备了近等原子比的压电ＰＺＴ薄膜,在准同型相界附近的ＰＺＴ薄膜的应变机制是受极化控制的压电效应,内电场导致薄膜的自发极化定向,使薄膜未经极化就具有明显的压电响应。     

PZT／Si薄膜的扩散反应研究

运用ＸＰＳ和ＡＥＳ研究了ＰＺＴ膜／Ｓｉ在热处理过程中的薄膜及界面化学反应；在热处理过程中，气氛中的气通过ＰＺＴ的缺陷通道扩散到ＰＺＴ／Ｓｉ同旧，并与界面上的硅发生氧化反应形成ＳｉＯ２界面层。同时基底上的硅通过ＰＺＴ的缺陷扩散么样品表面形成ＳｉＯ２表面层。此外，在ＰＺＴ／Ｓｉ界面上，Ｔｉ的氧化物和Ｓｉ发生还原反应，形成了ＴｉＳｉｘ金属硅化物，并残留在ＰＺＴ膜层和和ＳｉＯ２界面层中。在ＰＺＴ膜层内，有     

PZT—NiTi铁电—铁弹多层膜的制备及表征

用溶胶－凝胶法制备了ＰＺＴ压电薄膜,研制了Ａｕ／ＰＺＴ／ＰＴ／ＴｉＯ２／ＮｉＴｉ／Ｓｉ（１００）多层膜结构,用ＸＲＤ,ＡＦＭ,ＴＥＭ－ＥＤＸ和ＳＡＤ技术考察了薄膜的表面形貌,相结构演化,以及面的元素分布特性。结果表明：ＰＺＴ膜与ＮｉＴｉ合金膜的结合良好,稳定;ＰＴ层的引入,使无定型ＰＺＴ薄膜在５５０℃退火后,转变为钙钛矿结构,降低了晶化温度,并有效地抑制焦碌石相的形成;ＮｉＴｉ薄膜结晶良好;ＴｉＯ     

改进溶胶-凝胶法制备PZT50/50铁电薄膜

采用改进的溶胶凝胶法在Ｐｔ／Ｔｉ／ＳｉＯ２／Ｓｉ衬底上制备了ＰＺＴ５０／５０铁电薄膜，用Ｘ射线衍射表征了薄膜的物相，用原子力显微镜（ＡＦＭ）表征薄膜的微观形貌，用ＲＴ６６Ａ测量了薄膜的铁电特性，获得了具有优良的铁电性能的晶粒尺寸为１００ｎｍ的ＰＺＴ５０／５０铁电薄膜，在２０Ｖ电压下，Ｐｒ＝３１．８３μＣ／ｃｍ２。     

溅射工艺参数对PZT铁电薄膜相变过程的影响

采用射频磁控溅射工艺,在（１１１）Ｐｔ／Ｔｉ／ＳｉＯ２／Ｓｉ衬底上用ＰＺＴ（５３／４７）陶瓷靶制备铁电薄膜。用快速光热退火炉对原位沉积的薄膜进行ＲＴＡ处理。     

基于溶胶-凝胶的两种旋涂方法制备PZT厚膜(英文)

采用溶胶-凝胶法,研究了两种在Au/Cr/SiO2/Si基底上沉积PZT(Pb(Zr0.52Ti0.48)O3)厚膜的方法.把与PZT澄清溶胶成分相同的PZT纳米粉混入澄清PZT溶胶,然后超声混合形成PZT浆料,PZT纳米粉的粒径为50～100nm.XRD分析表明两种方法得到的PZT厚膜都获得了单相钙钛矿结构.SEM结果显示两种厚膜厚度大约4μm,第一种旋涂方法制得的PZT厚膜表面粗糙,第二种旋涂方法制得的厚膜表面致密,无裂纹.在1 kHz的测试频率下,第一种和第二种厚膜的矫顽场分别为30 kV/cm和50 kV/cm,饱和极化分别为45 μC/cm2和54 μC/cm2,剩余极化分别为25μC/cm2 and 30μC/cm2.第二种厚膜有较高的直流耐压性能,在300 kV/cm的电场下,仍然保持较好的铁电性能.因而,第二种旋涂方法能够改善PZT厚膜的表面形貌和铁电性能.     

Lead zirconate titanate thin films on GaAs substrates

Thin films of the piezoceramic lead zirconate titanate (PZT) of composition Pb(Zr0.53Ti0.47)O3 have been prepared on a platinized GaAs substrate system using a propanediol based sol-gel technique. A Si3N4 buffer layer was deposited onto the GaAs by plasma-enhanced chemical vapour deposition so as to minimize Ga and As diffusion during film fabrication. Rapid thermal processing (RTP) techniques were used to thermally decompose the sol-gel layer to PZT in a further effort to avoid problems of Ga and As diffusion. Adhesion between the electrode and substrate was found to improve when an intermediate Ti layer deposited between the Pt and Si3N4 was oxidized prior to depositing the Pt layer. A crystalline PZT film was produced on the Pt/TiO2/Si3N4/GaAs by firing the sol-gel coating at 350°C for 1 min and then at 650°C for 10 s using RTP. A single deposition of precursor sol resulted in a film 0.5 μm thick. Measured average values of remanant polarization and coercive field were 14 μC cm-2 and 47 kV cm-1, respectively. The polarization value is rather low, as conventionally fired films on silicon have remanent polarization values of 20–30 μC cm-2; the lower values may be due to incomplete crystallization during RTP, but a degradation of properties due to Ga-As diffusion, despite the precautions, cannot be ruled out at this stage. This revised version was published online in November 2006 with corrections to the Cover Date.     

Ferroelectric and piezoelectric behavior of (111)-oriented Pb(ZrxTi1−x)O3 thin films on cobalt ferrite nano-seed layered Pt(111)/Si substrate

Perfect (111)-oriented Pb(Zr_xTi_1?x)O₃ (PZT) thin films were grown on cobalt ferrite buffered Pt(111)/Ti/SiO₂/Si substrate by pulsed laser deposition method using various targets with different Zr/Ti ratios ranging from 30/70 to 70/30. The results of X-ray diffraction analyses indicated that the composition of morphotropic phase boundary in the present PZT films is same as the bulk PZT (Zr/Ti = 52/48). The effect of Zr/Ti ratio of the PZT films was investigated by the ferroelectric domain structure and the piezoelectric characteristics of the films by piezoresponse force microscopy, as well as polarization measurement. The results revealed that the present tetragonal PZT film has a higher ferroelectric domain switching than rhombohedral one and the film with composition of Zr/Ti = 52/48 showed relatively high value of squareness of P–E loop and E_c as well as high piezoresponse.     

PZT基体沉积条形分布NiTiSMA薄膜复合材料的介电性能

使用模具并采用磁控溅射法在铁电陶瓷PZT基体上沉积具有条形分布结构的Ni Ti SMA薄膜。显微组织结构观察发现,以条形分布结构方式沉积的Ni Ti SMA薄膜晶化处理后具有等轴晶结构。比较所制备PZT/Ni-Ti SMA薄膜复合材料与纯PZT的介电常数及介电损耗发现,两者的介电损耗水平接近;复合材料的介电常数比纯PZT的提高约18%。Ni Ti SMA的沉积使基体中靠近薄膜区域的Zr/Ti物质的量比恰好落在准同型相界区内,致使所制备复合材料的介电性能优于纯PZT。     

玻璃基Pt/Pb(Zr_(0.4)Ti_(0.6))O_3/ITO电容器的结构及物理性能研究

采用溶胶-凝胶方法在玻璃基ITO电极上制备了Pt/Pb(Zr0.4Ti0.6)O3(PZT)/ITO电容器.采用X射线衍射仪、铁电测试仪、分光光度计对其微观结构、电学性能及光学性能进行了测量.结果表明PZT薄膜结晶良好,具有(101)高度择优取向.铁电电容器具有良好的保持特性和抗疲劳特性,具有较大的剩余极化强度和电阻率,5V电压下的剩余极化强度和电阻率分别为41.7μC/cm2和2.5×109Ω.cm;漏电流测量结果表明电压小于0.8V时为欧姆导电机制,当电压大于0.8V时,漏电流满足肖特基发射机制.光学透射谱结果表明在短波范围内,PZT表现出强吸收作用;在长波范围内,PZT表现为强透射,最大透射率达到95%.     

