CN1983464B - Ferroelectric film, ferroelectric capacitor, ferroelectric memory, piezoelectric element, semiconductor element - Google Patents
Ferroelectric film, ferroelectric capacitor, ferroelectric memory, piezoelectric element, semiconductor element Download PDFInfo
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Abstract
一种强电介质膜,由AB1-XNbXO3的通式表示,其中,作为A元素至少含有Pb,作为B元素由Zr、Ti、V、W、Hf、和Ta中的至少一种以上构成,0.1≤x≤0.4。
A ferroelectric film, represented by the general formula of AB 1-X Nb X O 3 , wherein at least Pb is contained as the A element, and at least one of Zr, Ti, V, W, Hf, and Ta is used as the B element The above constitution, 0.1≤x≤0.4.
Description
本分案申请的母案为: The parent case of this divisional application is:
发明名称:强电介质膜、电容器及它们的制造方法、强电介质存储器 Title of Invention: Ferroelectric film, capacitor and their manufacturing method, ferroelectric memory
国际申请日:2003年10月23日 International filing date: October 23, 2003
国际申请号:PCT/JP03/13556 International application number: PCT/JP03/13556
国家申请号:200380101906.2 National application number: 200380101906.2
技术领域technical field
本发明涉及一种强电介质膜、强电介质电容器、强电介质存储器、压电元件、半导体元件、强电介质膜的制造方法、和强电介质电容器的制造方法。 The invention relates to a ferroelectric film, a ferroelectric capacitor, a ferroelectric memory, a piezoelectric element, a semiconductor element, a method for manufacturing a ferroelectric film, and a method for manufacturing a ferroelectric capacitor. the
背景技术Background technique
近年来,PZT、SBT等强电介质膜或使用其的强电介质电容器、强电介质存储器装置等的研究开发盛行。强电介质存储器装置的构成可大致分成1T型、1T1C型、2T2C型、单纯矩阵型。其中,由于1T型在结构上在电容器中产生内部电场,所以保持力(数据保持)短至1个月,不能满足半导体一般要求的10年保证。1T1C型、2T2C型与DRAM的构成大致相同,为了具有选择用晶体管,可适用DRAM的制造技术。另外,1T1C型、2T2C型由于实现了SRAM的写入速度,所以到目前为止256KB以下的小容量品被商品化。 In recent years, research and development of ferroelectric films such as PZT and SBT, ferroelectric capacitors, ferroelectric memory devices, and the like using them have been actively conducted. The configuration of ferroelectric memory devices can be roughly classified into 1T type, 1T1C type, 2T2C type, and simple matrix type. Among them, since the 1T type generates an internal electric field in the capacitor structurally, the retention (data retention) is as short as 1 month, and cannot meet the 10-year guarantee generally required by semiconductors. The 1T1C type and 2T2C type have almost the same configuration as DRAM, and the manufacturing technology of DRAM can be applied in order to have selection transistors. In addition, since the 1T1C type and 2T2C type have realized the writing speed of SRAM, so far, small-capacity products of 256 KB or less have been commercialized. the
迄今为止,作为强电介质材料,主要使用Pb(Zr、Ti)O3(PZT)。在PZT的情况下,使用Zr/Ti比为52/48或40/60的、菱面体晶和正方晶体的混合存在区域及其附近的组成。另外,在PZT的情况下,还掺杂使用La、Sr、Ca等元素。使用该区域是为了确保存储器元素最需要的可靠性。磁滞形状虽然丰富含有Ti的正方晶体区域很好,但产生离子性晶体结构引起的肖脱基缺陷。因此,会产生泄漏电流特性或印象(imprint)特性(所谓的磁滞的变形程度)不好,难以确保可靠性。 So far, Pb(Zr,Ti)O 3 (PZT) has been mainly used as a ferroelectric material. In the case of PZT, a Zr/Ti ratio of 52/48 or 40/60, a rhombohedral crystal and a tetragonal crystal mixed region and its vicinity are used. In addition, in the case of PZT, elements such as La, Sr, and Ca are also used for doping. This area is used to ensure the most required reliability of memory elements. The hysteresis shape is good for a tetragonal crystal region rich in Ti, but produces Schottky defects due to the ionic crystal structure. Therefore, the leakage current characteristic and the imprint characteristic (the degree of deformation of the so-called hysteresis) are not good, and it is difficult to ensure reliability.
另一方面,单纯矩阵型的单元尺寸比1T1C型、2T2C型小,另外,可多层化电容器,所以期待高集成化、低成本化。 On the other hand, the cell size of the simple matrix type is smaller than that of the 1T1C type and the 2T2C type, and capacitors can be multilayered, so high integration and cost reduction are expected. the
另外,就以往的单纯矩阵型强电介质存储器装置而言,如日本特开平9-116107号公报等中公开的那样。在该公开公报中,公开了当向存储器单元写入数据时,向非选择存储器单元施加写入电压的1/3电压的驱动方法。 In addition, conventional simple matrix ferroelectric memory devices are disclosed in Japanese Patent Application Laid-Open No. 9-116107 and the like. This publication discloses a driving method of applying a voltage of 1/3 of the write voltage to non-selected memory cells when writing data to the memory cells. the
但是,该技术中,未具体记载动作必需的强电介质电容器的磁滞环。为了得到可实际动作的单纯矩阵型强电介质存储器装置,方型性的良好的磁滞环是不可或缺的。作为可与之对应的强电介质材料,考虑富Ti的正方晶体PZT作为候补,但与已述的1T1C和2T2C型强电介质存储器一样,可靠性的确保成为最重要的课题。 However, this technique does not specifically describe the hysteresis loop of the ferroelectric capacitor necessary for operation. In order to obtain a practically operable simple matrix ferroelectric memory device, a hysteresis loop with good squareness is indispensable. As a compatible ferroelectric material, Ti-rich tetragonal PZT is considered as a candidate, but as with the 1T1C and 2T2C type ferroelectric memories described above, securing reliability is the most important issue. the
另外,虽然PZT正方晶体示出适于存储器用途的具有方型性的磁滞特性,但缺乏可靠性而未被实用化。其理由如下。 In addition, although the PZT tetragonal crystal has square-shaped hysteresis characteristics suitable for memory applications, it lacks reliability and has not been put into practical use. The reason for this is as follows. the
首先,结晶后的PZT正方晶体薄膜具有如下倾向,即若Ti含有率越高,则泄漏电流强度越高。另外,当进行向+或-方向的任一方仅写入一次数据、在加热保持在100度后读出数据的、所谓静态印象试验时,在24小时(h)之后,基本上未剩余写入的数据。这些是作为离子性结晶的PZT和作为PZT构成元素的Pb与Ti自身具有的本质特征,成为构成元素的大部分为Pb和Ti构成的PZT正方晶体薄膜具有的最大问题。该问题在PZT钙钛矿是离子性结晶时大,是PZT具有的本质问题。 First, the crystallized PZT tetragonal thin film tends to increase the leakage current intensity as the Ti content increases. In addition, when a so-called static impression test was performed in which data was written only once in either the + or - direction, and the data was read after being heated and kept at 100 degrees, after 24 hours (h), substantially no writing remained. The data. These are essential characteristics of PZT which is an ionic crystal and Pb and Ti which are constituent elements of PZT, and are the biggest problems of a PZT tetragonal thin film whose constituent elements are mostly composed of Pb and Ti. This problem is large when the PZT perovskite is an ionic crystal, and is an essential problem of PZT. the
图44是关联于PZT各构成元素的结合的主要能量的一览。已知PZT在结晶后多含有氧空穴。即,根据图44,预测Pb-O在PZT构成元素中的结合能量最小,烧成加热时或极化反转时被简单切断。即,若逸出(逸出)Pb,则根据电荷中性原则,会逸出O。 Fig. 44 is a list of main energies related to the bonding of each constituent element of PZT. It is known that PZT contains many oxygen vacancies after crystallization. That is, from FIG. 44 , it is predicted that Pb—O has the smallest binding energy among PZT constituent elements, and is easily cut off during firing heating or polarization inversion. That is, when Pb escapes (escapes), O escapes according to the principle of charge neutrality. the
接着,在印象(imprint)试验等的加热保持时,PZT的各构成元素振动并反复冲击,但PZT构成元素中Ti最轻,容易由于高温保持时的振动冲击而逸出。因此,若逸出Ti,则根据电荷中性原则,会逸出O。另外,因为Pb:+2、Ti:4的最大价数有助于结合,所以在逸出O之外,电荷中性不成立。即,PZT容易形成对于Pb和Ti等1个阳离子容易逸出两个O等阴离子的所谓肖脱基缺陷。 Next, during heating and holding such as an imprint test, each constituent element of PZT vibrates and repeatedly impacts, but Ti is the lightest among PZT constituent elements, and easily escapes due to vibration shock during high temperature holding. Therefore, if Ti escapes, O will escape according to the principle of charge neutrality. In addition, since the maximum valence number of Pb:+2 and Ti:4 contributes to the combination, charge neutrality does not hold except for escaped O. That is, PZT tends to form so-called Schottky defects in which two anions such as O are easily released from one cation such as Pb and Ti. the
这里,说明PZT结晶中的氧缺损引起的泄漏电流产生的原理。图45A~图45C是说明具有用通式ABO2.5表示的褐针镍矿(Brownmillerite)型晶体结构的氧化物结晶中的泄漏电流产生的图。如图45A所示,褐针镍矿型晶体结构是相对于具有用通式ABO3表示的PZT结晶等的钙钛矿型晶体结构具有氧缺损的晶体结 构。另外,如图45B所示,由于在褐针镍矿型晶体结构中阳离子附近是氧离子,所以阳离子缺损很难成为泄漏电流增大的原因。但是,如图45C所示,氧离子在PZT结晶整体中串联连接,当由于氧缺损而晶体结构变为褐针镍矿型晶体结构时,泄漏电流也会因此增大。 Here, the principle of leakage current generation due to oxygen deficiency in the PZT crystal will be described. 45A to 45C are diagrams illustrating the generation of leakage current in an oxide crystal having a Brownmillerite-type crystal structure represented by the general formula ABO 2.5 . As shown in FIG. 45A , the lignite-type crystal structure is a crystal structure having oxygen deficiency relative to a perovskite-type crystal structure having a PZT crystal represented by the general formula ABO 3 or the like. In addition, as shown in FIG. 45B , since oxygen ions are in the vicinity of cations in the lignite-type crystal structure, cation deficiency is unlikely to cause an increase in leakage current. However, as shown in FIG. 45C , oxygen ions are connected in series throughout the entire PZT crystal, and when the crystal structure changes to a chrysanthemum crystal structure due to oxygen deficiency, the leakage current also increases.
