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    • 42. 发明授权
    • Magnetic bubble memory chip
    • 磁性气泡存储芯片
    • US4568618A
    • 1986-02-04
    • US659879
    • 1984-10-15
    • Hidema UchishibaSeiichi IwasaKazuyuki Yamaguchi
    • Hidema UchishibaSeiichi IwasaKazuyuki Yamaguchi
    • G11C11/14G11C19/08H01F10/24G11B5/64
    • H01F10/24G11C19/085Y10S428/90Y10S428/91
    • In order for the temperature dependence of the strip out field of a magnetic garnet crystal film (54) to match the temperature dependence of the residual magnetization of a permanent magnet (56) for applying a bias magnetic field in a magnetic bubble memory chip (2) after conductor paterns are formed thereon, it is necessary that the temperature coefficient of the collapse field of the magnetic garnet crystal film (51) be from 0.01 to 0.04%/.degree.C., in terms of an absolute value, greater than the temperature coefficient of the above-mentioned residual magnetization (56). The present invention achieves this by increasing the degree of substitution of Lu ions for Fe ions in the octahedral sites constituting the unit lattice of the magnetic garnet crystal. As a result, an operating temperature range about twice as wide as the conventional operating temperature range is ensured.
    • 为了使磁性石榴石晶体膜(54)的剥离场的温度依赖性与用于在气泡存储芯片(2)中施加偏置磁场的永磁体(56)的剩余磁化的温度依赖性相匹配 )之后,在其上形成导电体之后,必须使磁性石榴石晶体膜(51)的塌陷场的温度系数为0.01〜0.04%/℃,绝对值大于温度 上述剩余磁化强度的系数(56)。 本发明通过增加构成磁性石榴石晶体的单位晶格的八面体位置中的Lu离子对Fe离子的取代度来实现。 因此,确保了与现有的工作温度范围相当的两倍宽的工作温度范围。