SCOPUS 정보 검색 플랫폼

8
- 33645129168
- Relationship between Kerr effect and perpendicular magnetic anisotropy in Co1−xPtx and Co1−xPdx alloys
- (1993) Journal of Magnetism and Magnetic Materials , vol.121 , pp. 461
- Weller, D.¹ Brändle, H.² Chappert, C.³

9
- 0000429864
- (1973) Phys. Rev. B , vol.8 , pp. 1239
- Erskine, J.L.¹ Stern, E.A.²

11
- 84931522387
- Appl. Phys. Lett. (to be published).
- Lairson, B.¹ Clemens, B.²

13
- 0003689862
- American Society for Metals, Metals Park, OH, Vol. 2.
- (1990) Binary Alloy Phase Diagrams
- Massalski, T.¹

15
- 0020907388
- (1983) Mater. Res. Soc. Symp. Proc. , vol.19 , pp. 175
- Inden, G.¹

18
- 84990678048
- Diffraction effects from h.c.p. crystals with random growth faults undergoing transformation to the f.c.c. phase by the deformation mechanism
- (1987) Physica Status Solidi (a) , vol.101 , pp. 329
- Sebastian, M.T.¹ Krishna, P.²

19
- 84931522390
- Strictly, this model applies to the hcp to fcc transition of a chemically homogeneous sample. However, the model provides a reasonable approximation to the scattering along (10q z) of alloy films with nearly random in plane chemical order. Similar fcc fractions are obtained through comparison of the fcc and hcp peak integrated areas.

21
- 84931522389
- These measurements were performed at beam line x20c of the National Synchrotron Light Source, Brookhaven, New York.

22
- 84931522388
- edited by, R.W. Cahn, P. Haasen, North Holland, New York
- (1984) Physical Metallurgy , pp. 1031 1074
- Wayman, C.M.¹

23
- 84931522394
- At very low deposition temperatures the kinetics limit even MBE growth as evidenced by the fcc inclusions and the absence of chemical ordering in the 450 K film.

24
- 0026911214
- Optical and magneto-optical characterization of evaporated Co/Pt alloys and multilayers
- (1992) IEEE Transactions on Magnetics , vol.28 , pp. 2967
- Brändle, H.¹ Weller, D.² Scott, J.C.³ Parkin, S.S.P.⁴ Lin, C.J.⁵

25
- 84931522393
- B.E. Warren, X ray Diffraction (Dover Publications, Inc., New York, 1990), p. 208. S is defined as (rPt - xPt)/yCo where rPt is the fraction of Pt sites correctly occupied, xPt is the Pt sample fraction, and yCo is the fraction of Co sites in the perfectly ordered alloy. We assume the perfectly ordered alloy consists of alternating CoCo and CoPt planes. This structure can be represented as two hexagonal sublattices, one containing only Co and the other consisting of alternating layers of Co and Pt. We apply the definition of S to the CoPt sublattice. With this definition S=1 for Co3Pt with perfect layerwise chemical order while S=0 for complete chemical disorder. By applying the definition of S to only the CoPt sublattice, S is sensitive only to layerwise chemical order and not to in plane chemical order.

* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.