另外,除上述泄漏电流的产生外,Pb和Ti的缺损或伴随其的O缺损也是所谓的晶格缺陷,构成图46所示的空间电荷极化的原因。此时,在PZT结晶中,由于强电介质的极化形成的电场,会产生晶格缺陷引起的反电场,变为所谓施加偏移电位的状态,结果,磁滞移位或减少极性。并且,温度越高,该现象越央产生。 In addition to the generation of the leakage current described above, defects of Pb and Ti and accompanying O defects are also so-called lattice defects, which cause the space charge polarization shown in FIG. 46 . At this time, in the PZT crystal, the electric field formed by the polarization of the ferroelectric generates a counter electric field caused by lattice defects, and a so-called offset potential is applied. As a result, the hysteresis is shifted or polarized. And, the higher the temperature, the more this phenomenon occurs. the
以上是PZT具有的本质的问题,在纯粹的PZT中,认为难以解决上述问题,到目前为止,在使用正方晶体的PZT的存储器元件中,未实现具有充分特性的元件。 The above are the essential problems of PZT, and it is considered difficult to solve the above-mentioned problems in pure PZT, and up to now, memory elements using tetragonal PZT have not realized elements with sufficient characteristics. the
另外,就强电介质存储器而言,含有于强电介质电容器中的强电介质膜的结晶状态是决定器件特性的重要因素之一。另外,在强电介质存储器的制造工序中,具有形成夹层绝缘膜或保护膜的工序,使用产生大量氢的工艺。此时,由于强电介质膜主要由氧化物形成,所以由制造工序中产生的氢而还原氧化物,会对强电介质电容器的特性造成不期望的影响。 In addition, in the ferroelectric memory, the crystallization state of the ferroelectric film included in the ferroelectric capacitor is one of the important factors for determining device characteristics. In addition, in the manufacturing process of the ferroelectric memory, there is a process of forming an interlayer insulating film or a protective film, and a process that generates a large amount of hydrogen is used. At this time, since the ferroelectric film is mainly formed of oxides, reduction of the oxides by hydrogen generated in the manufacturing process undesirably affects the characteristics of the ferroelectric capacitor. the
因此,在以往的强电介质存储器中,为了防止强电介质电容器的特性恶化,通过用氧化铝膜或氮化铝膜等阻挡膜覆盖强电介质电容器,担保电容的耐还原性。但是,这些阻挡膜在强电介质存储器的高集成化时需要多余的占有区域,另外,从生产性方面看,期望利用更简单的工艺来制造强电介质存储器的方法。 Therefore, in the conventional ferroelectric memory, in order to prevent the characteristics of the ferroelectric capacitor from deteriorating, the ferroelectric capacitor is covered with a barrier film such as an aluminum oxide film or an aluminum nitride film to ensure the reduction resistance of the capacitor. However, these barrier films require an extra occupied area for high integration of the ferroelectric memory, and from the viewpoint of productivity, a method of manufacturing the ferroelectric memory with a simpler process is desired. the
发明内容Contents of the invention
本发明的目的在于提供一种含有可对1T1C、2T2C和单纯矩阵型强电介质任一使用的具有磁滞特性的强电介质电容器的1T1C、2T2C和单纯矩阵型强电介质存储器。另外,本发明的另一目的在于提供一种适于上述强电介质存储器的强电介质膜及其制造方法。并且,本发明的又一目的在于提供一种使用上述强电介质膜的压电元件和半导体元件。另外,本发明的又一目的在于提供一种可利用不需要阻挡膜的简便工艺来担保充分特性的强电介质电容器、其制造方法和使用强电介质电容器的强电介质存储器。 An object of the present invention is to provide 1T1C, 2T2C and simple matrix ferroelectric memories including ferroelectric capacitors having hysteresis characteristics which can be used for any of 1T1C, 2T2C and simple matrix ferroelectrics. In addition, another object of the present invention is to provide a ferroelectric film suitable for the above-mentioned ferroelectric memory and a method of manufacturing the same. Furthermore, another object of the present invention is to provide a piezoelectric element and a semiconductor element using the above-mentioned ferroelectric film. Another object of the present invention is to provide a ferroelectric capacitor capable of securing sufficient characteristics by a simple process that does not require a barrier film, a method of manufacturing the same, and a ferroelectric memory using the ferroelectric capacitor. the
一种强电介质膜,由AB1-xNbxO3的通式表示,作为A元素至少含有 Pb,作为B元素由Zr、Ti、V、W、Hf、和Ta中的至少一种以上构成,其中0.1≤x≤0.4 A ferroelectric film represented by the general formula of AB 1-x Nb x O 3 , containing at least Pb as an A element, and composed of at least one of Zr, Ti, V, W, Hf, and Ta as a B element , where 0.1≤x≤0.4
附图说明Description of drawings
图1是模式地表示强电介质电容器的截面图。 FIG. 1 is a cross-sectional view schematically showing a ferroelectric capacitor. the
图2是表示用旋涂法形成PZTN膜用的流程图。 Fig. 2 is a flowchart showing the formation of a PZTN film by the spin coating method. the
图3是表示强电介质电容器的P(极化)-V(电压)磁滞曲线的图。 FIG. 3 is a graph showing a P (polarization)-V (voltage) hysteresis curve of a ferroelectric capacitor. the
图4A~图4C是表示实施例1的PZNT膜的表面组织的图。 4A to 4C are diagrams showing the surface structure of the PZNT film of Example 1. FIG. the
图5A~图5C是表示实施例1的PZNT膜的结晶性的图。 5A to 5C are graphs showing the crystallinity of the PZNT film of Example 1. FIG. the
图6A~图6C是表示实施例1的PZNT膜的膜厚与表面组织的关系的图。 6A to 6C are graphs showing the relationship between the film thickness of the PZNT film of Example 1 and the surface structure. the
图7A~图7C是表示实施例1的PZNT膜的膜厚与结晶性的关系的图。 7A to 7C are graphs showing the relationship between the film thickness and crystallinity of the PZNT film of Example 1. FIG. the
图8A~图8C是表示实施例1的PZNT膜的膜厚与磁滞特性的图。 8A to 8C are graphs showing the film thickness and hysteresis characteristics of the PZNT film of Example 1. FIG. the
图9A~图9C是表示实施例1的PZNT膜的膜厚与磁滞特性的图。 9A to 9C are graphs showing the film thickness and hysteresis characteristics of the PZNT film of Example 1. FIG. the
图10A和图10B是表示实施例1的PZNT膜的泄漏电流特性的图。 10A and 10B are graphs showing leakage current characteristics of the PZNT film of Example 1. FIG. the
图11A是表示实施例1的PZTN膜的疲劳特性的图。图11B是表示实施例1的PZTN膜的静态印象特性的图。 FIG. 11A is a graph showing the fatigue characteristics of the PZTN film of Example 1. FIG. 11B is a graph showing the static image characteristics of the PZTN film of Example 1. FIG. the
图12是表示实施例1的利用臭氧TEOS来形成SiO2保护膜的强电介质电容器的结构图。 12 is a diagram showing the structure of a ferroelectric capacitor in Example 1 in which a SiO 2 protective film is formed using ozone TEOS.
图13是表示实施例1的利用臭氧TEOS来形成SiO2保护膜之后的强电介质电容器的磁滞特性的图。 13 is a graph showing hysteresis characteristics of a ferroelectric capacitor after forming a SiO 2 protective film using ozone TEOS in Example 1. FIG.
图14是表示实施例1的现有PZT膜的泄漏电流特性的图。 FIG. 14 is a graph showing leakage current characteristics of a conventional PZT film of Example 1. FIG. the
图15是表示实施例1的使用现有PZT膜的强电介质电容器的疲劳特性的图。 FIG. 15 is a graph showing fatigue characteristics of a ferroelectric capacitor using a conventional PZT film according to Example 1. FIG. the
图16是表示实施例1的使用现有PZT膜的强电介质电容器的静态印象特性的图。 FIG. 16 is a graph showing static image characteristics of a ferroelectric capacitor using a conventional PZT film according to Example 1. FIG. the
图17A和图17B是表示实施例2的PZTN膜的磁滞特性的图。 17A and 17B are graphs showing hysteresis characteristics of the PZTN film of Example 2. FIG. the
图18A和图18B是表示实施例2的PZTN膜的磁滞特性的图。 18A and 18B are graphs showing hysteresis characteristics of the PZTN film of Example 2. FIG. the
图19A和图19B是表示实施例2的PZTN膜的磁滞特性的图。 19A and 19B are graphs showing hysteresis characteristics of the PZTN film of Example 2. FIG. the
图20是表示实施例2的PZTN膜的X射线衍射图案的图。 FIG. 20 is a diagram showing an X-ray diffraction pattern of a PZTN film of Example 2. FIG. the
图21是表示实施例2的PZTN结晶中的Pb缺损量与Nb的组成比的关系图。 21 is a graph showing the relationship between the amount of Pb defects and the composition ratio of Nb in the PZTN crystal of Example 2. FIG. the
图22是说明作为钙钛矿结晶的WO3的晶体结构的图。 Fig. 22 is a diagram illustrating the crystal structure of WO 3 which is a perovskite crystal.
图23A~图23C是模式地表示实施例3中的PZTN膜的形成工序的截面图。 23A to 23C are cross-sectional views schematically showing the steps of forming the PZTN film in Example 3. FIG. the
图24A和图24B是说明实施例3中的PZTN膜的晶格常数的变化的图。 24A and 24B are graphs illustrating changes in the lattice constant of the PZTN film in Example 3. FIG. the
图25是说明实施例3中的PZTN膜与Pt金属膜的晶格不匹配率的变化的图。 FIG. 25 is a graph illustrating changes in lattice mismatch ratios between the PZTN film and the Pt metal film in Example 3. FIG. the
图26是表示利用旋涂法形成参考例中的现有PZT膜用的流程图。 Fig. 26 is a flow chart for forming a conventional PZT film in a reference example by spin coating. the
图27A~图27E是表示参考例中的PZT膜的表面组织的图。 27A to 27E are diagrams showing the surface structure of the PZT film in the reference example. the
图28A~图28E是表示参考例中的PZT膜的结晶性的图。 28A to 28E are diagrams showing the crystallinity of the PZT film in the reference example. the
图29A和图29B是表示参考例中的正方晶体PZT膜的磁滞的图。 29A and 29B are diagrams showing hysteresis of a tetragonal PZT film in a reference example. the
图30是表示参考例中的现有正方晶体PZT膜的磁滞的图。 FIG. 30 is a graph showing hysteresis of a conventional tetragonal PZT film in a reference example. the
图31A和图31B是表示参考例中的正方晶体PZT膜的脱气分析结果的图。 31A and 31B are graphs showing the results of outgassing analysis of the tetragonal PZT film in Reference Example. the
图32A~图32C是表示强电介质电容器的制造工序的图。 32A to 32C are views showing the manufacturing process of the ferroelectric capacitor. the
图33A和图33B是表示强电介质电容器的磁滞特性的图。 33A and 33B are graphs showing hysteresis characteristics of ferroelectric capacitors. the
图34是表示强电介质电容器的电特性的图。 Fig. 34 is a graph showing electrical characteristics of a ferroelectric capacitor. the
图35A是模式地表示单纯矩阵型的强电介质存储器装置的平面图。图35B是模式地表示单纯矩阵型的强电介质存储器装置的截面图。 Fig. 35A is a plan view schematically showing a simple matrix type ferroelectric memory device. Fig. 35B is a cross-sectional view schematically showing a simple matrix type ferroelectric memory device. the
图36是表示将存储器单元阵列与外围电路共同集成在同一基板上的强电介质存储器装置的一例的截面图。 36 is a cross-sectional view showing an example of a ferroelectric memory device in which a memory cell array and peripheral circuits are commonly integrated on the same substrate. the
图37A是模式地表示1T1C型强电介质存储器的截面图。图37B是模式地表示1T1C型强电介质存储器的等效电路图。 Fig. 37A is a cross-sectional view schematically showing a 1T1C type ferroelectric memory. Fig. 37B is an equivalent circuit diagram schematically showing a 1T1C type ferroelectric memory. the
图38A~图38C是表示强电介质存储器的制造工序的图。 38A to 38C are views showing the manufacturing steps of the ferroelectric memory. the
图39是记录头的分解立体图。 Fig. 39 is an exploded perspective view of a recording head. the
图40A是记录头的平面图。图40B是记录头的截面图。 Fig. 40A is a plan view of a recording head. Fig. 40B is a sectional view of the recording head. the
图41是模式地表示压电元件的层结构的截面图。 Fig. 41 is a cross-sectional view schematically showing a layered structure of a piezoelectric element. the
图42是表示喷墨式记录装置一例的示意图。 Fig. 42 is a schematic diagram showing an example of an ink jet recording device. the
图43A是表示在PZT中添加Ta的强电介质膜的磁滞特性的图。图43B是表示在PZT中添加W的强电介质膜的磁滞特性的图。 FIG. 43A is a graph showing hysteresis characteristics of a ferroelectric film in which Ta is added to PZT. FIG. 43B is a graph showing hysteresis characteristics of a ferroelectric film in which W is added to PZT. the
图44是表示关联于PZT类强电介质的构成元素的结合的各特性图。 Fig. 44 is a graph showing various characteristics related to combinations of constituent elements of a PZT-based ferroelectric. the
图45A~图45C是说明褐针镍矿型晶体结构的肖脱基缺陷的图。 FIGS. 45A to 45C are diagrams illustrating Schottky defects in the browniite-type crystal structure. the
图46是说明强电介质的空间电荷极化的图。 Fig. 46 is a diagram illustrating space charge polarization of a ferroelectric. the
具体实施方式Detailed ways
(1)本实施方式的强电介质膜由AB1-XNbXO3的通式表示,A元素至少由Pb构成,B元素由Zr、Ti、V、W、Hf、和Ta中的至少一种以上构成,在0.05≤x<1的范围内含有Nb。 (1) The ferroelectric film of this embodiment is represented by the general formula of AB 1-X Nb X O 3 , the A element is composed of at least Pb, and the B element is at least one of Zr, Ti, V, W, Hf, and Ta. One or more kinds of constitutions, containing Nb within the range of 0.05≤x<1.
另外,A元素可由Pb1-yLny(0<y≤0.2)构成。另外,Ln可由La、Ce、Pr、Nd、Pm、Sm、Eu、Gd、Tb、Dy、Ho、Er、Tm、Yb和Lu中的至少一种以上构成。 In addition, the A element may be composed of Pb 1-y Ln y (0<y≦0.2). In addition, Ln may be composed of at least one of La, Ce, Pr, Nd, Pm, Sm, Eu, Gd, Tb, Dy, Ho, Er, Tm, Yb, and Lu.
(2)本实施方式的强电介质膜由(Pb1-yAy)(B1-xNbx)O3的通式表示,A元素由La、Ce、Pr、Nd、Pm、Sm、Eu、Gd、Tb、Dy、Ho、Er、Tm、Yb和Lu中的至少一种以上构成,B元素由Zr、Ti、V、W、Hf、和Ta中一种以上构成,在0.05≤x<1(最好是0.1≤x≤0.3)的范围内含有Nb。 (2) The ferroelectric film of this embodiment is represented by the general formula of (Pb 1-y A y )(B 1-x Nb x )O 3 , and the A element is La, Ce, Pr, Nd, Pm, Sm, Eu , Gd, Tb, Dy, Ho, Er, Tm, Yb and Lu at least one or more, B element is composed of Zr, Ti, V, W, Hf, and Ta at least one or more, in 0.05≤x< 1 (preferably 0.1≤x≤0.3) contains Nb.
(3)本实施方式的强电介质膜是如下PZT类强电介质膜,Ti组成比Zr组成多,并且,将Ti组成中2.5摩尔%以上,40摩尔以下(最好是10摩尔%以上30摩尔以下)置换成Nb。另外,该PZT类强电介质膜可具有正方晶系和菱面体晶系的至少一种晶体结构。并且,该PZT类强电介质膜可含有0.5摩尔%以上(更好是0.5摩尔%以上、不到5摩尔%)的Si或Si和Ge。另外,该PZT类强电介质膜可使用溶胶凝胶溶液来形成。 (3) The ferroelectric film of the present embodiment is the following PZT ferroelectric film, the composition of Ti is more than that of Zr, and the Ti composition is more than 2.5 mol % and not more than 40 mol (preferably more than 10 mol % and not more than 30 mol). ) is replaced by Nb. In addition, the PZT-based ferroelectric film may have at least one crystal structure of a tetragonal system and a rhombohedral system. Furthermore, the PZT-based ferroelectric film may contain Si or Si and Ge at 0.5 mol % or more (more preferably 0.5 mol % or more and less than 5 mol %). In addition, the PZT-based ferroelectric film can be formed using a sol-gel solution. the
(4)本实施方式的强电介质膜是如下PZT类强电介质膜,由ABO3的通式表示,含有Pb来作为A侧的构成元素,至少含有Zr和Ti来作为B侧的构成元素。该PZT类强电介质膜中A侧的Pb缺损量比所述ABO3的化学量理论组成最多也20摩尔%以下。该强电介质膜以相当于所述A侧的Pb缺损量的2倍的组成比在B侧含有Nb。该强电介质膜中,B侧的Ti组成比Zr组成高,并且可具有菱面体晶系的晶体结构。另外,该强电介质膜可使用溶胶凝胶溶液来形成。 (4) The ferroelectric film of this embodiment is a PZT-based ferroelectric film represented by the general formula of ABO 3 , contains Pb as a constituent element on the A side, and contains at least Zr and Ti as constituent elements on the B side. The amount of Pb deficiency on the A side of the PZT-based ferroelectric film is at most 20 mol% or less than the stoichiometric theoretical composition of the ABO 3 . The ferroelectric film contains Nb on the B side at a composition ratio equivalent to twice the amount of Pb deficiency on the A side. In this ferroelectric film, the Ti composition on the B side is higher than the Zr composition, and may have a rhombohedral crystal structure. In addition, the ferroelectric film can be formed using a sol-gel solution.
