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For an overview of GMR and exchange coupling see, e.g., Ultrathia Magnetic Structures, edited by B. Heinrich and J. A. C. Bland (Springer, Berlin, 1994), Vol. 2, or S. S. P. Parkin, Annu. Rev. Mater. Sci. 25, 357 (1995), and references therein.
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and references therein
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For an overview of GMR and exchange coupling see, e.g., Ultrathia Magnetic Structures, edited by B. Heinrich and J. A. C. Bland (Springer, Berlin, 1994), Vol. 2, or S. S. P. Parkin, Annu. Rev. Mater. Sci. 25, 357 (1995), and references therein.
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20
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85034550643
-
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note
-
2 large and 1 mm thick MgO substrate which was prepared at the same time and under the same conditions as the large sample. The volume of the magnetic material was calculated from the surface area, determined by weighting of the sample, times the thickness obtained from the x-ray measurement. The very small amount of magnetic material led to the noisy VSM measurement of Fig. 1.
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21
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0032093581
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A. Schreyer, R. Siebrecht, U. Englisch, U. Pietsch, and H. Zabel, Physica B 248, 349 (1998).
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24
-
-
85034556566
-
-
note
-
e: classical electron radius, p(r): electron density, λ: x-ray wavelength, Z: total number of electrons per unit cell]. The sum is taken over all atoms of the unit cell. δ is proportional to the electron density away from absorption edges.
-
-
-
-
25
-
-
0001419961
-
-
For an overview on neutron reflectivity see, e.g., G. P. Felcher, Phys. Rev. B 24, 1595 (1981); J. Penfold and R. K. Thomas, J. Phys.: Condens. Matter 2, 1369 (1990); S. J. Blundell and J. A. C. Bland, Phys. Rev. B 46, 3391 (1992); H. Zabel, Physica B 198, 156 (1994); Ultrathin Magnetic Structures, edited by J. A. C. Bland and B. Heinrich (Springer, Berlin, 1994), Vol. 1.
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Felcher, G.P.1
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26
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11644271678
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For an overview on neutron reflectivity see, e.g., G. P. Felcher, Phys. Rev. B 24, 1595 (1981); J. Penfold and R. K. Thomas, J. Phys.: Condens. Matter 2, 1369 (1990); S. J. Blundell and J. A. C. Bland, Phys. Rev. B 46, 3391 (1992); H. Zabel, Physica B 198, 156 (1994); Ultrathin Magnetic Structures, edited by J. A. C. Bland and B. Heinrich (Springer, Berlin, 1994), Vol. 1.
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J. Phys.: Condens. Matter
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Penfold, J.1
Thomas, R.K.2
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27
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25544465129
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-
For an overview on neutron reflectivity see, e.g., G. P. Felcher, Phys. Rev. B 24, 1595 (1981); J. Penfold and R. K. Thomas, J. Phys.: Condens. Matter 2, 1369 (1990); S. J. Blundell and J. A. C. Bland, Phys. Rev. B 46, 3391 (1992); H. Zabel, Physica B 198, 156 (1994); Ultrathin Magnetic Structures, edited by J. A. C. Bland and B. Heinrich (Springer, Berlin, 1994), Vol. 1.
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Phys. Rev. B
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Blundell, S.J.1
Bland, J.A.C.2
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28
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0028405712
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For an overview on neutron reflectivity see, e.g., G. P. Felcher, Phys. Rev. B 24, 1595 (1981); J. Penfold and R. K. Thomas, J. Phys.: Condens. Matter 2, 1369 (1990); S. J. Blundell and J. A. C. Bland, Phys. Rev. B 46, 3391 (1992); H. Zabel, Physica B 198, 156 (1994); Ultrathin Magnetic Structures, edited by J. A. C. Bland and B. Heinrich (Springer, Berlin, 1994), Vol. 1.
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Physica B
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Zabel, H.1
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29
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0001419961
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Springer, Berlin
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For an overview on neutron reflectivity see, e.g., G. P. Felcher, Phys. Rev. B 24, 1595 (1981); J. Penfold and R. K. Thomas, J. Phys.: Condens. Matter 2, 1369 (1990); S. J. Blundell and J. A. C. Bland, Phys. Rev. B 46, 3391 (1992); H. Zabel, Physica B 198, 156 (1994); Ultrathin Magnetic Structures, edited by J. A. C. Bland and B. Heinrich (Springer, Berlin, 1994), Vol. 1.
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Bland, J.A.C.1
Heinrich, B.2
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30
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26144449160
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The parametrized continuous refractive index profile was divided into 1.5 Å thin boxes and the reflectivity as calculated using the Parratt formalism for sharp interfaces ("slicing method") [L. G. Parratt, Phys. Rev. 95, 359 (1954); M. Tolan, X-ray Scattering from Soft Matter Thin Films: Materials Science and Basic Research, Springer Tracts in Modern Physics, Vol. 148 (Springer, Berlin, 1999)].
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Parratt, L.G.1
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31
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The parametrized continuous refractive index profile was divided into 1.5 Å thin boxes and the reflectivity as calculated using the Parratt formalism for sharp interfaces ("slicing method") [L. G. Parratt, Phys. Rev. 95, 359 (1954); M. Tolan, X-ray Scattering from Soft Matter Thin Films: Materials Science and Basic Research, Springer Tracts in Modern Physics, Vol. 148 (Springer, Berlin, 1999)].
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0000964055
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g)=b/l, with b the beam width and l the sample width [A. Gibaud, G. Vignaud, and S. K. Sinha, Acta Crystallogr., Sect. A: Found. Crystallogr. 49, 642 (1993)]. Further, the FWHM of the specular peak should be half of the width of the primary beam even in the total external reflection regime.
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Gibaud, A.1
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Landolt-Börnstein, Vol. III/19c, Heusler Alloys, edited by P. J. Webster and K. R. A. Ziebeck (Springer, Berlin, 1996).
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