SCOPUS 정보 검색 플랫폼

17
- 0022009994
- Deducing 3d spin polarization from 3s XPS in ultrathin metal films grown by molecular beam epitaxy
- (1986) Journal of Magnetism and Magnetic Materials , vol.54-57 , pp. 1025
- Arrott, A.S.¹ Heinrich, B.² Liu, C.³ Purcell, S.T.⁴

18
- 84926269518
- B. Heinrich, A. S. Arrott, J. F. Cochran, C. Liu, and K. Myrtle, Proceedings of the 32nd National Vacuum Symposium of the American Vacuum Society, 1985, Houston, Texas
- (1986) J. Vac. Sci. Technol. A , vol.4 , pp. 1376

23
- 36149012617
- . For a specific application of the Ament-Rado formalism to multilayer problems see: (a), 15, 5141, G. Spronken, A. Friedmann, A. Yelon, Phys. Rev. B
- (1955) Phys. Rev. , vol.97 , pp. 1558
- Ament, W.S.¹ Rado, G.T.²

26
- 0012083869
- For the connection between Landau-Lifshitz damping and Gilbert damping, see, e.g.,
- (1985) J. Appl. Phys. , vol.57 , pp. 3709
- Heinrich, B.¹ Arrott, A.S.²

29
- 0004256792
- Interscience, New York
- (1963) Micromagnetics , pp. 35
- Brown, W.F.¹

30
- 0018544980
- For a critical review of surface structures see
- (1979) J. Vac. Sci. Technol. , vol.18 , pp. 2073
- Biberian, J.P.¹ Somorjai, G.A.²

31
- 0000987417
- (1985) J. Phys. Chem. Solids , vol.4 , pp. 241
- Dzialoshinski, I.¹

34
- 1542436798
- (1972) Phys. Lett. , vol.40 A , pp. 29
- Martinova, L.¹ Frait, Z.²

35
- 0345732710
- (1975) Fiz. Tverd. Tela , vol.17 , pp. 2731
- Kaganov, M.I.¹ Paasch, G.²

38
- 4043181736
- Ferromagnetic resonance and surface anisotropy in iron single crystals
- (1980) Journal of Magnetism and Magnetic Materials , vol.15-18 , pp. 1081
- Frait, Z.¹ Fraitova, D.²

41
- 0004134845
- Wiley, New York
- (1964) The Physics of Magnetism , pp. 168-171
- Chikazumi, S.¹

42
- 84926267748
- The effect of a strain, e, homogeneous in the plane, but one which assumes a contraction normal to the plane in order to preserve volume, can be estimated using the magnetoelastic interaction energy described by Chikazumi (Ref. 26). For the case of a cubic metal having its cube axes parallel with the coordinate axes, and having the equilibrium magnetization along the x direction, this energy has the form E=E0 -3B1 e α32. This energy density produces an effective torque per unit area given by -6B1 e^d α3. According to Eq. (8) this torque would be produced by an effective pinning anisotropy Kz =-3B1 ed. For nickel B1 =6.2 times 107 erg/cm3_, so that for e=10-2 and d=50 Å, one would obtain Kz =-0.93 erg/cm2_. The negative sign means that the effective surface torque produced by an expansion of the lattice in the plane of the film would act so as to drive the magnetization out of the surface plane.

43
- 84926265342
- In calculating the nickel resonance field from Eq. (27), it must be remembered that a bulk magnetocrystalline anisotropy has been assumed which shifts the resonance by 2K1 /MA =-1.637 kOe.

* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.