(5)本实施方式的强电介质膜的制造方法是PZT类强电介质膜的制造方法,使用混合PbZrO3用溶胶凝胶溶液、PbTiO3用溶胶凝胶溶液、和PbNbO3用溶胶凝胶溶液的溶液作为所述溶胶凝胶溶液。 (5) The manufacturing method of the ferroelectric film of the present embodiment is a manufacturing method of a PZT-based ferroelectric film , using a mixture of a sol-gel solution for PbZrO , a sol-gel solution for PbTiO , and a sol-gel solution for PbNbO 3 solution as the sol-gel solution.
在本实施方式的强电介质膜的制造方法中,可使用进一步混合PbSiO3用溶胶凝胶溶液的溶液作为所述溶胶凝胶溶液。 In the method for producing a ferroelectric film according to this embodiment, a solution obtained by further mixing a sol-gel solution for PbSiO 3 can be used as the sol-gel solution.
(6)本实施方式的强电介质膜的制造方法是PZT类强电介质膜的制造方法,在将作为A侧的构成元素的Pb的化学量理论组成设为1的情况下,使用在0.9~1.2范围内含有Pb的溶胶凝胶溶液来形成。 (6) The method for producing a ferroelectric film of this embodiment is a method for producing a PZT-based ferroelectric film, and when the stoichiometric composition of Pb as a constituent element on the A side is set to 1, it is used in the range of 0.9 to 1.2 The sol-gel solution containing Pb in the range is formed. the
(7)本实施方式的强电介质膜的制造方法可含有在由铂类金属构成的金属膜上形成所述PZT类强电介质膜。 (7) The method for producing a ferroelectric film according to this embodiment may include forming the PZT-based ferroelectric film on a metal film made of a platinum-based metal. the
(8)在本实施方式的强电介质膜的制造方法中,所述铂类金属是Pt和Ir的至少任一种。 (8) In the method for producing a ferroelectric film according to this embodiment, the platinum-based metal is at least one of Pt and Ir. the
(9)本实施方式的强电介质存储器含有与事先形成于Si晶片上的CMOS晶体管的源极或漏极电极之一导通的第1电极、形成于所述第1电极上的强电介质膜、形成于所述强电介质膜上的第2电极,由所述第1电极、所述强电介质膜和所述第2电极构成的电容利用事先形成于Si晶片上的CMOS晶体管进行选择动作,其中,所述强电介质膜由Ti比率为50%以上的正方晶体PZT构成,Ti组成中5摩尔%以上40摩尔%以下由Nb置换,同时由含有1摩尔%以上的Si和Ge的强电介质膜构成。 (9) The ferroelectric memory according to the present embodiment includes a first electrode electrically connected to one of the source or drain electrodes of a CMOS transistor previously formed on a Si wafer, a ferroelectric film formed on the first electrode, The second electrode formed on the ferroelectric film, the capacitor formed by the first electrode, the ferroelectric film and the second electrode is selected by a CMOS transistor previously formed on the Si wafer, wherein, The ferroelectric film is composed of tetragonal PZT with a Ti ratio of 50% or more, 5 mol% to 40 mol% of the Ti composition is replaced by Nb, and it is composed of a ferroelectric film containing 1 mol% or more of Si and Ge. the
(10)本实施方式的强电介质存储器含有事先形成的第1电极、沿与所述第1电极交叉的方向排列的第2电极、和至少配置在所述第1电极与所述第2电极的交叉区域中的强电介质膜,由所述第1电极、所述强电介质膜和所述第2电极构成的电容被配置成矩阵状,其中,所述强电介质膜由Ti比率为50%以上的正方晶体PZT构成,Ti组成中5摩尔%以上40摩尔%以下由Nb置换,同时由含有1摩尔%以上的Si和Ge的强电介质膜构成。 (10) The ferroelectric memory of this embodiment includes a first electrode formed in advance, a second electrode arranged in a direction intersecting the first electrode, and at least one electrode disposed between the first electrode and the second electrode. The ferroelectric film in the intersecting region, the capacitors composed of the first electrode, the ferroelectric film and the second electrode are arranged in a matrix, wherein the ferroelectric film is made of a Ti ratio of 50% or more Composed of tetragonal crystal PZT, 5 mol% to 40 mol% of the Ti composition is replaced by Nb, and it is composed of a ferroelectric film containing 1 mol% or more of Si and Ge. the
(11)本实施方式的强电介质存储器的制造方法,包括:在涂布后结晶化作为第1原料溶液的PbZrO3形成用溶胶凝胶溶液、作为第2原料溶液的PbTiO3形成用溶胶凝胶溶液、作为第3原料溶液的PbNbO3形成用溶胶凝胶溶液与作为第4原料溶液的PbSiO3形成用溶胶凝胶溶液的工序,所述第1、第2和第3原料溶液是形成强电介质层用的原料液,第4原料溶液是生成具有将第1、第2和第3原料溶液形成为强电介质层时不可缺少的催化剂效应的常电介质层用的原料液。 (11) The method for manufacturing a ferroelectric memory according to this embodiment includes: crystallizing a sol-gel solution for forming PbZrO 3 as a first raw material solution after coating, and a sol-gel solution for forming PbTiO 3 as a second raw material solution. solution, a sol-gel solution for forming PbNbO3 as the third raw material solution, and a sol-gel solution for forming PbSiO3 as the fourth raw material solution, the first, second and third raw material solutions are for forming ferroelectric The raw material solution for the layer, the fourth raw material solution is the raw material solution for forming the permanent dielectric layer having the catalytic effect indispensable for forming the first, second and third raw material solutions into the ferroelectric layer.
(12)本实施方式的强电介质电容器的制造方法,包括:在所定的基体上形成下部电极的工序;在所述下部电极上形成由含有Pb、Zr、Ti和Nb作为构成元素的PZTN复合氧化物构成的强电介质膜的工序;在所述强电介质膜上形成上部电极的工序;形成保护膜,以覆盖所述下部电极、强电介质膜和上部电极的工序;和至少在形成所述保护膜之后,进行用于结晶化所述PZTN复合氧化物用的热处理的工序。 (12) The method for manufacturing a ferroelectric capacitor according to this embodiment includes: a step of forming a lower electrode on a predetermined substrate; The process of forming a ferroelectric film made of material; the process of forming an upper electrode on the ferroelectric film; the process of forming a protective film to cover the lower electrode, ferroelectric film and upper electrode; and at least forming the protective film Thereafter, a heat treatment step for crystallizing the PZTN composite oxide is performed. the
根据本实施方式,作为强电介质膜的材料,使用含有Pb、Zr、Ti和Nb作为构成元素的PZTN复合氧化物,在形成保护膜之后进行这种PZTN复合氧化物的结晶化。因此,即便假设在形成保护膜时、强电介质膜受到加工中产生的氢的损害,也可通过此后进行结晶化用的热处理,在恢复这种损害的同时,结晶化PZTN复合氧化物。因此,可省略以往那样形成保护强电介质膜不受还原反应用的阻挡膜的加工,可实现生产性的提高和生产成本的降低。 According to this embodiment, a PZTN composite oxide containing Pb, Zr, Ti, and Nb as constituent elements is used as a material of the ferroelectric film, and crystallization of this PZTN composite oxide is performed after forming a protective film. Therefore, even if the ferroelectric film is damaged by hydrogen generated during processing when the protective film is formed, the PZTN composite oxide can be crystallized while recovering the damage by subsequent heat treatment for crystallization. Therefore, the conventional process of forming a barrier film for protecting the ferroelectric film from the reduction reaction can be omitted, thereby improving productivity and reducing production cost. the
(13)在本实施方式的强电介质电容器的制造方法中,所述强电介质膜在形成 时在氧化气氛下实施临时热处理,在进行结晶化所述PZTN复合氧化物的热处理之前,变为非晶状态。 (13) In the method for manufacturing a ferroelectric capacitor according to this embodiment, the ferroelectric film is temporarily heat-treated in an oxidizing atmosphere during formation, and becomes amorphous before the heat treatment for crystallizing the PZTN composite oxide is performed. state. the
根据该方式,在结晶化强电介质膜之前,变为非晶状态。因此,该方式的强电介质膜中,可在形成保护膜之前,通过非晶状态来防止粒界扩散造成的结晶品质的恶化。另外,非晶状态的强电介质膜由于在氧化气氛下实施临时热处理,所以向膜中导入氧。因此,在结晶化用的热处理时,可不依赖于气氛中含有的气体种类来进行PZTN复合氧化物的结晶化。 According to this aspect, before the ferroelectric film is crystallized, it becomes an amorphous state. Therefore, in the ferroelectric film of this form, deterioration of crystal quality due to grain boundary diffusion can be prevented by the amorphous state before forming the protective film. In addition, since the ferroelectric film in the amorphous state is temporarily heat-treated in an oxidizing atmosphere, oxygen is introduced into the film. Therefore, during heat treatment for crystallization, crystallization of the PZTN composite oxide can proceed regardless of the type of gas contained in the atmosphere. the
(14)本实施方式的强电介质电容器的制造方法中,所述保护膜是氧化硅膜,可使用三甲硅烷来形成。 (14) In the method for manufacturing a ferroelectric capacitor according to this embodiment, the protective film is a silicon oxide film, which can be formed using trimethylsilane. the
根据该方式,与形成氧化硅膜中一般使用的四乙基原硅酸盐(TEOS)相比,由于使用加工中产生的氢量少的三甲硅烷(TMS)来形成由氧化硅膜构成的保护膜,所以可降低对强电介质膜的还原反应造成的损害。 According to this method, compared with tetraethylorthosilicate (TEOS) generally used for forming silicon oxide films, trimethylsilane (TMS) which generates less hydrogen during processing is used to form a protective film made of silicon oxide films. film, so the damage to the reduction reaction of the ferroelectric film can be reduced. the
(15)在本实施方式的强电介质电容器的制造方法中,可在非氧化气氛中进行结晶化所述PZTN复合氧化物的热处理。 (15) In the method for manufacturing a ferroelectric capacitor according to this embodiment, the heat treatment for crystallizing the PZTN composite oxide may be performed in a non-oxidizing atmosphere. the
根据该方式,由于在非氧化气氛中进行结晶化用的热处理,所以例如即便在加工中的器件中含有电容之外的外围部件(例如金属配线)等的情况下,也可防止外围部件受到高温热处理引起的氧化损害。 According to this aspect, since the heat treatment for crystallization is performed in a non-oxidizing atmosphere, for example, even if peripheral components (such as metal wiring) other than capacitors are included in the device being processed, the peripheral components can be prevented from being damaged. Oxidative damage caused by high temperature heat treatment. the
(16)本实施方式的强电介质电容器使用上述强电介质电容器的制造方法来形成。 (16) The ferroelectric capacitor of the present embodiment is formed using the method for manufacturing a ferroelectric capacitor described above. the
(17)另外,本实施方式的强电介质膜和强电介质电容器可适用于使用其的强电介质存储器、压电元件和半导体元件中。 (17) In addition, the ferroelectric film and the ferroelectric capacitor of this embodiment can be applied to ferroelectric memories, piezoelectric elements, and semiconductor elements using them. the
下面,参照附图来详细说明本发明的最佳实施方式。 Hereinafter, preferred embodiments of the present invention will be described in detail with reference to the drawings. the
1、强电介质膜、强电介质电容器及其制造方法 1. Ferroelectric film, ferroelectric capacitor and manufacturing method thereof
图1是模式地表示使用本发明的实施方式的强电介质膜101的强电介质电容器100的截面图。 FIG. 1 is a cross-sectional view schematically showing a
如图1所示,强电介质电容器100由强电介质膜101、第1电极102和第2电极103构成。 As shown in FIG. 1 , a
第1电极102和第2电极103由Pt、Ir、Ru等贵金属的单体或以所述贵金属为主的复合材料构成。当强电介质的元素向第1电极102和第2电极103扩散时,在电极与强电介质膜101的界面部产生组成波动(偏差),磁滞的方型性降低,所以要求第1电极102和第2电极103具有强电介质膜的元素不扩散的致密性。 The
为了提高第1电极102和第2电极103的致密性,例如采用由质量重的气体溅射成膜的方法、使Y、La等的氧化物分散到贵金属电极中的方法等。 In order to improve the density of the
强电介质膜101使用由含有Pb、Zr、Ti作为构成元素的PZT类强电介质来形成。尤其是在本实施方式中,该强电介质膜101的特征在于采用向Ti侧中掺杂Nb的Pb(Zr、Ti、Nb)O3(PZTN)。 The
Nb与Ti尺寸(离子半径相近,原子半径相同。)大致相同,重量是Ti的2倍,即便晶格振动引起的原子间冲击也难以从晶格中逸出原子。另外,Nb的原子价在+5价时稳定,即便逸出Pb,也可利用Nb5+来补偿Pb逸出的价数。另外,结晶化时,即便产生Pb逸出,也因为逸出尺寸大的O,所以尺寸小的Nb容易进入。 Nb and Ti have roughly the same size (similar ionic radius and the same atomic radius.) and twice the weight of Ti. Even the interatomic impact caused by lattice vibration is difficult to escape atoms from the lattice. In addition, the atomic valence of Nb is stable at +5. Even if Pb escapes, Nb 5+ can be used to compensate for the escaped valence of Pb. In addition, even if Pb escapes during crystallization, Nb with a small size easily enters because O with a large size escapes.
