[ Identification | Description | Input parameters | Output parameters | Links ]
This is a lay-out of the coherent hard x-ray (CHX) beamline at NSLS-II. Since the ray-tracing method doesn't allow to account for partial coherence of the undulator source, the best approximation was to use the gaussian photon beam and to neglect diffraction effects on apertures. The choice of the source sizes along with angular divergence corresponds to the situation of high emittance (e=0.99nm).
|L||m||Distance from the source to the SS1, secondary source aperture.||33.5|
|L2||m||Position of the CRL.||35.3|
|L3||m||Position of the Kinoform lens.||44|
|Energy||keV||primary energy used at the beamline.||10|
[ Identification | Description | Input parameters | Output parameters | Links ]Generated on 2022-01-24 12:07:05