Run trailing-whitespace, end-of-file-fixer, black

.clang-format

@@ -131,6 +131,6 @@ IncludeCategories:
     Priority: 9
 
 # Future options - not supported in clang-format 12
-# 
+#
 # OperandAlignmentStyle: Align
 ...

.gitattributes

@@ -1 +1 @@
-bin/* text eol=lf
+bin/* text eol=lf

CONTRIBUTING.md

@@ -290,4 +290,3 @@ Test Suite Examples
 
 You know a useful setting to validate our provided methods?
 Tell us about it or add it to our test sets in the examples/ folder!
-

COPYING

@@ -672,4 +672,3 @@ may consider it more useful to permit linking proprietary applications with
 the library.  If this is what you want to do, use the GNU Lesser General
 Public License instead of this License.  But first, please read
 <http://www.gnu.org/philosophy/why-not-lgpl.html>.
-

COPYING.LESSER

@@ -163,4 +163,3 @@ whether future versions of the GNU Lesser General Public License shall
 apply, that proxy's public statement of acceptance of any version is
 permanent authorization for you to choose that version for the
 Library.
-

bin/picongpu-completion.bash

@@ -250,4 +250,3 @@ complete -o nospace -F _pic-compile pic-compile
 complete -o nospace -F _pic-configure pic-configure
 complete -F _pic-edit pic-edit
 complete -o nospace -F _tbg tbg
-

docs/BorisPusher/BorisPusher.tex

@@ -24,7 +24,7 @@ \section{Boris-Pusher}
 \end{equation}
 wobei $q$ die Ladung und $\vec{v}$ die Geschwindigkeit ist. $\vec{E}$ und $\vec{B}$ befinden sich am Ort des Teilchens. Zwischen $\vec{p}$ und $\vec{v}$ besteht der Zusammenhang:
 \begin{equation}
-	\vec{v} = \frac{\vec{p}}{m \gamma} = \frac{\vec{p}}{\sqrt{m^{2} + \frac{\vec{p}^{2}}{c^{2}}}} 
+	\vec{v} = \frac{\vec{p}}{m \gamma} = \frac{\vec{p}}{\sqrt{m^{2} + \frac{\vec{p}^{2}}{c^{2}}}}
 \end{equation}
 mit der Ruhemasse $m$. Für kleine Impulse, also $p \ll m c$ gilt die nicht-relatistische Näherungsformel:
 \begin{equation}
@@ -38,7 +38,7 @@ \section{Boris-Pusher}
 \end{equation}
 Um $\vec{p}_{t}$ zu bekommen, wurden $\vec{p}_{t + \nicefrac{1}{2}}$ und $\vec{p}_{t - \nicefrac{1}{2}}$ gemittelt. Das Problem ist nur, dass wir $\vec{p}_{t + \nicefrac{1}{2}}$ nicht kennen. Hier hilft uns ein Trick weiter. Zunächst führen wir dazu die Variablen $\vec{p}^{-}$ und $\vec{p}^{+}$ ein:
 \begin{equation}
-	\vec{p}_{t - \nicefrac{1}{2}} = \vec{p}^{-} - \frac{1}{2} q \vec{E} \Delta t 
+	\vec{p}_{t - \nicefrac{1}{2}} = \vec{p}^{-} - \frac{1}{2} q \vec{E} \Delta t
 \end{equation}
 \begin{equation}
 	\vec{p}_{t + \nicefrac{1}{2}} = \vec{p}^{+} + \frac{1}{2} q \vec{E} \Delta t
@@ -72,4 +72,4 @@ \section{Boris-Pusher}
 	\vec{p}^{+} = \vec{p}^{-} + \vec{p}\prime \times \vec{s}
 \end{equation}
 
