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    • 11. 发明专利
    • Magnetoresistance effect element and magnetic disk device
    • 磁阻效应元件和磁盘设备
    • JP2008010509A
    • 2008-01-17
    • JP2006177100
    • 2006-06-27
    • Fujitsu Ltd富士通株式会社
    • MIYAJIMA TOYOOTSUKADA MINEHARU
    • H01L43/08G11B5/39H01L43/10H01L43/12
    • G11B5/3909B82Y10/00B82Y25/00G11B5/3163G11B5/3912G11B2005/3996Y10T29/49043
    • PROBLEM TO BE SOLVED: To provide a magnetoresistance effect element which can improve the stability of output, as well as a magnetic disk device using the same. SOLUTION: An orientation control film 3 is formed on an alumina film 2 by a sputtering method. A Ti film, a Ta film, a Ru film, or a MgO film or the like is formed as the orientation control film 3. A lower shield layer 4 is formed on the orientation control film 3. In this case, crystal grains forming the lower shield layer 4 become prismatic. When the Ti film, the Ta film or the Ru film is formed as the orientation control film 3, the surface of the lower shield layer 4 becomes a (111) plane; and when the MgO film is formed as the orientation control film 3, it becomes a (100) plane. A GMR film 5 is formed on the lower shield layer 4. When forming the GMR film 5, an anti-ferromagnetic film is epitaxially grown on the lower shield layer 4 first. At this time, the anti-ferromagnetic film is reflected by the crystal structure of the lower shield film 4, its surface also becomes a (111) plane or a (100) plane. COPYRIGHT: (C)2008,JPO&INPIT
    • 要解决的问题:提供可以提高输出稳定性的磁阻效应元件以及使用该磁阻效应元件的磁盘装置。 解决方案:通过溅射法在氧化铝膜2上形成取向控制膜3。 形成Ti膜,Ta膜,Ru膜或MgO膜等作为取向控制膜3.在取向控制膜3上形成下屏蔽层4.在这种情况下,形成 下屏蔽层4变成棱柱形。 当形成Ti膜,Ta膜或Ru膜作为取向控制膜3时,下屏蔽层4的表面成为(111)面; 并且当形成作为取向控制膜3的MgO膜时,成为(100)面。 在下屏蔽层4上形成有GMR膜5.当形成GMR膜5时,首先在下屏蔽层4上外延生长反铁磁性膜。 此时,反铁磁膜被下屏蔽膜4的晶体结构反射,其表面也成为(111)面或(100)面。 版权所有(C)2008,JPO&INPIT
    • 13. 发明专利
    • Compound semiconductor device and manufacturing method of the same
    • 化合物半导体器件及其制造方法
    • JP2014090033A
    • 2014-05-15
    • JP2012238334
    • 2012-10-29
    • Fujitsu Ltd富士通株式会社
    • MIYAJIMA TOYOOISHIGURO TETSUROYAMADA ATSUSHIIMANISHI KENJI
    • H01L27/098H01L21/337H01L29/808H02M3/28H02M7/12
    • Y02B70/1483
    • PROBLEM TO BE SOLVED: To achieve a highly reliable compound semiconductor device which achieves successful normally-off without causing problems such as increase in electrical resistance and an unstable operation, which are caused by dry etching of a p-type semiconductor layer though the p-type semiconductor layer is used for controlling 2DEG.SOLUTION: An AlGaN/GaN HEMT comprises: a compound semiconductor lamination structure 2; a gate electrode 7 formed above the compound semiconductor lamination structure 2; and a p-type semiconductor layer 3a locally formed between the compound semiconductor lamination structure 2 and the gate electrode 7. The compound semiconductor lamination structure 2 has flatness to an atomic step level on a surface in an unformed surface where the p-type semiconductor layer 3a is not formed.
    • 要解决的问题:为了实现一种高可靠性的化合物半导体器件,其通过p型半导体层的干法蚀刻引起的常规关闭,而不会引起诸如电阻增加和不稳定操作的问题, 类型半导体层用于控制2DEG。解决方案:AlGaN / GaN HEMT包括:化合物半导体层叠结构2; 形成在化合物半导体层叠结构体2上方的栅电极7; 以及局部地形成在化合物半导体层叠结构体2和栅电极7之间的p型半导体层3a。化合物半导体层叠结构体2在未形成表面的表面上具有与原子台阶水平的平坦度,其中p型半导体层 3a不形成。
    • 17. 发明专利
    • Electron beam device and its adjustment method
    • 电子束装置及其调整方法
    • JP2010086882A
    • 2010-04-15
    • JP2008256808
    • 2008-10-01
    • Fujitsu Ltd富士通株式会社
    • MIYAJIMA TOYOOHONDA KOICHIRO
    • H01J37/295
    • PROBLEM TO BE SOLVED: To automatically form an interference pattern of an electron beam having an optimal clear condition without depending on a human operation, and to perform a phase measurement at a stable condition by an electron beam holography method.
      SOLUTION: A control section 25 changes an astigmatism correction current value applied to an astigmatism correction lens 13, contrast is calculated from the interference pattern of the electron beam at an electron beam hologram image obtained by an image acquisition section 25, an interrelationship between the astigmatism correction current value and the contrast of the interference patterns is calculated, and the astigmatism correction current value is determined so as to maximize the contrast.
