1922
DOI: 10.1080/14786442208633940
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XCII. The reflexion of X-rays from imperfect crystals

Abstract: on the Reflexion of Equation (26) is suitable for use in computations for love temperatures. The expanded form for %(0) analogous to (24) is suitable for use with high temperatures and is more immediately intelligible than (26). This form is %(O)=27rvII(a) ~2 (2JII(¢))"-'-n~-I n ! x ~a + n+l " n+2 + n+3 .(27} and the corresponding form of the second virial coefficient is n=l ?t ! f(d-a)d ~ 2(d-~)-"d (d-~)83~ (28) × L" ~-~-+-i n+2 ÷ n+3 5" xoii. The Reflexlon of ,Y-Ra~/s from Imperfect Crystals.

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Cited by 285 publications
(70 citation statements)
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“…Failure to take account of this effect could lead to substantial underestimation of the nominally corrected value of the structure factor. Again, in his original paper, Darwin (1922) discussed whether an imperfect crystal should best be modelled as warped or cracked. Although he leaned towards the former model as probably the more realistic, he adopted the latter as being the more tractable mathematically.…”
Section: Importance Of Extrapolationmentioning
confidence: 99%
“…Failure to take account of this effect could lead to substantial underestimation of the nominally corrected value of the structure factor. Again, in his original paper, Darwin (1922) discussed whether an imperfect crystal should best be modelled as warped or cracked. Although he leaned towards the former model as probably the more realistic, he adopted the latter as being the more tractable mathematically.…”
Section: Importance Of Extrapolationmentioning
confidence: 99%
“…The crystal may have a mosaic structure, the third type of disorder, where there are several (or many) three dimensional regions of a crystal slightly misaligned to each other (Darwin, 1922). In the limit of very many small 'mosaic blocks' a crystal will have a crumbly nature (Stojanoff et al 1996).…”
Section: Quality Characterisation Of Protein Crystalsmentioning
confidence: 99%
“…This treatment uses the Zachariasen (1967) solution to the Darwin (1922) intensity transfer equations and is valid only for secondary extinction and small absorption. In addition, it is assumed that the crystal has a uniform cross section o-(to) over the irradiated volume and that the mosaic structure is sufficiently broad that the geometrical conditions for diffraction are satisfied for all neutrons in the incident beam.…”
Section: Extinction Treatmentmentioning
confidence: 99%
“…Secondly, the flipping ratio Rob s is measured across the rocking curve and not merely at the peak (R-on-rocking) and the curve is fitted on a point-by-point basis to a function in which the secondary extinction appears as a parameter ( van Laar, Maniawski & Kaprzyk, 1979). The fitting function is derived from Zachariasen's (1967) solution to the Darwin (1922) intensity transfer equations and should be excellent for weakly absorbing specimens. Unfortunately, the mechanical treatment of the sample increases the likelihood of multiple scattering and this, in turn, changes the measured flipping ratio at some or all points on the rocking curve, so that the fitting function no longer accurately describes the intensity distribution and unrealistic values for the extinction parameters and R may result.…”
mentioning
confidence: 99%