|
|
Line 13: |
Line 13: |
| </math> | | </math> |
| where <math>\scriptstyle d</math> is the sample-detector distance, <math>\scriptstyle \alpha_f ^{\prime} </math> is the out-of-plane component (angle w.r.t. to ''y''-axis, rotation about x-axis), and <math>\scriptstyle \theta_f </math> is the in-plane component (rotation about ''z''-axis). The alternate angle, <math>\scriptstyle \alpha_f </math>, is the elevation angle in the plane defined by <math>\scriptstyle \theta_f </math>. Also note that the full scattering angle is: | | where <math>\scriptstyle d</math> is the sample-detector distance, <math>\scriptstyle \alpha_f ^{\prime} </math> is the out-of-plane component (angle w.r.t. to ''y''-axis, rotation about x-axis), and <math>\scriptstyle \theta_f </math> is the in-plane component (rotation about ''z''-axis). The alternate angle, <math>\scriptstyle \alpha_f </math>, is the elevation angle in the plane defined by <math>\scriptstyle \theta_f </math>. Also note that the full scattering angle is: |
| + | |
| + | ====now==== |
| :<math> | | :<math> |
| \begin{alignat}{2} | | \begin{alignat}{2} |
− | 2 \theta_s = \Theta & = \arctan\left[ \frac{ \sqrt{x^2 + z^2}}{d} \right] | + | 2 \theta_s = \Theta & = \arctan\left[ \frac{ \sqrt{x^2 + z^2}}{d} \right] \\ |
| + | & = \arctan\left[ \frac{ \sqrt{x^2 + z^2}}{d} \right] \\ |
| \end{alignat} | | \end{alignat} |
| </math> | | </math> |
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Line 31: |
| </math> | | </math> |
| | | |
− | And, of course:
| + | As a check: |
| :<math> | | :<math> |
| \begin{alignat}{2} | | \begin{alignat}{2} |
Revision as of 17:45, 29 December 2015
The q-vector in fact has three components:
Consider that the x-ray beam points along +y, so that on the detector, the horizontal is x, and the vertical is z. We assume that the x-ray beam hits the flat 2D area detector at 90° at detector (pixel) position . The scattering angles are then:
where is the sample-detector distance, is the out-of-plane component (angle w.r.t. to y-axis, rotation about x-axis), and is the in-plane component (rotation about z-axis). The alternate angle, , is the elevation angle in the plane defined by . Also note that the full scattering angle is:
now
The momentum transfer components are:
As a check: