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    • 22. 发明授权
    • Memory element and memory device
    • 存储器元件和存储器件
    • US07196386B2
    • 2007-03-27
    • US10530006
    • 2003-10-02
    • Koji KadonoMasafumi Ata
    • Koji KadonoMasafumi Ata
    • H01L29/82
    • G11C11/16B82Y10/00B82Y30/00G11C13/025H01L27/222H01L43/08
    • A memory element wherein a spin conduction layer having a sufficient spin coherence length and a uniform spin field can be obtained, and thereby practical use is attained and a memory device are provided. A spin conduction layer (paramagnetic layer) (24) is a fullerene thin film being from 0.5 nm to 5 μm thick, for example. The fullerene has a hollow sized, for example, from 0.1 nm to 50 nm. A paramagnetic material is included in this hollow. A fermi vector of the fullerene thin film well laps over small number of spin band or plenty of spin band of a ferromagnetic fixed layer (23) and a ferromagnetic free layer (25). Further, spin orientations of the included paramagnetic material are random. Further, electron spin in the fullerene is in a quantized state in a pseudo zero dimensional space. Thereby, a spin coherence length becomes long in the fullerene thin film, and scatteration of spin-polarized conduction electrons goes away.
    • 可以获得具有足够的自旋相干长度和均匀自旋场的自旋导电层的存储元件,从而实现实用性并提供存储器件。 例如,自旋导电层(顺磁性层)(24)是0.5nm〜5μm厚的富勒烯薄膜。 富勒烯具有例如0.1nm至50nm的中空尺寸。 这个空心包含顺磁材料。 富勒烯薄膜阱的费米子向量在铁磁固定层(23)和铁磁自由层(25)的少量自旋带或大量自旋带上交叉。 此外,所包含的顺磁材料的自旋取向是随机的。 此外,富勒烯中的电子自旋在伪零维空间中处于量化状态。 因此,富勒烯薄膜中的自旋相干长度变长,自旋极化导电电子的散射消失。
    • 23. 发明申请
    • Memory element and memory device
    • 存储器元件和存储器件
    • US20060006334A1
    • 2006-01-12
    • US10530006
    • 2003-10-02
    • Koji KadonoMasafumi Ata
    • Koji KadonoMasafumi Ata
    • H01L37/00
    • G11C11/16B82Y10/00B82Y30/00G11C13/025H01L27/222H01L43/08
    • A memory element wherein a spin conduction layer having a sufficient spin coherence length and a uniform spin field can be obtained, and thereby practical use is attained and a memory device are provided. A spin conduction layer (paramagnetic layer) (24) is a fullerene thin film being from 0.5 nm to 5 μm thick, for example. The fullerene has a hollow sized, for example, from 0.1 nm to 50 nm. A paramagnetic material is included in this hollow. A fermi vector of the fullerene thin film well laps over small number of spin band or plenty of spin band of a ferromagnetic fixed layer (23) and a ferromagnetic free layer (25). Further, spin orientations of the included paramagnetic material are random. Further, electron spin in the fullerene is in a quantized state in a pseudo zero dimensional space. Thereby, a spin coherence length becomes long in the fullerene thin film, and scatteration of spin-polarized conduction electrons goes away.
    • 可以获得具有足够的自旋相干长度和均匀自旋场的自旋导电层的存储元件,从而实现实用性并提供存储器件。 例如,自旋导电层(顺磁性层)(24)是0.5nm〜5μm厚的富勒烯薄膜。 富勒烯具有例如0.1nm至50nm的中空尺寸。 这个空心包含顺磁材料。 富勒烯薄膜阱的费米子向量在铁磁固定层(23)和铁磁自由层(25)的少量自旋带或大量自旋带上交叉。 此外,所包含的顺磁材料的自旋取向是随机的。 此外,富勒烯中的电子自旋在伪零维空间中处于量化状态。 因此,富勒烯薄膜中的自旋相干长度变长,自旋极化导电电子的散射消失。