Link to ToF pages

hugo/content/py/fitting/extended/reflectometry-honeycomb/index.md

@@ -62,7 +62,7 @@ the $M_{s150}$ parameter is fitted.
 
 
 All layers are modeled without absorption, i.e. no imaginary part of the SLD.
-Ferthermore, we apply a resolution correction as described in [this tutorial]({{% ref-py "instr/scan/tofr-with-resolution" %}})
+Ferthermore, we apply a resolution correction as described in [this tutorial]({{% ref-py "instr/scan/tof-resolution" %}})
 with a fixed value for $\Delta Q / Q = 0.018$.
 The experimental data is normalized to unity, but we still fit the intensity, as is necessary due to the resolution correction.
 

hugo/content/py/fitting/extended/reflectometry-pt-layer/index.md

@@ -35,7 +35,7 @@ and the following six parameters are utilized:
 
 * Thickness of the Pt layer: `t_pt/nm`
 
-* The relative $Q$-resolution: `q_res/q` ([c.f.]({{% ref-py "instr/scan/tofr-with-resolution" %}}))
+* The relative $Q$-resolution: `q_res/q` ([c.f.]({{% ref-py "instr/scan/tof-resolution" %}}))
 
 * A $Q$-offset: `q_offset`
 

hugo/content/py/instr/polarized/polarized-non-perfect-ap/index.md

@@ -15,7 +15,7 @@ On top of the iron layer is a thin Pd cap layer.
 We don't explain the whole script in detail here, it combines all concepts that were introduced before
 in the polarized reflectometry section.
 Instrument resolution is simulated as explained in the
-[ToF - Resolution effects example]({{% ref-py "instr/scan/tofr-with-resolution" %}}).
+[ToF - Resolution effects example]({{% ref-py "instr/scan/tof-resolution" %}}).
 Furthermore, a constant background is added:
 
 {{< highlight python>}}

hugo/content/py/instr/polarized/polarized-spinasymmetry/index.md

@@ -41,7 +41,7 @@ This is performed in the function `plotSpinAsymmetry`.
 #### Further corrections
 
 We also apply a resolution correction, as described in the
- [ToF - Resolution effects]({{% ref-py "instr/scan/tofr-with-resolution" %}}) example.
+ [ToF - Resolution effects]({{% ref-py "instr/scan/tof-resolution" %}}) example.
 
 Furthermore, we introduce an offest in the $Q$-axis, in order to accomodate for experimental uncertainties
 in the measurement of $\theta$.

hugo/content/py/instr/scan/_index.md

@@ -55,4 +55,15 @@ and
 scan = ba.QzScan(axis)
 ```
 
-{{% children  %}}
+After constructing a scan, set the wavelength and optionally a constant offset
+$\delta q_z$ using
+```python
+scan.setWavelength(lambda)
+scan.setOffset(dqz)
+```
+
+Usage is demonstrated in page [time-of-flight reflectometry](tof).
+
+Handling of resolution will change soon.
+The current API is demonstrated in page
+[time-of-flight reflectometry with resolution](tof-resolution).