另外,因为Nb的原子价还存在+4价,所以也可代替Ti4+来充分进行。另外,实际上Nb的共有结合性非常强,认为Pb也难以逸出(H.Miyazawa,E.Natori,S.Miyashita;Jpn.J.Appl.Phys.39(2000)5679)。 In addition, since the atomic valence of Nb still has a +4 valence, it can be sufficiently carried out instead of Ti 4+ . In addition, in fact, the co-combination of Nb is very strong, and it is considered difficult for Pb to escape (H. Miyazawa, E. Natori, S. Miyashita; Jpn. J. Appl. Phys. 39 (2000) 5679).
迄今为止,向PZT掺杂Nb主要在富Zr的菱面体晶区域中进行,但其量极少,为0.2~0.025mol%(J.Am.Ceram.Soc,84(2001)902;Phys.Rev.Let,83(1999)1347)左右。这样,认为不能掺杂大量Nb的主要原因在于若例如添加10摩尔%的Nb,则结晶化温度会上升到800度以上。 So far, doping Nb to PZT is mainly carried out in the rhombohedral region rich in Zr, but its amount is extremely small, being 0.2~0.025mol% (J.Am.Ceram.Soc, 84 (2001) 902; Phys.Rev . Let, 83 (1999) 1347) around. Thus, it is considered that the main reason why a large amount of Nb cannot be doped is that, for example, if 10 mol % of Nb is added, the crystallization temperature will rise to 800 degrees or more. the
因此,在形成强电介质膜101时,最好还例如以1~5摩尔%的比例添加PbSiO3硅酸盐。由此,可使PZTN的结晶化能量减轻。即,在使用PZTN作为强电介质膜101的材料时,可通过在添加Nb的同时,添加PbSiO3硅酸盐,实现PZTN的结晶化温度的降低。 Therefore, when forming the
下面,描述适用于本实施方式的强电介质电容器100的PZTN强电介质膜101的成膜方法的一例。 Next, an example of a method of forming the PZTN
PZTN强电介质膜101,可以准备由含有Pb、Zr、Ti和Nb至少之一的第1~第3原料溶液构成的混合溶液,通过热处理等使含有于这些混合液中的氧化物结晶化而得到。 The PZTN
作为第1原料溶液,可示例PZTN强电介质相的构成金属元素中,为了形成基于Pb和Zr的PbZrO3钙钛矿结晶,在无水状态下,在n-丁醇等溶剂中溶解了缩聚物的溶液。 As the first raw material solution, among the constituent metal elements of the PZTN ferroelectric phase, in order to form PbZrO3 perovskite crystals based on Pb and Zr, the polycondensate is dissolved in a solvent such as n-butanol in an anhydrous state. The solution.
作为第2原料溶液,可示例PZTN强电介质相的构成金属元素中,为了形成基于Pb和Ti的PbTiO3钙钛矿结晶,在无水状态下在n-丁醇等溶剂中溶解了缩聚物的溶液。 As the second raw material solution, among the constituent metal elements of the PZTN ferroelectric phase, in order to form PbTiO 3 perovskite crystals based on Pb and Ti, a polycondensate is dissolved in a solvent such as n-butanol in an anhydrous state. solution.
作为第3原料溶液,可示例PZTN强电介质相的构成金属元素中,为了形成基于Pb和Nb的PbNbO3钙钛矿结晶,在无水状态下在n-丁醇等溶剂中溶解了缩聚物的溶液。 As the third raw material solution, among the constituent metal elements of the PZTN ferroelectric phase, in order to form PbNbO 3 perovskite crystals based on Pb and Nb, a polycondensate is dissolved in a solvent such as n-butanol in an anhydrous state. solution.
在使用上述第1、第2和第3原料溶液,形成例如由PbZr0.2Ti0.8Nb0.2O3(PZTN)构成的强电介质膜101的情况下,可按(第1原料溶液)∶(第2原料溶液)∶(第3原料溶液)=2∶6∶2的比来进行混合。 In the case of using the above-mentioned 1st, 2nd and 3rd raw material solutions to form, for example, the
但是,即便使该混合溶液直接结晶化,在制作PZTN强电介质膜101时也必需高的结晶化温度。即,若混合Nb,则结晶化温度会急剧上升,在700度以下的可元件化的温度范围下由于不可能结晶化,所以以往不将5摩尔%以上的Nb用作Ti的置换元素,迄今为止不能得到添加剂的区域。另外,在含有Ti比Zr多的PZT正方晶体中,完全没有实例。这可从参考文献J.Am.Ceram.Soc,84(2001)902或Phys.Rev.Let,83(1999)1347等了解。 However, even if the mixed solution is directly crystallized, a high crystallization temperature is required to form the PZTN
因此,在本实施方式中,可通过例如在1摩尔%以上、不足5摩尔%下向上述混合溶液中进一步添加作为第4原料溶液的、为形成PbSiO3结晶,在无水状态下在n-丁醇等溶剂中溶解缩聚物的溶液来解决上述问题。 Therefore, in this embodiment, for example, in order to form PbSiO 3 crystals, in an anhydrous state, n- Solve the above-mentioned problems by dissolving the solution of the polycondensate in solvents such as butanol.
即,通过使用上述第1、第2、第3和第4溶液的混合溶液,可在PZTN的结晶化温度为700度以下的可元件化的温度范围下结晶化。 That is, by using the mixed solution of the above-mentioned first, second, third, and fourth solutions, it is possible to crystallize PZTN in a temperature range where the crystallization temperature of PZTN is 700 degrees or less and can be deviceized. the
具体而言,根据图2所示的流程图来成膜强电介质膜101。进行混合溶液涂布工序(步骤ST11)、乙醇去除工序~干燥热处理工序~脱脂热处理工序(步骤ST12、步骤ST13)等一连串工序期望次数,之后,通过结晶化退火(步骤ST14)进行烧成,形成强电介质膜101。 Specifically, the
下面示出各工序中的条件实例。 Examples of conditions in each step are shown below. the
首先,在Si基板上覆盖Pt等电极用贵金属,成膜下部电极(步骤ST10)。接着,通过旋涂法等涂布法进行混合液的涂布(步骤ST11)。具体而言,向Pt覆盖基板上滴下混合溶液。为了使滴下的溶液在基板的整个面中流动,以500rpm程度进行旋转后,使转速降低到50rpm以下,旋转约10秒。干燥热处理工序在150度~180度下进行(步骤ST13)。干燥热处理在大气气氛下使用热板等来进行。同样,在脱脂热处理工序中,在保持在300度~350度的热板上,在大气气氛下进行(步骤ST13)。结晶化用的烧成在氧气氛中使用热快速退火(RTA)等来进行(步骤ST14)。 First, a noble metal for electrodes such as Pt is covered on a Si substrate to form a film of a lower electrode (step ST10 ). Next, the mixed solution is applied by a coating method such as a spin coating method (step ST11 ). Specifically, the mixed solution was dropped onto the Pt-coated substrate. In order to make the dripped solution flow over the entire surface of the substrate, the substrate was rotated at about 500 rpm, and then the rotation speed was reduced to 50 rpm or less, and the substrate was rotated for about 10 seconds. The drying heat treatment step is performed at 150°C to 180°C (step ST13). The drying heat treatment is performed using a hot plate or the like in an air atmosphere. Similarly, in the degreasing heat treatment step, it is performed in an air atmosphere on a hot plate kept at 300°C to 350°C (step ST13). Firing for crystallization is performed in an oxygen atmosphere using rapid thermal annealing (RTA) or the like (step ST14 ). the
另外,烧成后的膜厚可为100~200nm左右。接着,在通过溅射法等形成上 部电极之后(步骤ST15),将形成第2电极与强电介质薄膜的界面、和改善强电介质薄膜的结晶性作为目的,与烧成时一样,在氧气氛中使用RTA等进行后期退火(步骤ST16),得到强电介质电容器100。 In addition, the film thickness after firing may be about 100 to 200 nm. Next, after the upper electrode is formed by sputtering or the like (step ST15), for the purpose of forming the interface between the second electrode and the ferroelectric thin film and improving the crystallinity of the ferroelectric thin film, as in the firing, the ferroelectric thin film is heated in an oxygen atmosphere. In this process, post-annealing is performed using RTA or the like (step ST16 ) to obtain the
下面,考察使用PZTN强电介质膜101对强电介质电容器100的磁滞特性的影响。 Next, the effect of using the PZTN
图3是模式地示出强电介质电容器100的P(极化)-V(电压)磁滞曲线的图。首先,当施加电压+Vs时,变为极化量P(+Vs),之后,当电压变为0时,变为极化量Pr。并且,当电压为-1/3Vs时,极化量变为P(~1/3Vs)。另外,当电压为-Vs时,极化量变为P(-Vs),当再次变为电压0时,变为极化量-Pr。另外,当电压为+1/3Vs时,极化量变为P(+1/3Vs)当电压再次变为+Vs时,极化量再次返回P(+Vs)。 FIG. 3 is a diagram schematically showing a P (polarization)-V (voltage) hysteresis curve of the
另外,强电介质电容器100就磁滞特性而言还具有以下特性。首先,在暂时施加电压Vs并变为极化量P(+Vs)之后,施加-1/3Vs的电压,并且在施加电压变为0时,磁滞环追踪图3中箭头A所示的轨迹,极化量具有稳定值PO(0)。另外,在暂时施加电压-Vs并将极化量变为P(-Vs)之后,施加+1/3Vs的电压,并且在施加电压变为0时,磁滞环追踪图3中箭头B所示的轨迹,极化量具有稳定值PO(1)。若该极化量PO(0)与极化量PO(1)的差足够大,则可利用所述特开平9-116107号公报等中公开的驱动法来使单纯矩阵型强电介质存储器装置动作。 In addition, the
另外,根据本实施方式的强电介质电容器100,可实现结晶化温度的低温化、磁滞的方型性的提高、Pr的提高。另外,基于强电介质电容器100的磁滞的方型性的提高对通过单纯矩阵型强电介质存储器装置的驱动而变得重要的扰动的 In addition, according to the
稳定性具有显著的效果。就单纯矩阵型强电介质存储器装置而言,由于向未进行写入、读出的单元也施加±1/3Vs的电压,所以需要在该电压下极化不变化,即扰动特性稳定。实际上,本申请发明人发现在一般的PZT中,当从极化的稳定状态开始沿使极化反转的方向提供108次1/3Vs脉冲时,极化量下降80%左右,但确认根据本实施方式的强电介质电容器100,则为10%以下的下降量。因此,若将本实施方式的强电介质电容器100适用于强电介质存储器装置中,则可实用化单纯矩阵型存储器。 Stability has a dramatic effect. In a simple matrix ferroelectric memory device, since a voltage of ±1/3Vs is applied to cells that are not written or read, it is necessary that the polarization does not change at this voltage, that is, the disturbance characteristics are stable. In fact, the inventors of the present application found that in a general PZT, when 10 8 1/3Vs pulses were applied in the direction of reversing the polarization from a stable state of polarization, the amount of polarization decreased by about 80%, but it was confirmed that According to the
下面,说明本实施方式的详细实施例。 Next, detailed examples of this embodiment will be described. the
[实施例1] [Example 1]
在本实施例中,比较本发明的PZTN与以往的PZT。成膜流程全部使用所述 的图2。 In this example, the PZTN of the present invention is compared with conventional PZT. The film formation process all uses the above-mentioned Figure 2. the
设Pb∶Zr∶Ti∶Nb=1∶0.2∶0.6∶0.2、1∶0.2∶0.7∶0.1和1∶0.3∶0.65∶0.05。即,设Nb添加量为整体的5~20摩尔%。这里添加0~1%的PbSiO3。 Let Pb:Zr:Ti:Nb=1:0.2:0.6:0.2, 1:0.2:0.7:0.1 and 1:0.3:0.65:0.05. That is, the amount of Nb added is 5 to 20 mol% of the whole. Here, 0-1% of PbSiO 3 is added.
