Updated READMEs

l-p-scattering/README.md

+# lepton proton scatter $`\mu p\to \mu p`$
+
+References: [[tbd]](https://arxiv.org/abs/20??.?????)
+
+Configurations implemented
+ * MESA $`ep\to ep`$, P2 experiment $`p_\text{in} = 155\,{\rm MeV}`$ with $`E_e > 45\,{\rm MeV}`$
+   and $`25^\circ < \theta < 45^\circ`$
+ * MUSE, $`ep\to ep`$ at $`p_\text{in} = 115\,{\rm MeV}`$
+   [[ref]](https://gitlab.psi.ch/mcmule/user-library/-/jobs/artifacts/master/file/ci/muse/muse.ipynb?job=run)

michel-decay/README.md

@@ -5,10 +5,13 @@ References: [[1909.10244]](https://arxiv.org/abs/1909.10244), [[1811.06461]](htt
 Configurations implemented
 
  * No cuts to obtain decay rate
+   [[ref]](https://gitlab.psi.ch/mcmule/user-library/-/jobs/artifacts/master/file/ci/validation/validation.ipynb?job=run)
  * Demonstration cuts: no photons with $`E_\gamma > 10\,{\rm MeV}`$
    within a cone of $`|\cos\sphericalangle(\vec p_\gamma,\vec p_e)| > 0.8`$
+   [[ref]](https://gitlab.psi.ch/mcmule/user-library/-/jobs/artifacts/master/file/ci/demo-observable/demo-observable.ipynb?job=run)
  * MEG cuts with photon veto
  * Full reconstruction of
+   [[ref]](https://gitlab.psi.ch/mcmule/user-library/-/jobs/artifacts/master/file/ci/f-and-g/f-and-g.ipynb?job=run)
 ```math
 \frac{{\rm d}^2\Gamma}{{\rm d}E_e\,{\rm d}(\cos\theta)} =
 \Gamma_0(f(E_e)+P\,\cos\theta\ g(E_e))

mu-e-scattering/README.md

+# Muon electron scattering $`\mu e\to \mu e`$
+
+References: [[tbd]](https://arxiv.org/abs/20??.?????)
+
+Configurations implemented
+ * MUonE experiment, Setups 2 and 4
+   [[ref]](https://gitlab.psi.ch/mcmule/user-library/-/jobs/artifacts/master/file/ci/muone/muone.ipynb?job=run)
+

radiative-lepton-decay/README.md

@@ -10,6 +10,7 @@ Configurations implemented
    * reduced cuts
  * PiBeta
  * BaBar
+   * Canonical cuts
    * Full implantation
    * Only the energy
    * Invariant mass
@@ -25,7 +26,8 @@ The canonical version refers to the values often quoted in the PDG of
 E_\gamma > 10\,\mathrm{MeV}
 ```
 Usually, this also means that we are exclusive, i.e. exactly one
-photon is visible.
+photon is visible. For the example for $`\tau\to\nu\bar\nu \gamma`$,
+see [here](babar/example/)
 
 ## MEG
 
@@ -48,7 +50,7 @@ E_\gamma > 40\,\mathrm{MeV}\,,\qquad E_e> 45\,\mathrm{MeV}
 ```
 MEG requires one and only one photon meaning that an event with real
 radiation with energy larger then the detector resolution of roughly 2
-MeV will be discarded if it hits the detector. 
+MeV will be discarded if it hits the detector.
 
 
 ### Reduced cuts
@@ -60,7 +62,7 @@ is valid.
 ## PiBeta cuts
 The PiBeta experiment had less stringent cuts when looking at the
 radiative muon decay, producing the current best result for this
-process. 
+process.
 
 ```math
 E_\gamma > 10\,\mathrm{MeV}\,,\qquad \sphericalangle(\vec p_\gamma,\vec p_e) > 30^\circ

radiative-lepton-decay/babar/example/README.md

@@ -8,3 +8,4 @@ of $`\tau\to\nu\bar\nu e\gamma`$ in
 [[1705.03782]](https://arxiv.org/pdf/1705.03782.pdf).
 
 We require $`E_\gamma > 10\,{\rm MeV}`$ in the $`\tau`$ restframe.
+[[ref]](https://gitlab.psi.ch/mcmule/user-library/-/jobs/artifacts/master/file/ci/example/example.ipynb?job=run)