      COPYRIGHT: (C)2010,JPO&INPIT
    • 要解决的问题:为了在不依赖于人体操作的情况下自动形成具有最佳清除条件的电子束的干涉图案,并且通过电子束全息术在稳定状态下进行相位测量。 解决方案:控制部分25改变应用于像散校正透镜13的像散校正电流值,根据由图像获取部分25获得的电子束全息图图像处的电子束的干涉图案计算对比度,相互关系 计算像散校正电流值和干涉图案的对比度之间的像差,并且确定像散校正电流值以使对比度最大化。 版权所有(C)2010,JPO&INPIT
    • 18. 发明专利
    • Electron beam tomography method, and electron beam tomography device
    • 电子束测量方法和电子束成像装置
    • JP2009152120A
    • 2009-07-09
    • JP2007330320
    • 2007-12-21
    • Fujitsu Ltd富士通株式会社
    • MIYAJIMA TOYOOITO RYOJI
    • H01J37/26H01J37/22H01J37/28
    • PROBLEM TO BE SOLVED: To provide an electron beam tomography method capable of obtaining a three-dimensionally reconstituted image of high precision by improving precision of information related to a projection direction of a sample, and to provide an electron beam tomography apparatus. SOLUTION: A transmission electron image is obtained by radiating the electron beam to an evaluation site of the sample having the evaluation site where the structure is to be evaluated, and a single crystal site integrally joined with the evaluation site, and the electron beam diffraction image is obtained by radiating the electron beam to the single crystal site without changing a radiation angle of the electron beam. The operation is carried out by a plurality of angles, a series of transmission electron images and the electron beam diffraction images are obtained, and based on the electron beam diffraction image, the projection direction for each of the series of the transmission electron images is decided. Based on the projection direction obtained by the method, positioning of the series of the transmission electron is carried out, and reconstituting calculation of a three-dimensional structure of the evaluation site is carried out. COPYRIGHT: (C)2009,JPO&INPIT
    • 解决问题:提供能够通过提高与样品的投影方向相关的信息的精度来获得高精度的三维重构图像的电子束断层摄影方法,并提供电子束断层摄影装置。 解决方案:通过将电子束照射到具有评价结构的评价部位的样品的评价部位和与评价部位一体接合的单晶部位而获得透射电子图像, 通过在不改变电子束的辐射角的情况下将电子束照射到单晶位置来获得光束衍射图像。 通过多个角度进行操作,获得一系列透射电子图像和电子束衍射图像,并且基于电子束衍射图像,确定一系列透射电子图像的投影方向 。 基于通过该方法获得的投影方向,进行一系列透射电子的定位,并且重新计算评价部位的三维结构。 版权所有(C)2009,JPO&INPIT
    • 19. 发明专利
    • Element evaluation method and apparatus
    • 元素评估方法和设备
    • JP2009052944A
    • 2009-03-12
    • JP2007218142
    • 2007-08-24
    • Fujitsu Ltd富士通株式会社
    • MIYAJIMA TOYOOODAKA YASUTOSHI
    • G01N23/04G01B15/02
    • G01B15/025
    • PROBLEM TO BE SOLVED: To provide an element evaluation method, constituted so as to evaluate the element shape of the lead element of a magnetic head, which enables the evaluation of lead width, core width and element height by the same evaluation sample, and an element evaluation apparatus.
      SOLUTION: An electron beam enters a first region where a first part comprising a first material overlies a second part comprising a second material to measure the intensity of the first electron beam showing the contrast depending on the atomic masses of the constituent elements of the first and second materials while an electron beam enters a second region comprising the first material to measure the intensity of the second electron beam showing the contrast depending on the atomic mass of the constituent element of the first material and an electron beam enters a third region comprising the second material to measure the intensity of the third electron beam showing the contrast depending on the atomic mass of the constituent element of the second material. The relationship between the intensity of the first electron beam and the thickness of the first part is calculated from the relationship between the intensity of the second electron beam and the thickness of an evaluated sample and the relationship between the intensity of the third electron beam and the thickness of the evaluated sample to calculate the thickness of the first part of the first region.
      COPYRIGHT: (C)2009,JPO&INPIT
    • 要解决的问题:提供一种元件评估方法,其构成为评估磁头的引线元件的元件形状,其能够通过相同的评估样本来评估引线宽度,芯宽度和元件高度 ,以及元件评价装置。 解决方案:电子束进入第一区域,其中包含第一材料的第一部分覆盖包括第二材料的第二部分,以测量显示对比度的第一电子束的强度,这取决于组成元素的原子质量 第一和第二材料,而电子束进入包含第一材料的第二区域,以测量根据第一材料的构成元素的原子质量显示对比度的第二电子束的强度,并且电子束进入第三区域 包括第二材料,以测量根据第二材料的构成元素的原子质量显示对比度的第三电子束的强度。 第一电子束的强度与第一部分的厚度之间的关系由第二电子束的强度与评价样品的厚度之间的关系以及第三电子束的强度与第 评估样品的厚度,以计算第一区域的第一部分的厚度。 版权所有(C)2009,JPO&INPIT