Difference between revisions of "Geometry:WAXS 3D"
KevinYager (talk | contribs) (Created page with "In wide-angle scattering (WAXS), one cannot simply assume that the detector plane is orthogonal to the incident x-ray beam. Converting from detector pixel coordina...") |
KevinYager (talk | contribs) (→Area Detector on Goniometer Arm) |
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In wide-angle [[scattering]] ([[WAXS]]), one cannot simply assume that the detector plane is orthogonal to the incident [[x-ray]] beam. Converting from detector pixel coordinates to 3D ''q''-vector is not always trivial, and depends on the experimental geometry. | In wide-angle [[scattering]] ([[WAXS]]), one cannot simply assume that the detector plane is orthogonal to the incident [[x-ray]] beam. Converting from detector pixel coordinates to 3D ''q''-vector is not always trivial, and depends on the experimental geometry. | ||
− | + | =Area Detector on Goniometer Arm= | |
Consider a 2D (area) detector connected to a goniometer arm. The goniometer has a center of rotation at the center of the sample (i.e. the incident beam passes through this center, and scattered rays originate from this point also). Let <math>\scriptstyle \phi_g </math> be the in-plane angle of the goniometer arm (rotation about <math>\scriptstyle z </math>-axis), and <math>\scriptstyle \theta_g </math> be the elevation angle (rotation away from <math>\scriptstyle xy </math> plane and towards <math>\scriptstyle z </math> axis). | Consider a 2D (area) detector connected to a goniometer arm. The goniometer has a center of rotation at the center of the sample (i.e. the incident beam passes through this center, and scattered rays originate from this point also). Let <math>\scriptstyle \phi_g </math> be the in-plane angle of the goniometer arm (rotation about <math>\scriptstyle z </math>-axis), and <math>\scriptstyle \theta_g </math> be the elevation angle (rotation away from <math>\scriptstyle xy </math> plane and towards <math>\scriptstyle z </math> axis). | ||
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* <math>\scriptstyle x </math>: Pixel position on detector (horizontal). | * <math>\scriptstyle x </math>: Pixel position on detector (horizontal). | ||
* <math>\scriptstyle z </math>: Pixel position on detector (vertical). | * <math>\scriptstyle z </math>: Pixel position on detector (vertical). | ||
+ | * <math>\scriptstyle d </math>: Sample-detector distance. | ||
* <math>\scriptstyle \theta_g </math>: Elevation angle of detector. | * <math>\scriptstyle \theta_g </math>: Elevation angle of detector. | ||
* <math>\scriptstyle \phi_g </math>: In-plane angle of detector. | * <math>\scriptstyle \phi_g </math>: In-plane angle of detector. | ||
Note that <math>\scriptstyle x </math> and <math>\scriptstyle z </math> are defined relative to the direct-beam. That is, for <math>\scriptstyle \theta_g = 0 </math> and <math>\scriptstyle \phi_g =0 </math>, the direct beam is at position <math>\scriptstyle (x,z)=(0,0) </math> on the area detector. | Note that <math>\scriptstyle x </math> and <math>\scriptstyle z </math> are defined relative to the direct-beam. That is, for <math>\scriptstyle \theta_g = 0 </math> and <math>\scriptstyle \phi_g =0 </math>, the direct beam is at position <math>\scriptstyle (x,z)=(0,0) </math> on the area detector. | ||
+ | |||
+ | ==Central Point== | ||
+ | The point <math>\scriptstyle (x,z)=(0,0) </math> on the detector probes the total scattering angle: | ||
+ | :<math> | ||
+ | \begin{alignat}{2} | ||
+ | 2 \theta_s = \Theta & = 1 \\ | ||
+ | & = 1 | ||
+ | \end{alignat} | ||
+ | </math> | ||
==See Also== | ==See Also== | ||
* [[Geometry:TSAXS 3D]] | * [[Geometry:TSAXS 3D]] | ||
* <math>\scriptstyle \theta_g </math> | * <math>\scriptstyle \theta_g </math> |
Revision as of 09:44, 13 January 2016
In wide-angle scattering (WAXS), one cannot simply assume that the detector plane is orthogonal to the incident x-ray beam. Converting from detector pixel coordinates to 3D q-vector is not always trivial, and depends on the experimental geometry.
Area Detector on Goniometer Arm
Consider a 2D (area) detector connected to a goniometer arm. The goniometer has a center of rotation at the center of the sample (i.e. the incident beam passes through this center, and scattered rays originate from this point also). Let be the in-plane angle of the goniometer arm (rotation about -axis), and be the elevation angle (rotation away from plane and towards axis).
The final scattering vector depends on:
- : Pixel position on detector (horizontal).
- : Pixel position on detector (vertical).
- : Sample-detector distance.
- : Elevation angle of detector.
- : In-plane angle of detector.
Note that and are defined relative to the direct-beam. That is, for and , the direct beam is at position on the area detector.
Central Point
The point on the detector probes the total scattering angle: