Starting with the integral form of the correction factor derived in the previous paper [Holmes & Barrington-Leigh (1974). Acta Cryst. A30, 635-638], the explicit form of the function describing intensity in reciprocal space for slightly disoriented non-crystalline fibres is described, and simplifying approximations are made. Correction factors for real data are calculated, and the validity of the theory tested with data from tobacco mosaic virus gels. A correction factor is also given for crystalline fibres
Processes of redistribution of optical signal energy between the optical fiber core and shell in con...
The intensity at the end face of a short graded-index optical fiber is evaluated in a convolution by...
The intensity profiles in a monomode fibre are approximated by Gaussian functions with spot size def...
The intensity function in reciprocal space is derived for the case of non-crystalline fibres with a ...
Many strong biological materials exist in the form of fibres that are partially crystalline but cont...
X-ray diffraction patterns from oriented polymer fibers depend both on the conformations of the poly...
In many systems of interest, both physical and biological, disorder inhibits the organization and co...
A procedure is given for separating and phasing terms originating from different Bessel-function ord...
Many objects in the real world can be modeled as fibres (i.e. lines in 2D or 3D space). If the proce...
The intensities of far-field diffraction patterns of orientationally aligned molecules obey Wilson s...
The validity conditions of the derivation of the expression for the variation of the reciprocal latt...
Crystal size and lattice distortion parameters were determined experimentally by recording X-ray dif...
The mathematical theory of the powder diffraction intensity function is presented in the form access...
Dispersion properties of photonic crystal fibers are analyzed by introducing perturbations to the id...
In Parnell & Abrahams (2008 Proc. R. Soc. A 464, 1461–1482. (doi:10.1098/rspa.2007.0254)), a homogen...
Processes of redistribution of optical signal energy between the optical fiber core and shell in con...
The intensity at the end face of a short graded-index optical fiber is evaluated in a convolution by...
The intensity profiles in a monomode fibre are approximated by Gaussian functions with spot size def...
The intensity function in reciprocal space is derived for the case of non-crystalline fibres with a ...
Many strong biological materials exist in the form of fibres that are partially crystalline but cont...
X-ray diffraction patterns from oriented polymer fibers depend both on the conformations of the poly...
In many systems of interest, both physical and biological, disorder inhibits the organization and co...
A procedure is given for separating and phasing terms originating from different Bessel-function ord...
Many objects in the real world can be modeled as fibres (i.e. lines in 2D or 3D space). If the proce...
The intensities of far-field diffraction patterns of orientationally aligned molecules obey Wilson s...
The validity conditions of the derivation of the expression for the variation of the reciprocal latt...
Crystal size and lattice distortion parameters were determined experimentally by recording X-ray dif...
The mathematical theory of the powder diffraction intensity function is presented in the form access...
Dispersion properties of photonic crystal fibers are analyzed by introducing perturbations to the id...
In Parnell & Abrahams (2008 Proc. R. Soc. A 464, 1461–1482. (doi:10.1098/rspa.2007.0254)), a homogen...
Processes of redistribution of optical signal energy between the optical fiber core and shell in con...
The intensity at the end face of a short graded-index optical fiber is evaluated in a convolution by...
The intensity profiles in a monomode fibre are approximated by Gaussian functions with spot size def...