-\end{document}
+\end{document}

docs/BorisPusher/VayPusher.tex

@@ -17,7 +17,7 @@ \section{Vay-Pusher}
 
 
 \subsection{Conventions}
-All indices have been reduced by a $\frac{1}{2}$-step compared to the paper. 
+All indices have been reduced by a $\frac{1}{2}$-step compared to the paper.
 Locations ($\vec r_i$) and fields ($\vec E_i$, $\vec B_i$) are known at full time steps, momenta and speeds ($\vec p_i$, $\vec u_i$, $\vec v_i$) at half time steps. In contrast to the Vay paper real momenta ($\vec p_i = \vec u_i \cdot m_0$) will be used.
 \begin{eqnarray*}
 \mbox{Vay paper} & \rightarrow & \mbox{implematation in PIC} \\
@@ -30,7 +30,7 @@ \subsection{Conventions}
 \end{eqnarray*}
 
 \subsection{Variables handed to particle pusher}
-The pusher takes: 
+The pusher takes:
 \begin{itemize}
 	\item $\vec E_0$ \quad \texttt{eField}
 	\item $\vec B_0$ \quad \texttt{bField}
@@ -50,7 +50,7 @@ \subsection{Second step of the algorithm}
 \vec p \prime  & = & \vec p_{0} + \frac{q \Delta t}{2} \vec E_{0} \\
 \gamma \prime & = & \sqrt{1 + \frac{{\vec p \prime}^2}{m_0^2 c^2 }} \\
 \vec \tau & = & \frac{q \Delta t}{2 m_0} \vec B_{0} \\
-u^{\star} & = & \frac{\vec p \prime \cdot \vec \tau}{m_0 c} \\ 
+u^{\star} & = & \frac{\vec p \prime \cdot \vec \tau}{m_0 c} \\
 \sigma & = & {\gamma \prime }^2 - {\vec \tau}^2 \\
 \gamma_{+1/2} & = & \sqrt{\frac{  \sigma + \sqrt{  \sigma^2 + 4 \left( {\vec \tau}^2 + {u^\star}^2 \right) } }{2}} \\
 \vec t & = & \frac{\vec \tau}{\gamma_{+1/2}} \\
@@ -63,4 +63,4 @@ \subsection{Particle push}
 
 
 
-\end{document}
+\end{document}

docs/COMMIT.md

@@ -136,4 +136,3 @@ Compile **all CMake presets** of a *single example* with:
 - Compile like a boss!
   `<pathToYourPIConGPUgitDirectory>/compile -l -q -j 60 <pathToYourPIConGPUgitDirectory>/examples/ $tmpPath`
 - Wait for the **thumbs up/down** :)
-

docs/picongpu-docs-env.yml

@@ -12,4 +12,3 @@ dependencies:
   - pip
   - pip:
     - "-r requirements.txt"
-

docs/propose_changelog.py

@@ -27,8 +27,7 @@
 print(m_list[m_sel], milestones[m_sel].number)
 
 # get pulls (all pulls are also issues but not vice versa)
-issues = repo.get_issues(state="closed", sort="updated", direction="asc",
-                         milestone=milestones[m_sel])
+issues = repo.get_issues(state="closed", sort="updated", direction="asc", milestone=milestones[m_sel])
 # Use this in the future, but pagination seems broken in it:
 # search_string = 'repo:ComputationalRadiationPhysics/picongpu ' +
 #                 'type:pr is:merged milestone:"'+milestones[m_sel].title+'"'
@@ -37,34 +36,11 @@
 
 
 # categories
-user = {
-    "input": []
-}
-bugs = {
-    "core": [],
-    "pmacc": [],
-    "plugin": [],
-    "tools": [],
-    "other": []
-}
-features = {
-    "core": [],
-    "pmacc": [],
-    "plugin": [],
-    "tools": [],
-    "other": []
-}
-refactoring = {
-    "core": [],
-    "pmacc": [],
-    "plugin": [],
-    "tools": [],
-    "other": []
-}
-misc = {
-    "docs": [],
-    "other": []
-}
+user = {"input": []}
+bugs = {"core": [], "pmacc": [], "plugin": [], "tools": [], "other": []}
+features = {"core": [], "pmacc": [], "plugin": [], "tools": [], "other": []}
+refactoring = {"core": [], "pmacc": [], "plugin": [], "tools": [], "other": []}
+misc = {"docs": [], "other": []}
 
 for i in issues:
     # skip issues, only pull requests