From 2c0b4a32b925bffd3590ded6baade9d40718e882 Mon Sep 17 00:00:00 2001
From: "juso.koc" <juso.koc@gmail.com>
Date: Thu, 20 Mar 2025 13:31:33 +0000
Subject: [PATCH] Update on Overleaf.
---
main.tex | 2 +-
1 file changed, 1 insertion(+), 1 deletion(-)
diff --git a/main.tex b/main.tex
index ede4a46..ec90553 100644
--- a/main.tex
+++ b/main.tex
@@ -101,7 +101,7 @@ code-for-last-col = \color{blue}
\item Manifolds $\textcolor{blue}{M} := \mathbb{S}^3 /_ \sim$ where $\sim $ identifies the orbits of finite $H \leq SO(4)$ finite
\item Helmholtz equation on $M$ given by
- $$(\Delta + E_\textcolor{red}{\beta}^M\textcolor{blue}{M})\psi_\textcolor{red}{\beta}^{M, i} = 0$$
+ $$(\Delta + E_\textcolor{red}{\beta}^\textcolor{blue}{M})\psi_\textcolor{red}{\beta}^{M, i} = 0$$
\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