1
Fork 0
This commit is contained in:
prescientmoon 2025-03-21 13:36:08 +01:00
commit 62f8a1c05f
Signed by: prescientmoon
SSH key fingerprint: SHA256:UUF9JT2s8Xfyv76b8ZuVL7XrmimH4o49p4b+iexbVH4
3 changed files with 5 additions and 4 deletions

View file

@ -4,7 +4,7 @@
\begin{definition}[Laplace-Beltrami operator]
a generalization of the Laplace operator to more general spaces
\begin{align*}
\Delta f \coloneq \divergence \nabla f
\Delta f \coloneq \divergence \nabla f.
\end{align*}
\end{definition}
\item The spectrum of this operator is a subset of $[0, \infty)$. We call it the \emph{spectrum} of the manifold.

View file

@ -4,6 +4,7 @@
\usecolortheme{lily}
\setbeamertemplate{navigation symbols}{}
% boadilla seems to be the only one with enough space for stuff.compile it now it is very toxic but works
\usepackage{graphicx} % Required for inserting images
@ -122,7 +123,7 @@ code-for-last-col = \color{blue}
\pause
\item For the majority of groups $\Gamma$, the anisotropies $\frac{\delta T}{T}$ do not coincide with observations.
\pause
\item The only groups for which it does are $\Gamma = O^*$ and $\Gamma = I^*$ — the \textcolor{red}{binary octahedral} and \textcolor{red}{binary icosahedral} groups of order 48 and 120 respectively.
\item The only groups for which they do are $\Gamma = O^*$ and $\Gamma = I^*$ — the \textcolor{red}{binary octahedral} and \textcolor{red}{binary icosahedral} groups of order 48 and 120 respectively.
\pause
\end{itemize}
\begin{figure}[H]
@ -160,7 +161,7 @@ code-for-last-col = \color{blue}
\begin{frame}{Statistical Isotropy and Hypothesis}
\small
\textbf{Theoretical Expectation:}\\
From the perspective of an Earth-based observer, we can view the CMB as a function defined on the celestial sphere $\mathbb{S}^2$.\\
From the perspective of an Earth-based observer, we can view the CMB as a function defined on the celestial sphere $\mathbb{S}^2.$\\
\begin{itemize}
\pause
\item The CMB temperature fluctuations can be expanded as:

View file

@ -47,7 +47,7 @@
& \rotmat{2 \pi s_2 / q} & & \\
& & \ddots & \\
& & & \rotmat{2 \pi s_n / q}
\end{pmatrix}
\end{pmatrix}.
\end{align*}
\end{definition}