1981
DOI: 10.1107/s0567739481001770
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On the integrated reflectivity of perfect crystals in extremely asymmetric Bragg cases of X-ray diffraction

Abstract: TheoryIn the case of grazing incidence, the integrated reflectivity calculated according to the theory appropriate for extreme asymmetry is smaller than that calculated according to the conventional theory. In the case of grazing emergence the results calculated according to each theory exhibit smaller differences than for the first case within a great range of extreme asymmetry. In the conventional theory the integrated reflectivity tends to zero for a -0 B tending to zero, whereas the theory for extremely as… Show more

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Cited by 35 publications
(5 citation statements)
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“…[9][10][11][12][13][14][15][16][17][18][19][20]28 In this section, we will consider some examples at high incidence angles, where our GDT is always valid, in contrast to other theoretical models. [9][10][11][12][13][14][15][16][17][18][19][20]28 As a first example we may consider a short-period AlAs/GaAs superlattice ͑SL͒ coherently grown on a ͓100͔oriented GaAs substrate crystal. We assume that the SL is made by 66 periods with a period length of Pϭ1.2 nm, while the thicknesses of the two layers constituting one SL period are equal, i.e., 0.56 nm.…”
Section: Comparison With the Conventional Dynamical X-ray Theorymentioning
confidence: 99%
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“…[9][10][11][12][13][14][15][16][17][18][19][20]28 In this section, we will consider some examples at high incidence angles, where our GDT is always valid, in contrast to other theoretical models. [9][10][11][12][13][14][15][16][17][18][19][20]28 As a first example we may consider a short-period AlAs/GaAs superlattice ͑SL͒ coherently grown on a ͓100͔oriented GaAs substrate crystal. We assume that the SL is made by 66 periods with a period length of Pϭ1.2 nm, while the thicknesses of the two layers constituting one SL period are equal, i.e., 0.56 nm.…”
Section: Comparison With the Conventional Dynamical X-ray Theorymentioning
confidence: 99%
“…7,8 However, in some cases the above approximations are not valid: ͑i͒ for highly asymmetric x-ray diffractions, where simultaneously x-ray diffraction and reflection occur, [9][10][11][12][13][14][15][16][17][18] ͑ii͒ for grazing-incidence diffraction, 19,20 ͑iii͒ for Bragg angles that are very close to /2, 21-23 and ͑iv͒ for diffraction patterns, where the angular distance between the Bragg peaks is large ͑of the order of degrees͒. 24 Experimental evidences of the failure of the conventional x-ray dynamical theory ͑CDT͒ were also reported for extremely asymmetric Bragg x-ray diffractions on silicon ͑001͒ crystals.…”
Section: Introductionmentioning
confidence: 99%
“…1͒: ͑i͒ The coplanar extremely asymmetric diffraction ͑EAD͒ is realized when the diffraction planes make the Bragg angle with the crystal surface and either the incident or exit x-ray wave is grazing. [5][6][7][8][9][10][11][12] ͑ii͒ Surface or ''grazing-incidence'' diffraction 13 ͑GID͒ is the geometry where the Bragg planes are perpendicular to the surface and both the x-ray waves are grazing. [14][15][16][17][18][19][20][21][22][23] ͑iii͒ Finally, grazing Bragg-Laue diffraction ͑GBL͒ is a combination of the EAD and GID.…”
Section: Introductionmentioning
confidence: 99%
“…X-ray diffraction at grazing incidence and/or exit can be treated with the help of either an extended kinematical theory ͑often called the ''distorted wave Born approximation''͒, 16,19,41,49,55 or extended dynamical theory. 5,6,8,9,11,14,17,22,45,48,51,[56][57][58][59] Both approaches take into account refraction and specular reflection effects for grazing x rays at crystal surfaces and interfaces. As with ordinary Bragg diffraction, the kinematical theory is applicable to mosaic crystals, to the tails of the Bragg peaks, and to the diffraction from layers thinner than the x-ray extinction depth.…”
Section: Introductionmentioning
confidence: 99%
“…only the points close to the dispersion surface intersections are considered. However this second-order description of the dispersion surface is an assumption and the actual shape in figure 2.3.5 is of fourthorder, Härtwig (1981), Holý and Fewster (2003);…”
Section: Combination Of Specular Scattering and One Diffracted Wavementioning
confidence: 99%