Update on Overleaf.
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main.tex
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main.tex
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@ -98,12 +98,12 @@ code-for-last-col = \color{blue}
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\begin{frame}[fragile]{CMB Anisotropy of Homogeneous Spherical Spaces}
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\begin{itemize}
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\item Manifolds $M := \mathbb{S}^3 /_ \sim$ where $\sim $ identifies the orbits of finite $H \leq SO(4)$ finite
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\item Manifolds $\textcolor{blue}{M} := \mathbb{S}^3 /_ \sim$ where $\sim $ identifies the orbits of finite $H \leq SO(4)$ finite
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\item Helmholtz equation on $M$ given by
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$$(\Delta + E_\beta^M)\psi_\beta^{M, i} = 0$$
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$$(\Delta + E_\textcolor{red}{\beta}^M)\psi_\textcolor{red}{\beta}^{M, i} = 0$$
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\item In fact $E_\beta^m = \beta^2-1$ for $\beta \in \mathbb{N}$ we call $\beta$ a wave number
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\item In fact $E_\textcolor{red}{\beta}^m = \textcolor{red}{\beta}^2-1$ for $\textcolor{red}{\beta} \in \mathbb{N}$ we call $\textcolor{red}{\beta}$ a wave number
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\item The set of all possible wave numbers [for which there exists a non-zero solution] depends on $H$
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@ -154,7 +154,8 @@ code-for-last-col = \color{blue}
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\begin{itemize}
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\item Multi-connected space: it has non-contractable loops
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\item Inhomogeneous space: it does not look the same from every point in space
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\item Inhomogeneous space: it does not look identical from every point in space
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\item
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\end{itemize}
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\end{frame}
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