Commit 11776df9 authored by Florian Goth's avatar Florian Goth
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typos

parent f958f52c
......@@ -182,7 +182,7 @@ This document is intended to be self-contained, but the interested reader should
%%%%%%%%%%%%%%%%%%%%
\part{Just run it}
What follows is a collection of self-explanatory Jupyter notebooks written in Python, each centered on a detailed example followed by a few simple exercises. The notebooks printed bellow can be found, together with the necessary files and an increasing number of additional notebooks exploring ALF's capabilities, in the \href{https://git.physik.uni-wuerzburg.de/ALF/pyALF}{pyALF repository}.
What follows is a collection of self-explanatory Jupyter notebooks written in Python, each centered on a detailed example followed by a few simple exercises. The notebooks printed below can be found, together with the necessary files and an increasing number of additional notebooks exploring ALF's capabilities, in the \href{https://git.physik.uni-wuerzburg.de/ALF/pyALF}{pyALF repository}.
\section*{Requirements}
......@@ -228,7 +228,7 @@ jupyter notebook
%\begin{lstlisting}[style=bash]
%jupyter-notebook
%\end{lstlisting}
which opens the ``notebook dashboard'' in your default browser, where you can navigate through your file structure to the pyALF directory. There you will find the interface's core module, \texttt{py\_alf.py}, some auxiliary files, and notebooks such as the ones included bellow. Have fun.
which opens the ``notebook dashboard'' in your default browser, where you can navigate through your file structure to the pyALF directory. There you will find the interface's core module, \texttt{py\_alf.py}, some auxiliary files, and notebooks such as the ones included below. Have fun.
%We note that pyALF can also be used to start a simulation from the command line, without starting a Jupyter server. For instance:
%\begin{lstlisting}[style=bash]
......@@ -364,7 +364,7 @@ The SU(2) Hubbard-Stratonovich decomposition couples to the density and conserve
\exercise{Defining a new model: The one-dimensional t-V model}
In this section, one we will show what modifications have to be carried out for computing the physics of the one dimensional t-V model of spinless fermions.
In this section, we will show what modifications have to be carried out for computing the physics of the one dimensional t-V model of spinless fermions.
\begin{equation}
\hat{H} = -t \sum_{i} \left( \hat{c}^{\dagger}_{i} \hat{c}^{\phantom\dagger}_{i+a} + \hat{c}^{\dagger}_{i+a} \hat{c}^{\phantom\dagger}_{i} \right) - \frac{V}{2} \sum_{i} \left( \hat{c}^{\dagger}_{i} \hat{c}^{\phantom\dagger}_{i+a} + \hat{c}^{\dagger}_{i+a} \hat{c}^{\phantom\dagger}_{i} \right)^2 .
\end{equation}
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