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    • 41. 发明授权
    • Synthetic free layer for CPP GMR
    • CPP GMR的合成自由层
    • US07130168B2
    • 2006-10-31
    • US11229155
    • 2005-09-16
    • Min LiSimon LiaoKochan Ju
    • Min LiSimon LiaoKochan Ju
    • G11B5/33
    • B82Y25/00B82Y10/00B82Y40/00G11B5/3903G11B2005/3996H01F10/324H01F10/3272H01F41/302H01L43/10
    • Reduction of the free layer thickness in GMR devices is desirable in order to meet higher signal requirements, besides improving the GMR ratio itself. However, thinning of the free layer reduces the GMR ratio and leads to poor thermal stability. This problem has been overcome by making AP2 from an inverse GMR material and by changing the free layer from a single uniform layer to a ferromagnetic layer AFM (antiferromagnetically) coupled to a layer of inverse GMR material. Examples of alloys that may be used for the inverse GMR materials include FeCr, NiFeCr, NiCr, CoCr, CoFeCr, and CoFeV. Additionally, the ruthenium layer normally used to effect antiferromagnetic coupling can be replaced by a layer of chromium. A process to manufacture the structure is also described.
    • 为了满足更高的信号要求,除了改善GMR比率本身外,希望降低GMR器件中的自由层厚度。 然而,自由层的减薄降低了GMR比并导致差的热稳定性。 通过从反GMR材料制备AP 2并通过将自由层从单个均匀层改变为耦合到反向GMR材料层的铁磁层AFM(反铁磁性)而已经克服了该问题。 可用于逆GMR材料的合金的实例包括FeCr,NiFeCr,NiCr,CoCr,CoFeCr和CoFeV。 此外,通常用于实现反铁磁耦合的钌层可以被铬层代替。 还描述了制造该结构的方法。
    • 46. 发明授权
    • GMR configuration with enhanced spin filtering
    • GMR配置与增强的自旋过滤
    • US06770382B1
    • 2004-08-03
    • US09443447
    • 1999-11-22
    • Jei-Wei ChangBernard DienyMao-Min ChenCheng HorngKochan JuSimon Liao
    • Jei-Wei ChangBernard DienyMao-Min ChenCheng HorngKochan JuSimon Liao
    • G11B5127
    • H01F10/30B82Y10/00B82Y25/00G01R33/093G11B5/3133G11B5/3903G11B5/3909H01F10/3272H01L43/08Y10T428/1121Y10T428/1129Y10T428/1157Y10T428/1171Y10T428/12944Y10T428/2495
    • A Spin Valve GMR and Spin Filter SVGMR configuration where in the first embodiment an important buffer layer is composed of an metal oxide having a crystal lattice constant that is close the 1st FM free layer's crystal lattice constant and has the same crystal structure (e.g., FCC, BCC, etc.). The metal oxide buffer layer enhances the specular scattering. The spin valve giant magnetoresistance (SVGMR) sensor comprises: a seed layer over the substrate. An important metal oxide buffer layer (buffer layer) over the seed layer. The metal oxide layer preferably is comprised of NiO or alpha-Fe2O3. A free ferromagnetic layer over the metal oxide layer. A non-magnetic conductor spacer layer over the free ferromagnetic layer. A pinned ferromagnetic layer (2nd FM pinned) over the non-magnetic conductor spacer layer and a pinning material layer over the pinned ferromagnetic layer. In the second embodiment, a high conductivity layer (HCL) is formed over the buffer layer to create a spin filter -SVGMR. The HCL layer enhances the GMR ratio of the spin filter SVGMR. The third embodiment is a pinned FM layer comprised of a three layer structure of an lower AP layer, a spacer layer (e.g., Ru) and an upper AP layer.
    • 自旋阀GMR和自旋滤波器SVGMR配置,其中在第一实施例中,重要的缓冲层由具有接近第1个FM自由层的晶格常数的晶格常数的金属氧化物组成并且具有相同的晶体结构 例如FCC,BCC等)。 金属氧化物缓冲层增强了镜面散射。 自旋阀巨磁阻(SVGMR)传感器包括:衬底上的种子层。 种子层上重要的金属氧化物缓冲层(缓冲层)。 金属氧化物层优选由NiO或α-Fe2O3组成。 在金属氧化物层上的自由铁磁层。 在自由铁磁层上的非磁性导体间隔层。 在非磁性导体间隔层上方的钉扎铁磁层(第二个FM被钉住)和钉扎铁磁层上的钉扎材料层。 在第二实施例中,在缓冲层上形成高电导率层(HCL)以产生自旋滤波器-SVGMR。 HCL层增强了旋转过滤器SVGMR的GMR比。 第三实施例是由下AP层,间隔层(例如Ru)和上AP层组成的三层结构的钉扎FM层。
    • 47. 发明授权
    • CPP and MTJ reader design with continuous exchange-coupled free layer
    • CPP和MTJ读卡器设计,具有连续的交换耦合自由层
    • US07201947B2
    • 2007-04-10
    • US10238269
    • 2002-09-10
    • Simon LiaoKochan JuYoufeng Zheng
    • Simon LiaoKochan JuYoufeng Zheng
    • B29C35/08
    • B82Y25/00B82Y10/00G11B5/3116G11B5/313G11B5/3163G11B5/3903G11B5/3909G11B2005/3996Y10T29/49046
    • As track widths of magnetic read heads grow very small, conventional longitudinal bias stabilization has been found to no longer be suitable since the strong magnetostatic coupling at the track edges also pins the magnetization of the free layer. This problem has been overcome by extending the free layer so that it is no longer confined to the area immediately below the spacer or tunneling layer. A longitudinal bias layer immediately below the free layer is given a relatively weak magnetic exchange coupling field of about 200 Oe. Although there is strong exchange coupling between this and the free layer, the degree of pinning of the free layer is low so that the device's output signal is reduced by less than about 10%. A process for manufacturing both the CPP SV and a MTJ versions of the invention is described.
    • 随着磁读头的轨道宽度增长非常小,传统的纵向偏置稳定性已经被发现不再适用,因为轨道边缘处的强静磁耦合也引导自由层的磁化。 已经通过延伸自由层来克服这个问题,使得它不再局限于间隔物或隧道层正下方的区域。 在自由层正下方的纵向偏置层被给予约200Oe的相对较弱的磁交换耦合场。 尽管在这种自由层之间存在很强的交换耦合,但是自由层的钉扎程度很低,因此器件的输出信号减少了约10%。 描述了用于制造本发明的CPP SV和MTJ版本的方法。