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    • 7. 发明授权
    • Method for forming an image on a magnetic composite medium and apparatus
therefor
    • 在磁性复合介质上形成图像的方法及其装置
    • US5324603A
    • 1994-06-28
    • US870524
    • 1992-04-17
    • Sungho JinThomas H. Tiefel
    • Sungho JinThomas H. Tiefel
    • G03G19/00B43L1/00
    • B43L1/008
    • In accordance with the invention, an image is formed by applying a local magnetic field to selected regions of a magnetic composite medium comprising columns of magnetic particles distributed in a matrix medium. The particles are "hard" or "semi-hard" magnetic materials in order to retain the latent image as residual magnetism, and the image is developed by exposure to magnetic fluid or powders. The image can be erased by exposure to an AC demagnetizing field or a DC sweep magnet. Preferred apparatus for making such images comprises a sheet of such composite material having a pair of major surfaces with columns of magnetic particles oriented between the surfaces. A local magnetic field, such as a magnetic pen, can be used to write a latent magnetic image on one of the major surfaces. The magnetic columns present the latent image for development at either major surface. In preferred apparatus, one major surface is adapted for magnetic image writing and the other major surface is positioned in sealed relationship with a chamber for exposing the image to magnetic development material. In this arrangement the columns provide a high resolution image on the second surface despite the thickness of the medium between the write and development surfaces.
    • 根据本发明,通过将局部磁场施加到包括分布在矩阵介质中的磁性颗粒列的磁性复合介质的选定区域来形成图像。 颗粒是“硬”或“半硬”磁性材料,以便将潜像保留为剩余磁性,并且通过暴露于磁性流体或粉末来显影图像。 可以通过暴露于AC去磁场或DC扫描磁体来擦除图像。 用于制造这种图像的优选装置包括这种复合材料的片材,其具有一对主表面和磁性颗粒列之间的表面。 可以使用诸如磁笔的局部磁场将潜在磁图像写在主表面之一上。 磁性柱呈现在两个主表面的潜像用于显影。 在优选的装置中,一个主表面适用于磁图像书写,另一个主表面与用于将图像曝露于磁性显影材料的室密封关系。 在这种布置中,尽管在写入和显影表面之间的介质的厚度,列在第二表面上提供高分辨率图像。
    • 10. 发明授权
    • Method of making high T.sub.c superconductor material, and article
produced by the method
    • 制造高Tc超导体材料的方法,以及通过该方法制备的制品
    • US5244868A
    • 1993-09-14
    • US780555
    • 1991-10-15
    • Sungho JinShohei NakaharaThomas H. Tiefel
    • Sungho JinShohei NakaharaThomas H. Tiefel
    • C04B35/45H01L39/14H01L39/24
    • C04B35/4508H01L39/143H01L39/2477Y10S505/725Y10S505/78
    • The disclosed method can produce high T.sub.c superconductor material e.g., YBa.sub.2 Cu.sub.3 O.sub.7) of substantially increased intra-grain critical current density (J'.sub.c), as compared to conventionally produced bulk material of analogous composition. Exemplarily, YBa.sub.2 Cu.sub.3 O.sub.7 pellets produced according to the invention had J'.sub.c of about 10.sup.5 A/cm.sup.2 at 77 K. in an applied magnetic field of 0.9 Telsa. The inventive method comprises providing a precursor material whose composition differs from that of the desired superconductor with respect to at least one of the metal constituents of the desired superconductor. It further comprises heating the precursor material above the decomposition temperature (T.sub.d) of the precursor material such that a multiphase material results. The multiphase material comprises, in addition to a majority first phase, a dispersed precipitate phase. The method further comprises cooling the multiphase material to a temperature below T.sub.d at a rate such that at least a major portion of the precipitate phase is retained. The first phase differs from the desired superconductor at most with regard to oxygen content, and the heat treatment of the multiphase material is carried out such that the desired superconductor results. Exemplarily, the desired superconductor is YBa.sub.2 Cu.sub.3 O.sub.7, the precursor material has average composition YBa.sub.2 Cu.sub.4 O.sub.z (z.about.8), the precipitate phase comprises one or more copper oxides, T.sub.d is about 860.degree. C., and the multiphase material is produced at 920.degree. C.
    • 与常规制备的类似组合物的本体材料相比,所公开的方法可以产生显着增加的晶粒内临界电流密度(J'c)的高Tc超导体材料,例如YBa2Cu3O7)。 示例性地,根据本发明制备的YBa2Cu3O7颗粒在0.9Telsa的施加磁场中在77K下具有约105A / cm 2的J'c。 本发明的方法包括提供与期望的超导体的至少一种金属组分的组成不同于所需超导体的组成的前体材料。 其还包括将前体材料加热到高于前体材料的分解温度(Td),从而得到多相材料。 多相材料除了大多数第一相之外还包含分散的沉淀相。 该方法还包括以使得至少大部分沉淀相被保留的速率将多相材料冷却至低于Td的温度。 第一阶段相对于氧含量最多不同于期望的超导体,并且进行多相材料的热处理,使得期望的超导体结果。 示例性地,期望的超导体是YBa2Cu3O7,前体材料具有平均组成YBa2Cu4Oz(z DIFFERENCE 8),沉淀相包含一种或多种氧化铜,Td约为860℃,多相材料在920℃下生产。