• Journal of Magnetics
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• 제12권4호
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• pp.152-155
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• 2007

Spin dependent transport was investigated in lateral $Py(Ni_{81}Fe_{19})/Au/Py$ spin valve devices. Clear spin valve effect was observed in conventional four-terminal measurement geometry. Higher resistance was found in antiparallel magnetization field of two Py electrodes which is determined by anisotropy magnetoresistance (AMR) measurements. The rectangular shape of spin signal together with good agreement of switching field convinces observed spin valve signal is resulted from effective spin injection and detection. The magnetoresistance ratio decays exponentially with channel length by which spin diffusion length of Au channel was estimated to be 76 nm.

• Journal of Magnetics
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• 제14권1호
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• pp.23-26
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• 2009

Spin injection from a ferromagnet into an n-doped $In_{0.53}Ga_{0.47}As$ channel was electrically detected by a ferromagnetic detector. At T = 20 K, using non-local and local spin-valve measurements, a non-local signal of $2\;{\mu}V$ and a local spin valve signal of 0.041% were observed when the bias current was 1 mA. The band calculation and Shubnikov-de Haas oscillation measurement in a bulk channel showed that the gate controlled spin-orbit interaction was not large enough to control the spin precession but it could be a worthy candidate for a logic device using spin accumulation and diffusion.

• 한국자기학회:학술대회 개요집
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• 한국자기학회 2004년도 하계학술연구발표회 논문개요집
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• pp.44-45
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• 2004

• 한국초전도ㆍ저온공학회논문지
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• 제19권3호
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• pp.23-26
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• 2017

We have studied magnetic and transport properties of NbN/FeN/Cu/FeN/FeMn spin-valve structure. In-plane magnetic moment exhibited typical hysteresis loops of spin valves in the normal state of NbN film at 20 K. On the other hand, the magnetic hysteresis loop in the superconducting state exhibited more complex behavior in which exchange bias provided by antiferrmagnetic FeMn layer to adjacent FeN layer was disturbed by superconductivity. Because of this, the ideal superconducting spin-valve effect was not detected. Instead the stray field originated from unsaturated magnetic states dominated the transport properties of NbN/FeN/Cu/FeN/FeMn multilayer.

• 한국자기학회:학술대회 개요집
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• 한국자기학회 2003년도 하계학술연구발표회 및 한.일 공동심포지엄
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• pp.68-69
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• 2003

• 한국자기학회지
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• 제14권6호
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• pp.236-239
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• 2004

미소 자유자성층에 인접한 스핀필터층 (SFL; spin filter layer)을 갖는 Ta3/NiFe2/IrMn7/CoFe1/(NOL1)/CoFe2/Cu 1.8/CoFe( $T_{f}$)/Cu( $t_{SF}$ )/(NOL2)/Ta3.5 (두께단위 nm) 구조의 스페큘라 스핀밸브 (SSV; specular spin valve)를 마그네트론 스퍼터링 장치를 사용하여 제작하였다. 반강자성체 I $r_{22}$M $n_{78}$을 속박층으로 한 스핀필터 스페큘라 스핀밸브 (SFSSV; spin filter specular spin valve) 박막에 대하여 자유자성층의 두께 ( $t_{F}$)와 SFL의 두께 ( $t_{SF}$ )가 각각 1.5nm일 때 극대 자기저항 (MR; magnetoresistance)비 11.9%를 얻었으며, $t_{SF}$ 가 1.0nm으로 감소하여도 11%이상의 MR비를 유지하였다. 이것은 나노산화층 (NOL; nano-oxide layer)에 의한 스페큘라 전자와 SFL에 의한 전류분류효과의 증가 때문이다. 또한, 자유자성층과 피속박층 사이의 층간결합장 ( $H_{int}$; interlayer coupling field)은 RKKY력과 정자기결합력으로 설명할 수 있다. 자유자성층의 보자력 ( $H_{cf}$ ; coercivity of the free layer)은 기존의 스핀밸브 (TSV; traditional spin valve)에 비해 현저히 감소했으며, $t_{F}$가 1nm에서 4nm로 변하여도 4 Oe이하의 값을 유지하였다. 따라서 SFL의 삽입으로 자유자성층의 연자성 특성을 떨어뜨리지 않으면서 자유자성층 두께의 감소와 MR비의 향상을 가능하게 하였다.

• Journal of Magnetics
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• 제5권2호
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• pp.44-49
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• 2000

Computer simulation of sensing current effects on the magnetic and magnetoresistance properties of a crossed spin-valve head is carried out. The spin-valve head has the following layer structure: Ta (8.0 nm)/NiMn (25 nm)/NiFe (2.5 nm)/Cu (3.0 nm)/NiFe (5.5 nm)/Ta (3.0 nm), and it is 1500 nm long and 600 nm wide. Even with a high pinning field of 300 Oe and a high hard-biased field of 50 Oe, the ideal crossed spin-valve structure, which is essential to the symmetry of the output signal and hence high density recording, is not realized mainly due to large interlayer magnetostatic interactions. This problem is solved by applying a suitable magnitude of sensing currents along the length direction generating magnetic fields in the width direction. The ideal spin-valve head is expected to show good symmetry of the output signal. This has not been shown explicitly in the present simulation, however, The reason for this is possibly related to the simple assumption used in this calculation that each magnetic layer consists of a single domain.

• 한국자기학회:학술대회 개요집
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• 한국자기학회 2004년도 동계학술연구발표회 논문개요집
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• pp.70-71
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• 2004

• Journal of Magnetics
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• 제16권4호
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• pp.328-331
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• 2011

Here, we describe a dual spin valve structure with distinct switching fields for two pinned layers. A device with this structure has a staircase of three distinct magnetoresistive states. The multiple resistance states are achieved by controlling the exchange coupling between two ferromagnetic pinned layers and two adjacent anti-ferromagnetic pinning layers. The maximum magnetoresistance ratio is 7.9% for the current-perpendicular-to-plane and 7.2% for the current-in-plane geometries, with intermediate magnetoresistance ratios of 3.9% and 3.3%, respectively. The requirements for using this exchange-biased stack as a three-state memory device are also discussed.

• Journal of Magnetics
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• 제11권3호
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• pp.108-110
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• 2006

We successfully enhanced the performance of a spin valve by inserting an ultra-thin layer of partially oxidized Fe in the pinned and free layers. With the exchange bias field kept large, the spin valve reached a GMR of 12%, which corresponded to a 55% increase in GMR when we compared it with that of spin valves without any inserted layer. The layer of partially oxidized Fe was more effective for improving the properties of the spin valve than the layer of partially oxidized $Co_{90}Fe_{10}$. Considering all the results, we can contribute the significant improvement to the combined effect of the modified local electronic structures at the Fe impurities and theenhanced spin-dependent reflections at the $\alpha-Fe_{2}O_{3} phase in the magnetic layer.