Date: Feb. 2017 Version: 1.1 Release: McXtrace 1.2 Origin: DTU Physics, DTU Space
Stack of conical shells as part of a Wolter optic.
Author: Erik B Knudsen and Desiree D. M. Ferreira
Origin: DTU Physics, DTU Space
Date: Feb. 2016
A stack of conical shells is simulated. To intersect the Wolter I plates we take advatage of the azimuthal symmetry and only consider the radial component of the photon’s wavevector.
Parameters in boldface are required; the others are optional.
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Name |
Unit |
Description |
Default |
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ring_nr |
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radius_m |
m |
Ring radius of the upper (reflecting) plate of the shell at the optic centre. |
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Z0 |
m |
Distance between optics centre plane and focal spot (essentially focal length). |
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xwidth |
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yheight |
m |
Height of the shell. |
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gap |
m |
Gap between the plate and the intersection plane with the hyperbolic section. (currently ignored) |
0 |
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chamferwidth |
m |
Width of side walls. |
0 |
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length |
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0 |
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mirror_reflec |
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Data file containing reflectivities of the reflector surface (TOP). |
”” |
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bottom_reflec |
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Data file containing reflectivities of the bottom surface (BOTTOM). |
”” |
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R_d |
|
Default reflectivity value to use if no reflectivity file is given. Useful f.i. is one surface is reflecting and the others absorbing. |
1 |
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primary |
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If non-zero, the shell is considered a primary reflector, and extends towards negative z. I.e. the entry plane is behind the z=0-plane. If zero, the shell is considered secondary |
1 |
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dalpha |
deg |
Offset to the alpha angle computed from the focal length. Useful for targeting the modified conical geometry (currently ignored). |
0 |
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waviness |
rad |
Waviness of the shell reflecting surface. The slope error is assumed to be uniformly distributed in the interval [-waviness:waviness]. |
0 |
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longw |
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If non-zero, waviness is 1D and along the shell axis. |
0 |
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Component source code found in file Ring_c.comp.