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About McXtrace Documentation |
14.5 The Shell_p McXtrace ComponentSingle parabolic shell as part of a Wolter optic.
Identification
DescriptionA single shell is simulated. The top and bottom are curved cylindrically azimuthally. The sagital profile is defined by a parabola, which passes through the radii raidus_m at z=0, and radius_p at zentry (<0). To intersect the Wolter I plates we take advatage of the azimuthal symmetry and only consider the radial component of the photon’s wavevector. Imperfect mirrors may be modelled using one of 4 models. In all cases the surface normal of the mirror at the ideal mirror intersection point is perturbed before the exit vector is computed. 1. Longitudinal 1D. A perturbation angle is chosen from a uniform distribution with width waviness. 2. Isotropic 2D. The surface normal is perturbed by choosing an angle on a disc with radius waviness 3. Externally measured/computed data. We interpolate in a data-file consisting of blocks of dtheta/theta with 1 block per energy. dtheta is a sampled angle offset from the nominal Fresnel grazing angle theta. 4. Double gaussian. dtheta is chosen from one of two gaussian distributions. Either specular or off-specular, where the widths (sigmas) are given by the tables in the file ”wave_file”. If the off-specular case the behaviour is similar to 2D uniform case. In the case of 3, the format of the data file should be: #e_min=0.1 #e_max=15 #e_step=0.01 #theta_min=0.01 #theta_max=1.5 #theta_step=0.01 #dtheta_min=-0.02 #dtheta_max=0.02 #dtheta_step=0.001 1.0 0.9 0.8 0.75 ... 0.99 0.89 0.79 0.749 ...
... #block 2 (energy data point 2) 1.0 0.9 0.8 0.75 ... 0.99 0.89 0.79 0.749 ...
... I.e. one 2D data block per energy data point where rows represent the steps in nominal incident angle, and columns represent the sampled granularity of the off-specular scattering. Example: Shell_p( radius_p=0.535532, radius_m=0.533113, zdepth=0.5, Z0=12, yheight=1e-2, R_d=1)
Input parametersParameters in boldface are required; the others are optional.
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