图4A~图4C示出此时的膜的表面组织。另外,当利用X射线衍射法测定该膜的结晶性时,如图5A~图5C所示。在图5A所示的0%(无)的情况下,即便结晶化温度上升到800度,也仅得到常电介质烧绿石(Pyrochlore)。另外,在图5B所示的0.5%的情况下,PZT与烧绿石混合存在。另外,在图5C所示的1%的情况下,得到PZT(111)单一取向膜。另外,结晶性也是迄今为止没有得到的最好的。 4A to 4C show the surface structure of the film at this time. In addition, when the crystallinity of this film was measured by the X-ray diffraction method, it was as shown in FIGS. 5A to 5C . In the case of 0% (none) shown in FIG. 5A , even if the crystallization temperature was raised to 800° C., only the paradielectric pyrochlore (Pyrochlore) was obtained. In addition, in the case of 0.5% shown in FIG. 5B , PZT and pyrochlore are mixed. In addition, in the case of 1% shown in FIG. 5C, a PZT (111) single alignment film was obtained. In addition, the crystallinity is also the best that has not been obtained so far. the
接着,对添加1%PbSiO3的PZTN薄膜,当设膜厚为120~220nm后,如图6A~图6C和图7A~图7C所示,分别示出与膜厚成正比的结晶性。另外,图6A~图6C是表示膜厚120nm~200nm下的表面组织的电子显微镜照片,图7A~图7C是表示膜厚120nm~200nm下的PZTN薄膜的结晶性的基于X射线衍射法的测定结果。另外,如图8A~图8C和图9A~图9C所示,在膜厚为120nm~200nm的整个范围内,得到方型性好的磁滞特性。另外,图9A~图9C是图8A~图8C的磁滞曲线的放大图。尤其是如图9A~图9C所示,在本例的PZTN薄膜中,确认在2V以下的低电压下,磁滞充分打开,并且饱和。 Next, for the PZTN thin film added with 1% PbSiO 3 , when the film thickness is set to 120 to 220 nm, as shown in FIGS. In addition, FIGS. 6A to 6C are electron micrographs showing the surface structure at a film thickness of 120 nm to 200 nm, and FIGS. 7A to 7C show the crystallinity of the PZTN thin film at a film thickness of 120 nm to 200 nm measured by the X-ray diffraction method. result. In addition, as shown in FIGS. 8A to 8C and FIGS. 9A to 9C , hysteresis characteristics with good squareness were obtained over the entire range of the film thickness from 120 nm to 200 nm. In addition, FIGS. 9A to 9C are enlarged views of the hysteresis curves in FIGS. 8A to 8C . In particular, as shown in FIGS. 9A to 9C , in the PZTN thin film of this example, it was confirmed that the hysteresis was sufficiently opened and saturated at a low voltage of 2 V or less.
另外,就泄漏特性而言,如图10A和图10B所示,无论膜组成或膜厚如何,在施加2V时(饱和时),都为5×10-8~7×10-9A/cm2,非常好。 In addition, as shown in FIG. 10A and FIG. 10B , the leakage characteristic is 5×10 -8 to 7×10 -9 A/cm when 2 V is applied (at saturation), regardless of the film composition or film thickness. 2 , very good.
接着,在测定PbZr0.2Ti0.6Nb0.2O3薄膜的疲劳特性和静态印象时,如图11A和图11B所示,非常好。尤其是图11A所示的疲劳特性无论在上下电极中是否使用Pt都非常好。 Next, when the fatigue properties and static impressions of the PbZr 0.2 Ti 0.6 Nb 0.2 O 3 thin film were measured, they were very good as shown in FIGS. 11A and 11B . In particular, the fatigue characteristics shown in FIG. 11A are very good regardless of whether Pt is used for the upper and lower electrodes.
并且,如图12所示,尝试在基板601上形成下部电极602、本实施例的PZTN强电介质膜603、上部电极604的强电介质电容器600上形成基于臭氧TEOS的SiO2膜605。已知以往的PZT当进行基于臭氧TEOS的SiO2膜形成时,从TEOS产生的氢通过上部Pt,还原PZT,完全未示出磁滞,损伤PZT结晶。 Furthermore, as shown in FIG. 12 , an attempt was made to form an ozone-TEOS-based SiO 2 film 605 on a
但是,本实施例的PZTN强电介质膜603如图13所示,基本未恶化,保持良好的磁滞。即,可知本实施例的PZTN强电介质膜603的耐还原性强。另外,在本发明的正方晶体PZTN强电介质膜603中,当Nb未超过40摩尔%的情况下,对应于Nb的添加量,得到好的磁滞。 However, as shown in FIG. 13, the PZTN
接着,为了比较,进行以往的PZT强电介质膜的评价。作为以往的PZT,分别设Pb∶Zr∶Ti=1∶0.2∶0.8、1∶0.3∶0.7和1∶0.6∶0.4。其泄漏特性如图14所示,Ti含量越增加,则泄漏特性越恶化,在Ti:80%的情况下,当施加2V时,变为10-5A/cm2,可知不适用于存储器应用。同样,疲劳特性如图15所示,Ti含量越增加,则疲劳特性越恶化。另外,在印象后,如图16所示,可知基本上不读出数据。Next, the conventional PZT ferroelectric film was evaluated for comparison. As conventional PZT, Pb:Zr:Ti=1:0.2:0.8, 1:0.3:0.7, and 1:0.6:0.4 are respectively set. Its leakage characteristics are shown in Fig. 14. As the Ti content increases, the leakage characteristics deteriorate. In the case of Ti: 80%, when 2V is applied, it becomes 10 -5 A/cm 2 , which is not suitable for memory applications. . Likewise, as shown in FIG. 15 , the fatigue properties deteriorate as the Ti content increases. In addition, after the impression, as shown in Fig. 16, it can be seen that basically no data was read.
从以上实施例可知,本实施例的PZTN强电介质膜除解决以往认为PZT的本质是原因的泄漏电流增大和印象特性恶化等问题外,还可无论存储器的种类、结构如何将由于上述理由而不可使用的正方晶体PZT用于存储器用途中。另外,在由于相同理由而不使用正方晶体PZT的压电元件用途中也可适用本材料。 As can be seen from the above examples, the PZTN ferroelectric film of the present example solves the problems of increased leakage current and deterioration of image characteristics, which were thought to be the essence of PZT in the past. The tetragonal crystal PZT used is used in memory applications. In addition, this material can also be applied to piezoelectric element applications where tetragonal PZT is not used for the same reason. the
[实施例2] [Example 2]
在本实施例中,就PZTN强电介质膜而言,使Nb添加量变化为0.5、10、20、30、40摩尔%来比较强介电特性。对于全部试件,添加5摩尔%的PbSiO3硅酸盐。另外,向构成膜形成用原料的强电介质膜形成用溶胶凝胶溶液中添加琥珀酸甲酯,将pH设为6。成膜流程全部使用所述的图2。 In this example, for the PZTN ferroelectric film, the amount of Nb added was changed to 0.5, 10, 20, 30, and 40 mol % to compare the ferroelectric properties. For all test pieces, 5 mol% PbSiO3 silicate was added. Further, methyl succinate was added to the ferroelectric film-forming sol-gel solution constituting the film-forming raw material to set the pH to 6. The above-mentioned FIG. 2 was used for all the film formation processes.
图17~图19中示出测定本实施例的PZTN强电介质膜的磁滞特性。 17 to 19 show the measurement of the hysteresis characteristics of the PZTN ferroelectric film of this example. the
如图17A所示,在Nb添加量为0的情况下,得到漏泄的磁滞,但如图17B所示,当Nb添加量为5摩尔%时,得到绝缘性高的好的磁滞特性。 As shown in FIG. 17A , leakage hysteresis was obtained when the amount of Nb added was 0, but good hysteresis characteristics with high insulation were obtained when the amount of Nb added was 5 mol % as shown in FIG. 17B . the
另外,如图18A所示,强介电特性在Nb添加量为10摩尔%以往,基本上看不到变化。在Nb添加量为0的情况下,虽也有漏泄,但强介电特性中看不到变化。另外,如图18B所示,在Nb添加量为20摩尔%的情况下,得到方型性非常好的磁滞特性。 In addition, as shown in FIG. 18A , substantially no change in the ferroelectric properties was seen until the Nb addition amount was 10 mol %. In the case where the amount of Nb added was 0, although there was leakage, no change was observed in the ferroelectric characteristics. In addition, as shown in FIG. 18B , when the amount of Nb added was 20 mol%, hysteresis characteristics with very good squareness were obtained. the
但是,如图19A和图19B所示,当Nb添加量超过20摩尔%时,磁滞特性变化大,确认恶化。 However, as shown in FIGS. 19A and 19B , when the amount of Nb added exceeds 20 mol %, the hysteresis characteristic changes greatly and deterioration is confirmed. the
因此,比较X射线衍射图案,如图20所示。在Nb添加量为5摩尔%(Zr/Ti/Nb=20/75/5)的情况下,(111)峰值位置与以往未添加Nb的PZT膜时无变化,随着Nb添加量增加为20摩尔%(Zr/Ti/Nb=20/60/20)、40摩尔%(Zr/Ti/Nb=20/40/40),(111)峰值移位到低角侧。即,可知,无论PZT的组成是否富Ti为正方晶体区域,实际的结晶都变为菱面体晶。另外,可知随着结晶系的变化,强介电特性变化。 Therefore, compare the X-ray diffraction patterns, as shown in FIG. 20 . When the Nb addition amount is 5 mol% (Zr/Ti/Nb=20/75/5), the (111) peak position does not change from that of the conventional PZT film without Nb addition, and increases to 20 as the Nb addition amount increases. Mole % (Zr/Ti/Nb=20/60/20), 40 mole % (Zr/Ti/Nb=20/40/40), (111) peak shifted to the low angle side. That is, it can be seen that the actual crystal becomes a rhombohedral crystal regardless of whether the composition of PZT is Ti-rich in a tetragonal crystal region. In addition, it can be seen that the ferroelectric properties change with the change of the crystal system. the
另外,在添加45摩尔%Nb后,磁滞未打开,不能确认强介电特性(省略图示)。 In addition, after adding 45 mol % of Nb, the hysteresis did not open, and the ferroelectric characteristics could not be confirmed (illustration omitted). the
另外,已叙述了本发明的PZTN膜绝缘性非常高,但这里求出PZTN为绝缘 体的条件如图21所示。 In addition, it has been described that the PZTN film of the present invention has very high insulating properties, but the conditions for obtaining PZTN as an insulator here are shown in Fig. 21. the
即,本发明的PZTN膜的绝缘性非常高,以相当于Pb缺损量的2倍的组成比,向Ti侧添加Nb。另外,钙钛矿结晶从如图22所示的WO3的晶体结构可知,即便A侧离子缺损100%也成立,并且WO3的结晶系易变化。 That is, the PZTN film of the present invention has very high insulating properties, and Nb is added to the Ti side at a composition ratio equivalent to twice the amount of Pb defects. In addition, the perovskite crystal can be seen from the crystal structure of WO 3 shown in FIG. 22 , even if the A-side ion deficiency is 100%, it is established, and the crystal system of WO 3 is easy to change.
