-                      r5ed76f8
+                      r8cc9048
    careful to note that distances are specified in cm!
 ) Enter values for the source wavelength(s), $\lambda$, and its spread (= $\text{FWHM}/\lambda$).
+) Enter values for the source wavelength(s), $\lambda$, and its spread (= $\mathrm{FWHM}/\lambda$).
    For monochromatic sources, the inputs are just one value. For TOF sources,
 …
    region near the beam block/stop
    [i.e., $Q < (2 \pi \cdot \text{beam block diameter}) / (\text{sample-to-detector distance} \cdot \lambda_\text{min})$]
+   [i.e., $Q < (2 \pi \cdot \mathrm{beam block diameter}) / (\mathrm{sample-to-detector distance} \cdot \lambda_\mathrm{min})$]
    the variance is slightly under estimated.

src/sas/sasgui/perspectives/calculator/media/sas_calculator_help.rst

-                      r1b67f3e
+                      r8cc9048
 where $\beta_j$ and $r_j$ are the scattering length density and
 the position of the $j^\text{th}$ pixel respectively.
+the position of the $j^\mathrm{th}$ pixel respectively.
 The total volume $V$
 …
     V = \sum_j^N v_j
 for $\beta_j \ne 0$ where $v_j$ is the volume of the $j^\text{th}$
 pixel (or the $j^\text{th}$ natural atomic volume (= atomic mass / (natural molar
+for $\beta_j \ne 0$ where $v_j$ is the volume of the $j^\mathrm{th}$
+pixel (or the $j^\mathrm{th}$ natural atomic volume (= atomic mass / (natural molar
 density * Avogadro number) for the atomic structures).
 …
 Now let us assume that the angles of the $\vec Q$ vector and the spin-axis ($x'$)
 to the $x$-axis are $\phi$ and $\theta_\text{up}$ respectively (see above). Then,
+to the $x$-axis are $\phi$ and $\theta_\mathrm{up}$ respectively (see above). Then,
 depending upon the polarization (spin) state of neutrons, the scattering
 length densities, including the nuclear scattering length density ($\beta_N$)
 …
 .. math::
     M_{\perp x'} &= M_{0q_x}\cos\theta_\text{up} + M_{0q_y}\sin\theta_\text{up} \\
     M_{\perp y'} &= M_{0q_y}\cos\theta_\text{up} - M_{0q_x}\sin\theta_\text{up} \\
+    M_{\perp x'} &= M_{0q_x}\cos\theta_\mathrm{up} + M_{0q_y}\sin\theta_\mathrm{up} \\
+    M_{\perp y'} &= M_{0q_y}\cos\theta_\mathrm{up} - M_{0q_x}\sin\theta_\mathrm{up} \\
     M_{\perp z'} &= M_{0z} \\
     M_{0q_x} &= (M_{0x}\cos\phi - M_{0y}\sin\phi)\cos\phi \\
 …
 where $v_j \beta_j \equiv b_j$ is the scattering
 length of the $j^\text{th}$ atom. The calculation output is passed to the *Data Explorer*
+length of the $j^\mathrm{th}$ atom. The calculation output is passed to the *Data Explorer*
 for further use.

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SasView

Changeset 8cc9048 in sasview for src/sas/sasgui/perspectives/calculator/media

Legend:

src/sas/sasgui/perspectives/calculator/media/resolution_calculator_help.rst

src/sas/sasgui/perspectives/calculator/media/sas_calculator_help.rst

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