Difference between revisions of "Geometry:WAXS 3D"

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(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...")
 
(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==
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=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).
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* <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.
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==Central Point==
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The point <math>\scriptstyle (x,z)=(0,0) </math> on the detector probes the total scattering angle:
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:<math>
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\begin{alignat}{2}
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2 \theta_s = \Theta & = 1 \\
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    & = 1
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\end{alignat}
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</math>
  
 
==See Also==
 
==See Also==
 
* [[Geometry:TSAXS 3D]]
 
* [[Geometry:TSAXS 3D]]
 
* <math>\scriptstyle \theta_g </math>
 
* <math>\scriptstyle \theta_g </math>

Revision as of 10:44, 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:

See Also