因此,在PZTN的情况下,通过添加Nb,积极地控制Pb缺损量,并且控制结晶系。 Therefore, in the case of PZTN, by adding Nb, the amount of Pb defects is actively controlled and the crystal system is controlled. the
这点表示出本实施方式的PZTN膜在应用于压电元件中也非常有效。一般在将PZT应用于压电元件的情况下,使用富Zr组成的菱面体晶区域。此时,将Zr丰富的PZT称为软系PZT。这如文字所示,意味着结晶软。例如,虽也在喷墨打印机的墨水喷出喷嘴中使用软系PZT,但由于太软,所以在粘度过高的墨水中,不能施加墨水压力压出。 This shows that the PZTN film of this embodiment is also very effective in application to piezoelectric elements. In general, when PZT is applied to a piezoelectric element, a rhombohedral domain having a Zr-rich composition is used. In this case, Zr-rich PZT is called soft PZT. This, as the text indicates, means crystalline soft. For example, although soft PZT is used in ink ejection nozzles of inkjet printers, it cannot be extruded by applying ink pressure because it is too soft for ink with too high viscosity. the
另一方面,将富Ti的正方晶体PZT称为硬系PZT,意味着牢固而脆。但是,在本发明的PZTN膜中,在作为硬类的同时,可人工地使结晶系变化成菱面体晶。其中,可通过Nb的添加量来使结晶系任意变化,并且,由于富Ti的PZT系强电介质膜的比介电常数小,所以可用低电压来驱动元件。 On the other hand, Ti-rich tetragonal crystal PZT is called hard PZT, which means firm and brittle. However, in the PZTN film of the present invention, it is possible to artificially change the crystal system to a rhombohedral crystal while being hard. Among them, the crystal system can be changed arbitrarily by the amount of Nb added, and since the specific permittivity of the Ti-rich PZT-based ferroelectric film is small, the device can be driven at low voltage. the
由此,例如可将迄今为止未使用的硬类PZT用于喷墨打印机的墨水喷出喷嘴中。另外,由于Nb使PZT变软,所以适度地硬,可提供不脆的PZT。 Thus, for example, hard PZT, which has not been used until now, can be used in ink ejection nozzles of inkjet printers. In addition, since Nb softens PZT, it is moderately hard and can provide PZT that is not brittle. the
最后,如上所述,本实施例中,不仅添加Nb,也可在添加Nb的同时,添加硅酸盐,由此降低结晶化温度。 Finally, as described above, in this embodiment, not only Nb is added, but silicate may be added at the same time as Nb, thereby lowering the crystallization temperature. the
[实施例3] [Example 3]
在本实施例中,例如从在由用作构成强电介质存储器的存储器单元部分的强电介质电容器、或例如构成喷墨打印机的墨水喷出喷嘴部分的压电执行元件的电极材料的Pt或Ir等铂类金属构成的金属膜上、形成PZTN膜的情况下的晶格匹配性的观点,研究了使用PZTN膜的有效性。铂类金属在元件应用PZT类强电介质膜的情况下,在变为确定强电介质膜的结晶取向性的底部膜的同时,还是作为电极材料也有用的材料。但是,由于两者的晶格匹配性不充分,所以就元件应用而言,强电介质膜的疲劳特性成为问题。 In this embodiment, for example, Pt or Ir used as an electrode material of a ferroelectric capacitor constituting a memory cell portion of a ferroelectric memory, or a piezoelectric actuator constituting an ink ejection nozzle portion of an inkjet printer, etc. The effectiveness of using a PZTN film was investigated from the viewpoint of lattice matching properties when a PZTN film is formed on a metal film composed of a platinum-based metal. When a PZT-based ferroelectric film is applied to a device, the platinum-based metal serves as an underlying film that determines the crystal orientation of the ferroelectric film and is also useful as an electrode material. However, the fatigue properties of the ferroelectric film pose a problem for device applications because the lattice matching properties of both are insufficient. the
因此,本申请发明人通过使Nb含有于PZT类强电介质膜的构成元素中,开发出改善PZT类强电介质膜与铂类金属薄膜之间的晶格不匹配的技术。图23A~图23C示出此时的PZT类强电介质膜的成膜工序。 Therefore, the inventors of the present application developed a technique for improving the lattice mismatch between the PZT-based ferroelectric film and the platinum-based metal thin film by including Nb in the constituent elements of the PZT-based ferroelectric film. 23A to 23C show the film-forming process of the PZT-based ferroelectric film at this time. the
首先,如图23A所示,准备所定的基板11。作为基板11,使用在SOI基板上形成TiOx层的基板。另外,作为基板11,可从公知的材料构成的基板中选择适当的基板来使用。 First, as shown in FIG. 23A , a
之后,如图23B所示,在基板11上,例如使用溅射法,形成由PT构成的金属膜(第1电极)102,之后,如图23C所示,在金属膜102上形成PZTN膜,作为强电介质膜101。用作形成PZTN膜的材料,例如可使用溶胶凝胶溶液。更具体而言,使用在混合PbZrO3用溶胶凝胶溶液、PbTiO3用溶胶凝胶溶液、和PbNbO3 用溶胶凝胶溶液的溶液中进一步添加PbNbO3用溶胶凝胶溶液的溶液。另外,PZTN膜,由于在构成元素中含有Nb,所以结晶化温度高。因此,为了使结晶化温度降低,最好使用进一步添加了PbSiO3用溶胶凝胶溶液的溶液。在本实施例中,利用旋涂法将上述溶胶凝胶溶液涂布在Pt金属膜102上,进行所定的热处理之后,进行结晶化。成膜工序的流程与图2所示的一样。 Afterwards, as shown in FIG. 23B, on the
在本实施例中,就将Nb的添加量设为0摩尔%~30摩尔%的范围的PZTN膜而言,使用X射线衍射法测定结晶的晶格常数如图24A和图24B所示。根据图24A和图24B,可知Nb的添加量越多,则a轴(或b轴)中的晶格常数与c轴中的晶格常数越接近。另外,图24A中的V(abc)是体积变换了晶格常数(a、b、c)后的指数。另外,图24A中的V/V0是PZTN结晶的V(abc)与体积变换未添加Nb的PZT结晶的晶格常数的指数V0之比。这样,也可根据V(abc)或V/V0栏来确认PZTN结晶随着Nb的添加量增加、结晶晶格变小。 In this example, for the PZTN film in which the amount of Nb added was in the range of 0 mol % to 30 mol %, the lattice constant of the crystal was measured by the X-ray diffraction method as shown in FIGS. 24A and 24B . From FIGS. 24A and 24B , it can be seen that the larger the amount of Nb added, the closer the lattice constant on the a-axis (or b-axis) is to the lattice constant on the c-axis. In addition, V(abc) in FIG. 24A is an index obtained by changing the volume of lattice constants (a, b, c). In addition, V/V 0 in FIG. 24A is the ratio of V(abc) of the PZTN crystal to the exponent V 0 of the volume
另外,在图25中示出根据如此添加Nb后形成的PZTN膜的晶格常数来计算与Pt金属膜的晶格常数(a、b、c+3.96)的晶格不匹配率,将Nb的添加量(摩尔%)设为横轴绘制的图。根据图25,对PZT类强电介质膜含有Nb的效果不仅上述各实施例中提高强电介质特性的效果,还确认该晶格常数接近Pt等铂类金属结晶的晶格常数的效果。尤其是在Nb的添加量为5摩尔以上的区域中,确认显著示出该效果。 In addition, Fig. 25 shows the calculation of the lattice mismatch rate with the lattice constant (a, b, c+3.96) of the Pt metal film from the lattice constant of the PZTN film formed after adding Nb in this way. The added amount (mol %) is a graph plotted on the horizontal axis. According to FIG. 25, the effect of adding Nb to the PZT-based ferroelectric film is not only the effect of improving the ferroelectric characteristics in the above-mentioned examples, but also the effect of the lattice constant close to that of platinum-based metal crystals such as Pt. In particular, it was confirmed that this effect is remarkably exhibited in the range where the amount of Nb added is 5 mol or more. the
因此,若使用本发明的方法,则减轻作为电极材料的金属膜与强电介质膜之间的晶格不匹配,例如,在Nb的添加量为30摩尔%时,确认晶格不匹配率改善至2%左右。这被认为在PZTN的晶体结构中,置换B侧的Ti原子的Nb原子与O原子之间产生同时具有离子结合性与共有结合性的强的结合,该结合力沿压缩结晶晶格的方向作用,晶格常数向变小的方向变化。 Therefore, if the method of the present invention is used, the lattice mismatch between the metal film as the electrode material and the ferroelectric film is reduced. For example, when the addition amount of Nb is 30 mol%, it is confirmed that the lattice mismatch ratio is improved to 2% or so. It is considered that in the crystal structure of PZTN, the Nb atom replacing the Ti atom on the B side and the O atom have a strong bond with both ionic bonding and shared bonding, and this bonding force acts in the direction of compressing the crystal lattice. , the lattice constant changes to a smaller direction. the
另外,Pt等铂类金属是化学上稳定的物质,适用于强电介质存储器或压电执行元件的电极材料,根据本实施例的方法,即便在该Pt金属膜上直接形成PZTN 膜,也可在比以往缓和晶格不匹配的同时,使界面特性提高。因此,本实施例的方法可减轻PZT类强电介质膜的疲劳特性,也适用于强电介质存储器或压电执行元件等的元件应用中。 In addition, platinum-based metals such as Pt are chemically stable substances, and are suitable for electrode materials of ferroelectric memories or piezoelectric actuators. According to the method of this embodiment, even if a PZTN film is directly formed on the Pt metal film, it can also be used on the Pt metal film. The interface properties are improved while relieving the lattice mismatch more than before. Therefore, the method of this embodiment can reduce the fatigue characteristics of the PZT ferroelectric film, and is also suitable for the application of components such as ferroelectric memories or piezoelectric actuators. the
(参考例) (reference example)
在本例中,制作PbZr0.4Ti0.6O3强电介质膜。 In this example, a PbZr 0.4 Ti 0.6 O 3 ferroelectric film is produced.
在以往的方法中,使用过剩地含有20%左右的Pb的溶液,这是为了抑制挥发Pb及降低结晶化温度。但是,不知得到的薄膜中过剩Pb如何,原本应以最小限度的Pb过剩量来进行抑制。 In the conventional method, a solution containing excessively about 20% of Pb is used for the purpose of suppressing volatilization of Pb and lowering the crystallization temperature. However, it is not known how excessive Pb is in the obtained thin film, but it should be suppressed with the minimum excess amount of Pb. the
因此,使用过剩Pb为0.5、10、15、20%的10重量%浓度的PbZr0.4Ti0.6O3 形成用溶胶凝胶溶液(溶剂:n-丁醇),进而分别添加1摩尔%的10重量%浓度的PbSiO3形成用溶胶凝胶溶液(溶剂:n-丁醇),进行图26所示的步骤ST20~步骤ST25的各工序,形成200nm的PbZr0.4Ti0.6O3强电介质膜。此时的表面组织如图27A~图27C所示,XRD图案如图28A~图28C所示。 Therefore, sol-gel solutions (solvent: n-butanol) for forming PbZr 0.4 Ti 0.6 O 3 with a concentration of 10% by weight with an excess of Pb of 0.5, 10, 15, and 20% (solvent: n-butanol) were used, and 1 mol% of 10% by weight was added. % concentration of PbSiO 3 formation sol-gel solution ( solvent : n-butanol), each step ST20 ~ step ST25 shown in FIG. The surface structure at this time is shown in FIGS. 27A to 27C , and the XRD patterns are shown in FIGS. 28A to 28C .
以往需要20%左右过剩的Pb,在5%过剩的Pb下示出结晶化充分进行。这表示仅1摩尔%的PbSiO3催化剂,为了降低PZT的结晶化温度,过剩Pb基本上消失。以后,全部使用5%Pb过剩溶液作为PZT、PbTiO3、和PbZrTiO3形成用溶液。 Conventionally, an excess of about 20% of Pb was required, but an excess of 5% of Pb showed that crystallization proceeded sufficiently. This represents only 1 mol% PbSiO3 catalyst, in order to lower the crystallization temperature of PZT, the excess Pb basically disappears. Hereafter, 5% Pb-excess solutions were all used as PZT, PbTiO 3 , and PbZrTiO 3 forming solutions.
接着,使用在按4∶6的比例混合的10重量%浓度的PbZrO3形成用溶胶凝胶溶液(溶剂:n-丁醇)和10重量%浓度的PbTiO3形成用溶胶凝胶溶液(溶剂:n-丁醇)的溶液中、添加1摩尔%10重量%浓度的PbSiO3形成用溶胶凝胶溶液(溶剂:n-丁醇)的混合溶液,按照图2的流程,制作200nm~PbZr0.4Ti0.6O3强电介质膜。此时的磁滞特性如图29A和图29B所示,方型性好。但是,可知同时泄漏。 Next, a sol-gel solution for forming PbZrO 3 at a concentration of 10% by weight (solvent: n-butanol) and a sol-gel solution for forming PbTiO 3 at a concentration of 10% by weight (solvent: n-butanol) mixed at a ratio of 4:6 (solvent: n-butanol) solution, add 1
另外,为了比较,在以往的方法中,使用所述图26的流程,使用在10重量%浓度的PbZr0.4Ti0.6O3形成用溶胶凝胶溶液(溶剂:n-丁醇)中、添加1摩尔%10重量%浓度的PbSiO3形成用溶胶凝胶溶液(溶剂:n-丁醇)的混合溶液,制作200nm-PbZr0.4Ti0.6O3强电介质膜。此时,磁滞特性如图30所示,未提供很好的磁滞。 In addition, for comparison, in the conventional method, using the flow chart of FIG. 26 , using a sol-gel solution (solvent: n-butanol) for forming PbZr 0.4 Ti 0.6 O 3 at a concentration of 10% by weight, adding 1 A mixed solution of a sol-gel solution (solvent: n-butanol) is used to form a PbSiO 3 with a concentration of 10% by weight by mole %, and a 200nm-PbZr 0.4 Ti 0.6 O 3 ferroelectric film is produced. At this time, the hysteresis characteristic is as shown in Fig. 30, and good hysteresis is not provided.
因此,在使用各强电介质膜进行脱气分析后,如图31A和图31B所示。 Therefore, after degassing analysis was performed using each ferroelectric film, as shown in FIGS. 31A and 31B . the
如图31A所示,利用PZT溶胶凝胶溶液制作的现有的强电介质膜相对于从室温到1000度的温度上升,始终确认联系于H或C的脱气。 As shown in FIG. 31A , the outgassing associated with H or C was always confirmed for the conventional ferroelectric film fabricated using the PZT sol-gel solution with respect to the temperature rise from room temperature to 1000°C. the
另一方面,如图31B所示,在使用按4∶6的比例混合10重量%浓度的PbZrO3 形成用溶胶凝胶溶液(溶剂:n-丁醇)和10重量%浓度的PbTiO3形成用溶胶凝胶溶液(溶剂:n-丁醇)的溶液的本发明的强电介质膜时,判明在分解之前基本上未见脱气。 On the other hand, as shown in FIG. 31B , when a sol-gel solution (solvent: n-butanol) for forming PbZrO 3 at a concentration of 10 wt % and a concentration of PbTiO 3 for forming 10 wt % were mixed at a ratio of 4:6, When using the ferroelectric film of the present invention as a solution of a sol-gel solution (solvent: n-butanol), it was found that there was substantially no outgassing before decomposition.
这认为是通过使用按4∶6的比例混合的10重量%浓度的PbZrO3形成用溶胶凝胶溶液(溶剂:n-丁醇)和10重量%浓度的PbTiO3形成用溶胶凝胶溶液(溶剂:n-丁醇)的溶液,首先利用混合溶液中的10重量%浓度的PbTiO3形成用溶胶凝胶溶液(溶剂:n-丁醇),PbTiO3在Pt上结晶化,这成为结晶初期核,而且,消除Pt与PZT的晶格不匹配,PZT容易结晶化。并且,认为通过使用混合溶液,PbTiO3与PZT在良好的界面上连续形成,与良好的磁滞的方型性相关联。 This is considered to be achieved by using a sol-gel solution for forming PbZrO 3 at a concentration of 10% by weight (solvent: n-butanol) and a sol-gel solution for forming PbTiO at a concentration of 10% by weight (solvent : n-butanol) solution, first use the 10% by weight concentration of PbTiO in the mixed solution to form a sol-gel solution (solvent: n-butanol), and PbTiO 3 crystallizes on Pt, which becomes the crystallization initial nucleus , Moreover, eliminating the lattice mismatch between Pt and PZT, PZT is easy to crystallize. Also, it is considered that by using a mixed solution, PbTiO 3 and PZT are continuously formed at a good interface, which is associated with good squareness of hysteresis.
2、强电介质电容器的制造方法 2. Manufacturing method of ferroelectric capacitor
图32A~图32C是模式地表示本发明实施方式的强电介质电容器的制造工序一例的截面图。 32A to 32C are cross-sectional views schematically showing an example of the manufacturing process of the ferroelectric capacitor according to the embodiment of the present invention. the
(1)首先,如图32A所示,在所定的基体110上依次层叠形成下部电极102、强电介质膜101、上部电极103。 (1) First, as shown in FIG. 32A , the
作为基体110,例如可任意采用半导体基板、树脂基板等适用于强电介质电容器用途的基板,不特别限定。 As the
作为下部电极102和上部电极103,例如可采用由Pt、Ir、Ru等贵金属单体或以所述贵金属为主的复合材料构成的电极。另外,下部电极102和上部电极103例如可使用溅射法或沉积法等公知的成膜方法来形成。另外,当强电介质的构成元素向下部电极102和上部电极103扩散时,在电极与强电介质膜101的界面部产生组成波动,磁滞的方型性降低,所以期望下部电极102和上部电极103具有强电介质的构成元素不扩散的致密性。因此,为了提高下部电极102和上部电极103的致密性,可采用由质量重的气体溅射成膜的方法、或使Y、La等的氧化物分散到贵金属电极中的方法等。 As the
强电介质膜101是含有Pb、Zr、Ti和Nb作为构成元素的所谓PZTN复合氧化物。另外,强电介质膜101,可通过例如使用旋涂法等将含有Pb、Zr、Ti、Nb的溶胶凝胶溶液涂布在下部电极102上来形成。作为这种溶胶凝胶溶液,可使用混合第1溶胶凝胶溶液、第2溶胶凝胶溶液和第3溶胶凝胶溶液的溶液,其中,第1溶胶凝胶溶液是为了形成基于Pb和Zr的PbZrO3钙钛矿结晶而在无水状态下在n-丁醇等溶剂中溶解缩聚物的溶液,第2溶胶凝胶溶液是为了形成基于PZTN强电介质相的构成金属元素中Pb和Ti的PbTiO3钙钛矿结晶而在无水状态 下在n-丁醇等溶剂中溶解缩聚物的溶液,第3溶胶凝胶溶液是为了形成基于PZTN强电介质相的构成金属元素中Pb和Nb的PbNbO3钙钛矿结晶而在无水状态下在n-丁醇等溶剂中溶解缩聚物的溶液。并且,在形成强电介质膜101时,为了降低PZTN复合氧化物的结晶化温度,也可添加含有硅酸盐或锗酸盐的溶胶凝胶溶液。具体而言,可以例如1摩尔%以上、不足5摩尔%向上述混合溶胶凝胶溶液中进一步添加第4溶胶凝胶溶液,该第4溶胶凝胶溶液例如是为了形成PbSiO3结晶而在无水状态下在n-丁醇等溶剂中溶解缩聚物的溶液。通过混合这种第4溶胶凝胶溶液,可在通过在构成元素中含有Nb、结晶化温度变高的PZTN复合氧化物的结晶化温度为700度以下的可元件化的温度范围下结晶化。 The
另外,最好强电介质膜101对这种涂布膜在氧化气氛中PZTN复合氧化物不结晶化的温度(例如400度以下)下进行临时热处理,将PZTN复合氧化物变为非晶状态。从而,强电介质膜101由于是非晶状态而变为不存在粒界的状态,可在防止构成元素扩散的同时推进后述的工序。另外,在氧化气氛中进行该临时热处理,也可起在后述的保护膜形成后向强电介质膜101中导入使PZTN复合氧化物结晶化所需的氧成分的作用。 In addition, it is preferable that
(2)接着,如图32B所示,蚀刻下部电极102、强电介质膜101和上部电极103,加工成期望的形状,形成由SiO2(氧化硅)膜构成的保护膜104,以覆盖所述下部电极、强电介质膜和上部电极。此时的保护膜104可使用三甲硅烷(TMS)利用CVD法形成。三甲硅烷(TMS)与氧化硅膜形成中一般使用的四乙基原硅酸盐(TEOS)相比,CVD工艺中的产生氢量少。因此,若使用三甲硅烷(TMS),则可降低对强电介质膜101的还原反应造成的工艺损害。另外,因为使用三甲硅烷(TMS)的保护膜104的形成工艺与使用TEOS的形成工艺(形成温度为400度以上)相比可在低温(室温~350度)下进行,所以在(1)工序中,在将强电介质膜101形成非晶状态的情况下,可防止由于这种保护膜104的形成工序中产生的热等PZTN复合氧化物结晶化,维持非晶状态不变。 (2) Next, as shown in FIG. 32B, the
(3)接着,如图32C所示,进行结晶化构成强电介质膜101的PZTN复合氧化物的热处理,可得到具有PZTN强电介质结晶膜101a的强电介质电容器。在该热处理中,不仅在氧气氛下,即便通过在例如Ar或N2等非氧化气体气氛下或大气中的热处理,也可结晶化PZTN复合氧化物。 (3) Next, as shown in FIG. 32C, a heat treatment is performed to crystallize the PZTN composite oxide constituting the
这里,就适用本实施方式的制造方法来在由PZTN强电介质膜、Pt上部电极构成的强电介质电容器上、形成使用TMS的SiO2保护膜而言,测定在这种SiO2 保护膜形成后在氧气氛中和大气中进行热处理后结晶化PZTN强电介质的情况下的电容磁滞特性的结果示于图33A和图33B中。图33A表示在氧气氛中进行热处理的情况,图33B表示在大气中进行热处理的情况。根据图33A和图33B,在氧气氛中和大气中任一气氛下进行热处理的情况下,尽管未形成耐氢用的阻挡膜,都可得到方型性好的磁滞特性。这是因为在强电介质膜101形成时在氧化气氛下实施临时热处理,所以事先向膜中导入结晶化所需的氧。即,在本实施方式的制造方法中,可不依赖于热处理的气氛来进行强电介质的结晶化。并且,在非氧化气体气氛下进行结晶化用的热处理的情况下,在适用于后述的强电介质存储器的制造方法的情况等中,可防止对电容以外的外围部件(例如金属配线)造成高温热处理引起的氧化损害。另外,这种工序中的PZTN复合氧化物的结晶化用热处理由于气氛中的气体种类的依赖性少,所以也可在保护膜104中形成用于形成将上部电极103与外部连接用的金属配线的接触孔之后再进行。 Here, when applying the production method of this embodiment to form a SiO 2 protective film using TMS on a ferroelectric capacitor composed of a PZTN ferroelectric film and a Pt upper electrode, it was measured that after the formation of such a SiO 2 protective film, The results of capacitive hysteresis characteristics in the case of crystallizing the PZTN ferroelectric after heat treatment in an oxygen atmosphere and in the air are shown in FIGS. 33A and 33B . FIG. 33A shows the case where the heat treatment is performed in an oxygen atmosphere, and FIG. 33B shows the case where the heat treatment is performed in the air. According to FIG. 33A and FIG. 33B , when the heat treatment is performed in either the oxygen atmosphere or the air atmosphere, hysteresis characteristics with good squareness can be obtained even though no hydrogen-resistant barrier film is formed. This is because when the
另外,就在适用由本实施方式的制造方法的Pt下部电极、PZTN强电介质膜、Pt上部电极构成的强电介质电容器上、形成使用TMS的SiO2保护膜、并在这种SiO2保护膜形成后结晶化PZTN强电介质而言,测定将SiO2保护膜的形成温度设为室温、125度、200度时的磁滞特性、和作为比较例不形成SiO2保护膜、而结晶化PZTN强电介质膜时的磁滞特性,并测量其残留极化量2Pr的值的变化的结果示于图34中。根据图34,即便在室温、125度、200度任一温度下形成SiO2 保护膜,残留极化量2Pr中都未见变化,确认得到不逊于形成SiO2保护膜时的值。即,在本实施方式的制造方法中,即便假设在形成保护膜104时强电介质膜101受到工艺中产生的氢引起的损害,也可通过之后进行PZTN复合氧化物的结晶化用热处理,在恢复这种损害的同时,结晶化PZTN复合氧化物,所以可省略以往必需的保护强电介质膜101不受还原反应影响的阻挡膜的形成工艺,可实现生产性的提高和生产成本的降低。 In addition, a SiO 2 protective film using TMS is formed on a ferroelectric capacitor composed of a Pt lower electrode, a PZTN ferroelectric film, and a Pt upper electrode to which the manufacturing method of this embodiment is applied, and after the SiO 2 protective film is formed, For the crystallized PZTN ferroelectric, the hysteresis characteristics were measured when the SiO2 protective film was formed at room temperature, 125 degrees, and 200 degrees, and as a comparative example, the crystallized PZTN ferroelectric film was not formed with a SiO2 protective film. Figure 34 shows the hysteresis characteristics and the measurement of the change in the value of the remanent polarization 2Pr. According to FIG. 34 , even when the SiO 2 protective film was formed at any temperature of room temperature, 125°C, or 200°C, there was no change in the residual polarization 2Pr, and it was confirmed that the value was not inferior to that obtained when the SiO 2 protective film was formed. That is, in the manufacturing method of the present embodiment, even if the
3、强电介质存储器 3. Ferroelectric memory
图35A和图35B是表示本发明的实施方式中的单纯矩阵型的强电介质存储器装置300的构成图。图35A是平面图,图35B是沿图35A的A-A线的截面图。强电介质存储器装置300如图35A和图35B所示,具有形成于基板308上的排列所定数量的字线301~303、和排列所定数量的位线304~306。在字线301~303与位线304~306之间,插入由上述实施方式中说明的PZTN构成的强电介质膜307,在字线301~303与位线304~306的交叉区域中形成强电介质电 容器。 35A and 35B are diagrams showing the configuration of a simple matrix ferroelectric memory device 300 according to an embodiment of the present invention. Fig. 35A is a plan view, and Fig. 35B is a cross-sectional view along line A-A of Fig. 35A. As shown in FIGS. 35A and 35B , the ferroelectric memory device 300 has a predetermined number of
在排列通过该单纯矩阵构成的存储器单元的强电介质存储器装置300中,利用未图示的外围的驱动电路或读出用放大电路等(将其称为外围电路)来进行对形成于字线301~303与位线304~306的交叉区域中的强电介质电容器的写入和读出。该外围电路通过MOS形成于存储器单元阵列以外的别的基板上,连接于字线301~303和位线304~306上,或者也可通过在基板308中使用单晶硅基板,将外围电路集成在与存储器单元阵列相同的基板上。 In the ferroelectric memory device 300 in which the memory cells constituted by this simple matrix are arranged, a peripheral drive circuit, a readout amplifier circuit, etc. (not shown in the figure) (referred to as a peripheral circuit) are used to perform pairing formed on the
图36是表示本实施方式中的、将存储器单元阵列与外围电路共同集成在同一基板上的强电介质存储器装置300的一例的截面图。 36 is a cross-sectional view showing an example of a ferroelectric memory device 300 in which a memory cell array and peripheral circuits are commonly integrated on the same substrate in this embodiment. the
图36中,在单晶硅基板401上形成MOS晶体管402,该晶体管形成区域构成外围电路部。MOS晶体管402由单晶硅基板401、源极·漏极区域405、栅极绝缘膜403和栅极电极404构成。 In FIG. 36, a
另外,强电介质存储器装置300具有元件分离用氧化膜406、第1夹层绝缘膜407、第1配线层408和第2夹层绝缘膜409。 In addition, the ferroelectric memory device 300 has an
另外,强电介质存储器装置300,具有由强电介质电容器420构成的存储器单元阵列,强电介质存储器420,由构成字线或位线的下部电极(第1电极或第2电极)410、含有强电介质相与常电介质相的强电介质膜411、和形成于强电介质膜411上并构成位线或字线的上部电极(第2电极或第1电极)412构成。 In addition, the ferroelectric memory device 300 has a memory cell array composed of
并且,强电介质存储器装置300在强电介质电容器420上具有第3夹层绝缘膜413,利用第2配线层414来连接存储器单元阵列与外围电路。就强电介质存储器装置300而言,在第3夹层绝缘膜413与第2配线层414上形成保护膜415。 Furthermore, the ferroelectric memory device 300 has a third
根据具有以上构成的强电介质存储器装置300,可以在同一基板上集成存储器单元阵列与外围电路部。另外,图36所示的强电介质存储器装置300是在外围电路部上形成存储器单元阵列的构成,但也可构成为不在外围电路部上配置存储器单元阵列,存储器单元阵列与外围电路部平面地接触。 According to the ferroelectric memory device 300 having the above configuration, the memory cell array and the peripheral circuit unit can be integrated on the same substrate. In addition, the ferroelectric memory device 300 shown in FIG. 36 has a structure in which a memory cell array is formed on the peripheral circuit portion, but it may also be configured such that the memory cell array is not disposed on the peripheral circuit portion, and the memory cell array and the peripheral circuit portion are in planar contact. . the
本实施方式中使用的强电介质电容器420,由于由上述实施方式的PZTN构成,所以磁滞的方形性非常好,具有稳定的扰动特性。并且,该强电介质电容器420由于加工温度的低温化,对外围电路等其它元件的损害少,另外,加工损害(尤其是氢的还原)少,所以可抑制损害引起的磁滞恶化。因此,通过使用这种强电介质电容器420,可实用化单纯矩阵型强电介质存储器装置300。 Since the
另外,图37A中表示1T1C型强电介质存储器装置500的结构图,作为变形 例。图37B是强电介质存储器装置500的等效电路图。 In addition, FIG. 37A shows a configuration diagram of a 1T1C type
如图37A所示,强电介质存储器装置500是由下部电极501、连接于板极线上的上部电极502、和适用本实施方式的PZTN强电介质的强电介质膜503构成的电容504(1C),和源极/漏极电极之一方连接于数据线505上、并具有连接于字线上的栅极电极506的开关用晶体管元件507(1T)构成的,类似于DRAM的结构的存储器元件。1T1C型的存储器的写入和读出可在100ns以下高速进行,并且,由于写入的数据不易失,所以期望SRAM的置换等。 As shown in FIG. 37A, a
4、强电介质存储器的制造方法 4. Manufacturing method of ferroelectric memory
下面,说明将“2、强电介质电容器的制造方法”栏中说明的制造方法适用于强电介质存储器的制造方法中的情况。 Next, a case where the manufacturing method described in the column "2. Manufacturing method of a ferroelectric capacitor" is applied to a manufacturing method of a ferroelectric memory will be described. the
图38A~图38C是模式地表示本发明实施方式的强电介质存储器的制造工序一例的截面图。 38A to 38C are cross-sectional views schematically showing an example of the manufacturing process of the ferroelectric memory according to the embodiment of the present invention. the
