Skip to content

Commit

Permalink
Updated Fig. 63. AJS
Browse files Browse the repository at this point in the history
  • Loading branch information
ajsteinmetz committed Sep 26, 2024
1 parent 4dc82d3 commit ccbc584
Show file tree
Hide file tree
Showing 5 changed files with 5 additions and 5 deletions.
10 changes: 5 additions & 5 deletions 06magnetization.tex
Original file line number Diff line number Diff line change
Expand Up @@ -572,7 +572,7 @@ \subsection{Relativistic paramagnetism of electron-positron gas}
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
\begin{figure}[ht]
\centering
\includegraphics[clip, trim=0.0cm 0.0cm 0.0cm 0.0cm,width=0.95\linewidth]{plots/thesis_perlepton.png}
\includegraphics[clip, trim=0.0cm 0.0cm 0.0cm 0.0cm,width=0.90\linewidth]{plots/thesis_perlepton.png}
\caption{The magnetic moment per lepton $\vert\vec{m}\vert_{z}$ along the field axis as a function of temperature. \cccite{Steinmetz:2023nsc}}
\label{fig:momentperlepton}
\end{figure}
Expand Down Expand Up @@ -612,10 +612,10 @@ \subsection{Polarization potential and ferromagnetism}
\noindent One exploratory model we propose is to fix the spin polarization asymmetry, described in \req{spotential}, to generate a homogeneous magnetic field which dissipates as the primordial Universe cools down. In this model, there is no external primordial magnetic field $({B}_\mathrm{PMF}=0)$ generated by some unrelated physics, but rather the $e^{+}e^{-}$ plasma itself is responsible for the field by virtue of spin polarization.

%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
\begin{figure}[ht]
\begin{figure}
\centering
\includegraphics[width=0.9\linewidth]{plots/Spinchemical_03.png}
\caption{The spin potential $\zeta$ and chemical potential\index{chemical potential} $\mu$ are plotted under the assumption of self-magnetization through a nonzero spin polarization in bulk of the plasma. \cccite{Steinmetz:2023nsc}}
\includegraphics[width=0.9\linewidth]{plots/Spinchemical_04.jpg}
\caption{The spin potential $\zeta$ and chemical potential\index{chemical potential} $\mu$ are plotted under the assumption of self-magnetization through a nonzero spin polarization in bulk of the plasma. \radapt{Steinmetz:2023nsc}}
\label{fig:self}
\end{figure}
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
Expand All @@ -632,7 +632,7 @@ \subsection{Polarization potential and ferromagnetism}
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
\begin{figure}[ht]
\centering
\includegraphics[width=0.90\linewidth]{plots/ElectronDensity_SpinChemicalPotential004.jpg}
\includegraphics[width=0.90\linewidth]{plots/ElectronDenisty_SpinChemicalPotential004.jpg}
\caption{The number density $n_{e^{\pm}}$ of polarized electrons and positrons under the self-magnetization model for differing values of $b_{0}$. \cccite{Steinmetz:2023nsc}}
\label{fig:polarswap}
\end{figure}
Expand Down
Loading
Sorry, something went wrong. Reload?
Sorry, we cannot display this file.
Sorry, this file is invalid so it cannot be displayed.
Binary file removed plots/ElectronDensity_SpinChemicalPotential004.jpg
Binary file not shown.
Binary file removed plots/Spinchemical_03.PNG
Binary file not shown.
Binary file added plots/Spinchemical_04.jpg
Loading
Sorry, something went wrong. Reload?
Sorry, we cannot display this file.
Sorry, this file is invalid so it cannot be displayed.

0 comments on commit ccbc584

Please sign in to comment.