Abstract
When bismuth is substituted at certain lattice points of rare earth garnet crystals, a material is formed which exhibits an almost ideal magnetic stripe domain structure. The structure consists of a one-dimensional periodic array of regions of nearly constants magnetization, so that the magnitudes of the magnetization vectors in two adjacent regions are the same, but their directions are opposite. This condition produces the alternating-sign magnetic permeability tensors shown in section 1.7(3). When a beam of light is passed through such a film, it splits into many diffracted beams, all sharing a plane defined by the periodicity direction (i.e., the y-component of all the wave vectors is the same; see Figure 1.1). The angles of the diffracted-beam directions relative to the incident-beam direction are determined by the periodicity length.
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Remarks and References
L.F. Schiff, Quantum Mechanics, McGraw-Hill, New York, 1968, pp. 298–320
B.A. Lippmann and J. Schwinger, Phys. Rev. 79, p. 469 (1950). The diffraction model described in section 1.1 is known as the Quantum Mechanical Kronig-Penney Diffraction Model; see
CA. Wert and R.M. Thomson, Physics of Solids, McGraw-Hill, New York, 1970, pp. 361–368.
J.M. Cowley, Diffraction Physics, North-Holland-American Elesvier, New York, 1975.
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© 1988 Springer-Verlag New York Inc.
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Friedman, A. (1988). Scattering by Stripe Grating. In: Mathematics in Industrial Problems. The IMA Volumes in Mathematics and Its Applications, vol 16. Springer, New York, NY. https://doi.org/10.1007/978-1-4615-7399-9_2
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DOI: https://doi.org/10.1007/978-1-4615-7399-9_2
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