在本实施方式中,首先如图38A所示,在基体110上依次形成强电介质电容器100的下部电极102、PZTN强电介质膜101、上部电极103。此时,PZTN强电介质膜101在氧化气氛中实施临时热处理后变为非晶状态。另外,作为基体100,例如图38A所示,可使用在半导体基体111上形成单元选择用的晶体管116的基体。该晶体管116可具有源极/漏极113、栅极氧化膜114、栅极电极115。另外,在晶体管116之一方的源极/漏极113上,例如形成由钨等构成的插头电极117,可采用可与强电介质电容器100的下部电极102连接地形成的堆叠结构。另外,在基体110内,晶体管116在单元间利用元件分离区域112对每个单元分离,在晶体管116的上部,例如可具有由氧化膜等构成的夹层绝缘膜118。 In this embodiment, first, as shown in FIG. 38A ,
接着,在本实施方式的制造工序中,如图38B所示,将强电介质电容器110图案化成期望的大小和形状。之后,使用三甲硅烷(TMS)形成由SiO2保护膜104,以覆盖强电介质电容器100,并在其中形成外部连接用的接触孔105之后,进行热处理,结晶化PZTN强电介质,形成PZTN强电介质膜101a。在PZTN强电介质的结晶化时,可在非氧化气氛中进行结晶化用的热处理。据此,可防止对强电介质电容器100之外的外围部件(例如金属配线)等造成高温热处理引起的氧化损害。 Next, in the manufacturing process of this embodiment, as shown in FIG. 38B ,
最终,如图38C所示,在SiO2保护膜104中形成将晶体管116与餐饮部连接用的接触孔,并通过形成金属配线层191、192来得到强电介质存储器。根据本实施方式的制造工序,可省略以往必需的保护强电介质膜101不受还原反应损 害用的阻挡膜的形成工艺,可实现生产性的提高和生产成本的降低。另外,由于即便省略这种阻挡膜的形成工艺也可形成具有方型性好的磁滞特性的强电介质电容器100,所以可以得到好的特性的强电介质存储器。 Finally, as shown in FIG. 38C , a contact hole for connecting the
另外,上述说明了所谓1T1C型强电介质存储器的制造工序,但本实施方式的强电介质电容器的制造方法,此外还可适用于所谓2T2C型或单纯矩阵型(交叉点型)等使用各种单元方式的强电介质存储器的制造工序中。 In addition, the manufacturing process of a so-called 1T1C type ferroelectric memory has been described above, but the method of manufacturing a ferroelectric capacitor according to this embodiment can also be applied to a so-called 2T2C type or a simple matrix type (cross-point type) using various cell systems. In the manufacturing process of ferroelectric memory. the
5、压电元件和喷墨式记录头 5. Piezoelectric element and inkjet recording head
下面,详细说明本发明实施方式中的喷墨式记录头。 Next, the ink jet type recording head in the embodiment of the present invention will be described in detail. the
在如下喷墨式记录头中,即由振动板构成与喷出墨滴的喷嘴开口连通的压力产生室的一部分,通过压电元件使该振动板变形,对压力产生室的墨水施压,从喷嘴开口喷出墨滴,实用化使用沿压电元件的轴向伸缩的纵向振动模式的压电执行元件的喷墨式记录头、与使用弯曲振动模式的压电执行元件的喷墨式记录头等两种。 In the ink jet type recording head, a vibrating plate constitutes a part of a pressure generating chamber communicating with a nozzle opening from which ink droplets are ejected, and the vibrating plate is deformed by a piezoelectric element to pressurize the ink in the pressure generating chamber to thereby The nozzle opening ejects ink droplets, and the inkjet recording head using the piezoelectric actuator in the longitudinal vibration mode that expands and contracts in the axial direction of the piezoelectric element, and the inkjet recording head using the piezoelectric actuator in the bending vibration mode, etc. two kinds. the
另外,作为使用弯曲振动模式的执行元件的喷墨式记录头,例如已知通过成膜技术在振动板的表面整体中形成均匀的压电体层,并利用光刻法将该压电体层分割成对应于压力产生室的形状,对每个压力产生室独立地形成压电元件。 In addition, as an inkjet type recording head using an actuator in a bending vibration mode, for example, it is known to form a uniform piezoelectric layer on the entire surface of the vibrating plate by a film-forming technique, and to form the piezoelectric layer by photolithography. It is divided into shapes corresponding to the pressure generating chambers, and piezoelectric elements are formed independently for each pressure generating chamber. the
图39是表示本发明的一实施方式的喷墨式记录头的示意分解立体图,图40A、40B是图39的平面图和A-A’截面图,图41是表示压电元件700的层结构的示意图。如图所示,流路形成基板10在本实施方式中由面方位(110)单晶硅基板构成,在其一方的面中形成事先通过热氧化形成的、由二氧化硅构成的厚度为1~2微米的弹性膜50。在流路形成基板10中,沿其宽度方向并列设置有多个压力产生室12。另外,在流路形成基板10的压力产生室12的长向外侧的区域中,形成连通部13,连通部13与各压力产生室12经对每个压力产生室12设置的墨水提供路径14连通着。另外,连通部13与后述的密封基板30的储备部32连通,构成形成各压力产生室12的共同墨水室的储备器800的一部分。墨水提供路径14以比压力产生室12窄的宽度形成,将从连通部13流入压力产生室12中的墨水的流路阻抗保持恒定。 39 is a schematic exploded perspective view showing an ink jet recording head according to an embodiment of the present invention. FIGS. 40A and 40B are a plan view and an AA' sectional view of FIG. schematic diagram. As shown in the figure, the channel-forming
另外,在流路形成基板10的开口面侧,经粘接剂或热熔融膜等固定着贯穿设置连通于与各压力产生室12的墨水提供路径14相反侧的端部附近上的喷嘴开口21的喷嘴板20。 In addition, on the opening surface side of the flow
另一方面,在这种流路形成基板10的开口面的相反侧,如上所述,形成厚 度约为1.0微米的弹性膜50,在该弹性膜50上,形成有厚度约为0.4微米的绝缘体膜55。并且,在该绝缘体膜55上,利用后述的工艺层叠形成厚度约为0.2微米的下电极膜60、厚度约为1.0微米的压电体层70、和厚度约为0.05微米的上电极膜80,以构成了压电元件700。这里,压电元件700是指含有下电极膜60、压电体层70和上电极膜80的部分。通常,将压电元件700的任一电极作为共同电极,对每个压力产生室12图案化另一方的电极和压电体层70来构成。而且,在此将由图案化的任一方电极和压电体层70构成、通过向两电极施加电压、产生压电变形的部分称为压电体能动部。在本实施方式中,将下电极膜60设为压电元件700的共同电极,将上电极膜80设为压电元件700的单独电极,但通过驱动电路或配线的配合,即便将之颠倒也无妨。在任一情况下,都可以对每个压电产生室形成了压电体能动部。这里,将压电元件700与利用该压电元件700的驱动产生位移的振动板合称为压电执行元件。另外,压电体层70对每个压力产生室12独立设置,如图40所示,由多层的强电介质膜71(71a~71f)构成。 On the other hand, on the opposite side of the opening surface of the flow
喷墨式记录头构成具备与墨水卡盘等连通的墨水流路的记录头单元的一部分,被装载于喷墨式记录装置上。图42是表示该喷墨式记录装置的一例的示意图。如图42所示,具有喷墨式记录头的记录头单元1A和1B可拆装地设置构成墨水提供单元的卡盘2A和2B,装载该记录头单元1A和1B的托架3被轴向自由移动地设置在安装于装置主体4上的托架轴5上。该记录头单元1A和1B例如分别喷出黑墨水组合物和彩色墨水组合物。另外,通过将驱动电机6的驱动力经未图示的多个齿轮和同步皮带7传递给托架3,使装载记录头单元1A和1B的托架3沿托架轴5移动。另一方面,在装置主体4上沿托架轴5设置压板8,在压板8上传输由未图示的供纸辊等供纸的纸等作为记录媒体的记录薄片S。 The inkjet recording head constitutes a part of a recording head unit having an ink flow path communicating with an ink cartridge or the like, and is mounted on an inkjet recording apparatus. FIG. 42 is a schematic diagram showing an example of the ink jet recording device. As shown in FIG. 42,
另外,将喷出墨水的喷墨式记录头作为一例说明为液体喷射头,但本发明也可以使用压电元件的液体喷射头和液体喷射装置整体作为对象。作为液体喷射头,例如有用于打印机等图像记录装置中的记录头、用于液晶显示器等滤色镜的制造中的色材喷射头、用于有机EL显示器、FED(面发光显示器)等电极形成的电极材料喷射头、用于生物芯片制造中的生物有机物喷射头等。 In addition, an inkjet type recording head that ejects ink is described as an example of a liquid ejection head, but the present invention may also be a liquid ejection head using a piezoelectric element and a liquid ejection device as a whole. Examples of liquid ejection heads include recording heads used in image recording devices such as printers, color material ejection heads used in the manufacture of color filters such as liquid crystal displays, and electrodes used in electrode formation such as organic EL displays and FEDs (surface emission displays). Material injection head, bio-organic matter injection head used in biochip manufacturing, etc. the
本实施方式的压电元件由于将上述实施方式的PZTN膜用于压电体层中,所以得到如下效果。 In the piezoelectric element of this embodiment, since the PZTN film of the above-mentioned embodiment is used for the piezoelectric layer, the following effects are obtained. the
(1)由于提高压电体层中的共有结合性,所以使压电常数提高。 (1) The piezoelectric constant is increased by increasing the shared bonding property in the piezoelectric layer. the
(2)由于可抑制压电体层中的PbO缺损,所以抑制压电体层与电极的界面中 的异相的产生,容易施加电场,使作为压电元件的效率提高。 (2) Since PbO defects in the piezoelectric layer can be suppressed, the generation of heterogeneous phases in the interface between the piezoelectric layer and the electrode is suppressed, an electric field is easily applied, and the efficiency as a piezoelectric element is improved. the
(3)由于抑制压电体层的泄漏电流,所以可薄膜化压电体层。 (3) Since the leakage current of the piezoelectric layer is suppressed, the piezoelectric layer can be thinned. the
另外,本实施方式的液体喷射头和液体喷射装置由于使用含有上述压电体层的压电元件,所以尤其得到以下效果。 In addition, since the liquid ejection head and the liquid ejection device according to the present embodiment use the piezoelectric element including the above-mentioned piezoelectric layer, the following effects can be obtained particularly. the
(4)由于可减轻压电体层的疲劳恶化,所以可抑制压电体层的位移量的随时间变化,使可靠性提高。 (4) Since the deterioration of the fatigue of the piezoelectric layer can be reduced, the temporal change of the displacement amount of the piezoelectric layer can be suppressed and the reliability can be improved. the
以上说明本发明的最佳实施方式,但本发明不限于此,可在发明精神的范围内利用各种实施方式来实施。 The best embodiments of the present invention have been described above, but the present invention is not limited thereto and can be implemented in various embodiments within the scope of the spirit of the invention. the
例如,在强电介质膜101上,即便将Ta、W、V、Mo作为添加物质以代替Nb对PZT施加,也可具有同等的效果。另外,即便将Mn用作添加物质,也可具有与Nb一样的效果。另外,通过同样的考虑,为了防止Pb逸出,还考虑用+3价以上的元素来置换Pb,作为替补,例如有La、Ce、Pr、Nd、Pm、Sm、Eu、Gd、Tb、Dy、Ho、Er、Tm、Yb和Lu等镧系元素。另外,作为促进结晶化的添加剂,也可不用硅酸盐(Si)而使用锗酸盐(Ge)。图43A中表示对PZT使用10摩尔%的Ta来代替Nb作为添加物质时的磁滞特性。图43B中表示对PZT使用10摩尔%的W来代替Nb作为添加物质时的磁滞特性。可知在使用Ta的情况下也可以得到与添加Nb一样的效果。另外,可知在使用W的情况下,就得到绝缘性好的磁滞特性而言,具有与添加Nb一样的效果。 For example, on the
Claims (17)
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| JP2003-302900 | 2003-08-27 | ||
| JP2003302900A JP3791614B2 (en) | 2002-10-24 | 2003-08-27 | Ferroelectric film, ferroelectric memory device, piezoelectric element, semiconductor element, piezoelectric actuator, liquid ejecting head, and printer |
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| JP2015065430A (en) * | 2013-08-27 | 2015-04-09 | 三菱マテリアル株式会社 | PNbZT thin film manufacturing method |
| WO2015147259A1 (en) | 2014-03-27 | 2015-10-01 | 三菱マテリアル株式会社 | Mn-doped pzt-based piezoelectric film formation composition and mn-doped pzt-based piezoelectric film |
| US10112872B2 (en) | 2014-03-28 | 2018-10-30 | Mitsubishi Materials Corporation | Composition for forming Mn and Nb co-doped PZT-based piezoelectric film |
| JP7085208B2 (en) * | 2018-12-11 | 2022-06-16 | 国立研究開発法人産業技術総合研究所 | Piezoelectric material and MEMS device using it |
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| JP2839253B2 (en) * | 1987-12-03 | 1998-12-16 | 三菱化学株式会社 | Piezoelectric ceramic composition for actuator |
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| EP1071121A1 (en) * | 1999-07-19 | 2001-01-24 | International Business Machines Corporation | Process for the formation of a collar oxide in a trench in a semiconductor substrate |
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