Electrohydrodynamic deposition of nanostructured lead zirconate titanate

The deposition of a propanol-based lead zirconate titanate (PZT) sol using electrohydrodynamic atomization (EHDA) in the stable cone-jet mode was investigated. The droplets generated were deposited onto a copper substrate as a film, which was investigated using X-ray diffraction and scanning electron microscopy. The PZT film was shown to contain uniform nano-particles of PZT, which maintained their shape on sintering (650 degrees C, 1 hour) while forming the perovskite phase of PZT.     

以溶胶-凝胶法PZT薄膜为驱动的微泵研制

采用溶胶-凝胶法(sol-gel)制备技术制作了Pb(Zr,Ti)O3(PZT)压电薄膜,并以PZT薄膜为驱动制作了微泵.采用了V型微阀的微泵主要利用PZT的压电效应.针对微泵的关键结构--复合驱动膜,探索了一种Si/SiO2/Ti/Au/PZT/Cr/Au多层驱动膜结构制备方法,解决了在硅基底上制备PZT薄膜的问题,同时探讨并解决了硅各向异性刻蚀微泵的微驱动腔、单向阀的工艺问题,并通过SEM照片对V型阀和多层驱动膜进行了表征.研究结果表明,采用MEMS技术成功地完成了微驱动器的研制,得到的驱动腔硅杯平坦均匀.在V型阀微泵整体设计中需要的硅片数目少,降低了器件的复杂性,可以满足功耗低、小型化和批量生产的要求.     

Interfacial mechanisms controlling phase formation in sol-gel derived lead zirconate titanate thin films

An RBS study has been carried out to study the relative extent of Pb diffusion in the substrate from PZT films. It is found that extensive diffusion of Pb occurs into the quartz substrate making the film severely deficient in Pb. No such diffusion occurs in the case of PZT films on sapphire and the concentration of Pb is near stoichiometric, except for a small loss due to volatilization. Excessive Pb deficiency, rather than any epitaxial effect, has earlier been proposed by us to be the crucial factor responsible for the existence of the pyrochlore phase in PZT thin films on substrates such as Si, glass, quartz etc. The present results confirm this. The effects of other process variables such as thickness and chemical composition (Zr/Ti ratio) of the film can also be understood in terms of the same phenomenon.     

Pb(Zr,Ti)O3薄膜微区残余应力的X射线面探扫描分析

根据在X射线二维衍射几何关系下建立的应力应变方程,提出了一种基于X射线多晶面探衍射仪系统分析射频磁控溅射制备的Pb(Zr,Ti)O3薄膜微区残余应力的测量方法,即通过基于X射线衍射圆锥形变的分析来表征薄膜的残余应力,试验结果表明薄膜所受为残余拉应力,同时利用X射线面探扫描方法评价了薄膜的残余应力分布.     

Theoretical investigation of the SAW properties of ferroelectric film composite structures

The characteristics of surface acoustic waves (SAW) propagating on a three-layered structure consisting of a perovskite-type ferroelectric film, a buffer layer and a semiconductor substrate have been studied theoretically. Large coupling coefficients (K(2)) can be obtained when the interdigital transducer (IDT) is on top of the perovskite-type ferroelectric film, with (type 4) and without (type 3) the floating-plane electrode at the perovskite-type ferroelectric film-buffer layer interface. In the above cases, the peak values of K (2) Of the Pb(Zr,Ti)O(3) (PZT) films (3.2%-3.8%) are higher than those of the BaTiO(3) (BT) and PbTiO(3) (PT) films. In the IDT configuration of type 4, there exists a minor peak of the coupling coefficients for the PZT and BT films, but not for the PT films when the normalized thickness (hK) of the perovskite-type ferroelectric film is about 0.3. The minor peak values of the coupling coefficients (0.62%-0.93%) for different layered structures (PZT/STO/Si, PZT/MgO/Si, and PZT/MgO/GaAs) all decrease when we increase hK value from 0 to 0.25. The results could be useful in the integration of ferroelectric devices, semiconductor devices, and SAW devices on the same substrate.