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Volumn 64, Issue 6, 2001, Pages

Angular dependence of the tunnel magnetoresistance in transition-metal-based junctions

Author keywords

[No Author keywords available]

Indexed keywords

METAL;

EID: 0035421547     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.64.064427     Document Type: Article
Times cited : (70)

References (37)
  • 3
    • 85038289672 scopus 로고    scopus 로고
    • Throughout this paper, we have defined the so-called TMR by the maximum difference of the conductivity (formula presented) normalized by its averaged value (formula presented) (formula presented)
    • Throughout this paper, we have defined the so-called TMR by the maximum difference of the conductivity (formula presented) normalized by its averaged value (formula presented) (formula presented).
  • 8
    • 85038306500 scopus 로고    scopus 로고
    • (unpublished)
    • D. Lacour(unpublished).
    • Lacour, D.1
  • 18
    • 85038345013 scopus 로고    scopus 로고
    • The resistance is generally assumed to vary like (formula presented) where (formula presented) is the resistance measured in the perpendicular magnetic configuration
    • The resistance is generally assumed to vary like (formula presented) where (formula presented) is the resistance measured in the perpendicular magnetic configuration.
  • 21
    • 0030261301 scopus 로고    scopus 로고
    • The analogy with magneto-optics is obvious. The differential Kerr effect, which is turned into account to detect a slight change of the magnetization vector [see, for example, can be viewed, inversely, as an elegant method to modulate the light intensity by acting on the magnetization orientation
    • The analogy with magneto-optics is obvious. The differential Kerr effect, which is turned into account to detect a slight change of the magnetization vector [see, for example, K. Postava, J. Magn. Magn. Mater.163, 8 (1996)] can be viewed, inversely, as an elegant method to modulate the light intensity by acting on the magnetization orientation.
    • (1996) J. Magn. Magn. Mater. , vol.163 , pp. 8
    • Postava, K.1
  • 29
    • 0033514208 scopus 로고    scopus 로고
    • See, for example, the review article, and
    • See, for example, the review article J. Nogués and I. Schuller, J. Magn. Magn. Mater.192, 203 (1998).
    • (1998) J. Magn. Magn. Mater. , vol.192 , pp. 203
    • Nogués, J.1    Schuller, I.2
  • 31
    • 85038270685 scopus 로고    scopus 로고
    • At 30 K, we have measured on CoO a unidirectional exchange bias (formula presented) and uniaxial exchange anisotropy (formula presented) respectively, equal to 250 and 800 Oe whereas its Néel temperature was estimated at about 180 K
    • At 30 K, we have measured on CoO a unidirectional exchange bias (formula presented) and uniaxial exchange anisotropy (formula presented) respectively, equal to 250 and 800 Oe whereas its Néel temperature was estimated at about 180 K.
  • 35
    • 85038292644 scopus 로고    scopus 로고
    • This expression is rigorous at the order considered and can be derived by differentiating the energy derivative of the magnetization in the vicinity of the equilibrium state (formula presented) corresponding to (formula presented) and given by (formula presented). At the upper order, the angle modulation (formula presented) is calculated to be (formula presented), which does not introduce any relevant corrections
    • This expression is rigorous at the order considered and can be derived by differentiating the energy derivative of the magnetization in the vicinity of the equilibrium state (formula presented) corresponding to (formula presented) and given by (formula presented). At the upper order, the angle modulation (formula presented) is calculated to be (formula presented), which does not introduce any relevant corrections.
  • 36
    • 85038337559 scopus 로고    scopus 로고
    • Expressions of (formula presented) can be put into a general form as (formula presented) where (formula presented) is a small phase equaling (formula presented) (0) in the case of a linear response of the conductivity (resistance) vs (formula presented)
    • Expressions of (formula presented) can be put into a general form as (formula presented) where (formula presented) is a small phase equaling (formula presented) (0) in the case of a linear response of the conductivity (resistance) vs (formula presented).
  • 37
    • 85038305358 scopus 로고    scopus 로고
    • This integral is not straightforward to calculate. However, it approaches (formula presented) or (formula presented), which can be easily developed in order of
    • This integral is not straightforward to calculate. However, it approaches (formula presented) or (formula presented), which can be easily developed in order of h.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.