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    • 5. 发明授权
    • MRAM with super-paramagnetic sensing layer
    • MRAM具有超顺磁感应层
    • US07696548B2
    • 2010-04-13
    • US11200380
    • 2005-08-09
    • Po-Kang WangYimin GuoCheng HorngTai MinRu-Ying Tong
    • Po-Kang WangYimin GuoCheng HorngTai MinRu-Ying Tong
    • H01L29/94
    • H01L43/08
    • An MRAM is disclosed that has a MTJ comprised of a ferromagnetic layer with a magnetization direction along a first axis, a super-paramagnetic (SP) free layer, and an insulating layer formed therebetween. The SP free layer has a remnant magnetization that is substantially zero in the absence of an external field, and in which magnetization is roughly proportional to an external field until reaching a saturation value. In one embodiment, a separate storage layer is formed above, below, or adjacent to the MTJ and has uniaxial anisotropy with a magnetization direction along its easy axis which parallels the first axis. In a second embodiment, the storage layer is formed on a non-magnetic conducting spacer layer within the MTJ and is patterned simultaneously with the MTJ. The SP free layer may be multiple layers or laminated layers of CoFeB. The storage layer may have a SyAP configuration and a laminated structure.
    • 公开了一种MRAM,其具有由沿第一轴的磁化方向的铁磁层,超顺磁性(SP)自由层和在它们之间形成的绝缘层构成的MTJ。 SP自由层具有在没有外部场的情况下基本为零的残余磁化,并且其中磁化大致与外部场成正比,直到达到饱和值。 在一个实施例中,单独的存储层形成在MTJ的上方,下方或附近,并且具有沿其易于轴线平行于第一轴线的磁化方向的单轴各向异性。 在第二实施例中,存储层形成在MTJ内的非磁性导电间隔层上,并与MTJ同时构图。 SP自由层可以是CoFeB的多层或层压层。 存储层可以具有SyAP配置和层压结构。
    • 8. 发明申请
    • MRAM with means of controlling magnetic anisotropy
    • MRAM具有控制磁各向异性的方法
    • US20090096043A1
    • 2009-04-16
    • US11973751
    • 2007-10-10
    • Tai MinPo Kang Wang
    • Tai MinPo Kang Wang
    • H01L43/08H01L43/12
    • H01L43/08G11C11/1675H01L43/12
    • We describe the manufacturing process for and structure of a CPP MTJ MRAM unit cell that utilizes transfer of spin angular momentum as a mechanism for changing the magnetic moment direction of a free layer. The strength of the switching field, Hs of the cell is controlled by the magnetic anisotropy of the cell which, in turn, is controlled by a combination of the shape anisotropy and the stress and magnetostriction of the cell free layer. The coefficient of magnetostriction of the free layer can be adjusted by methods such as adding Nb or Hf to alloys of Ni, Fe, Co and B or by forming the free layer as a lamination of layers having different values of their coefficients of magnetostriction. Thus, by tuning the coefficient of magnetostriction of the cell free layer it is possible to produce a switching field of sufficient magnitude to render the cell thermally stable while maintaining a desirable switching current.
    • 我们描述了使用自旋角动量转移作为改变自由层的磁矩方向的机制的CPP MTJ MRAM单元的制造过程和结构。 开关场的强度,电池的Hs由电池的磁各向异性控制,电池的磁各向异性又由形状各向异性和无电解层的应力和磁致伸缩的组合控制。 自由层的磁致伸缩系数可以通过添加Nb,Hf等Ni,Fe,Co,B的合金的方法来进行,也可以通过形成自由层作为其磁致伸缩系数不同的层的叠层来进行。 因此,通过调谐无电解层的磁致伸缩系数,可以产生足够大的开关场,使电池热稳定,同时保持理想的开关电流。