Remove total column from table

main.tex

@@ -302,61 +302,35 @@ presented in the following.
 
 \begin{table}
 \centering
-\begin{tabular}{cccc} \toprule
-    {$\gamma$} & Spatial & Spin & Total  \\ \hline
+\begin{tabular}{ccc} \toprule
+    {$\gamma$} & Spatial Pairing & Spin Pair  \\ \hline
     \sym A 1    & \numberedHexagon{$\Delta_s$}{1}{1}{1}{1}{1}{1}
-                & $\Psi$
-                &  $\begin{gathered}
-                    \Delta_{s} \Psi \\
-                    \Delta_{p_x} d_x  - \Delta_{p_y} d_y
-                   \end{gathered}$ \\
-    \sym A 2    & ---  & $d_z$
-                & $\Delta_{p_y} d_x  + \Delta_{p_x} d_y$\\
-    \sym B 1 & \numberedHexagon{$\Delta_f$}{-1}{1}{-1}{1}{-1}{1} & --- & --- \\
-    \sym B 2 & --- & --- & $\Delta_{f} d_z$ \\[0.5em] \hline \\
+                & $\Psi$ \\
+    \sym A 2    & ---  & $d_z$  \\
+    \sym B 1 & \numberedHexagon{$\Delta_f$}{-1}{1}{-1}{1}{-1}{1} & ---  \\
     \sym E 1 &
-    \hspace{0.15cm} % Fix spacing in the table
+    \hspace{0.2cm} % Fix spacing in the table
         $\begin{bmatrix}
-            \numberedHexagon{$\Delta_{p_x}$}{1}{-1}{-2}{-1}{1}{2} \\
+            \numberedHexagon{$\Delta_{p_x}$}{1}{-1}{-2}{-1}{1}{2} &
             \numberedHexagon{$\Delta_{p_y}$}{1}{1}{0}{-1}{-1}{0}
         \end{bmatrix} $
-    \hspace{0.15cm} % Fix spacing in the table
+    \hspace{0.2cm} % Fix spacing in the table
         &
         $\begin{bmatrix}
-            d_x \\
+            d_x &
             d_y
-        \end{bmatrix}$
-        & $\begin{bmatrix}
-            \Delta_{p_x} \\
-            \Delta_{p_y}
-        \end{bmatrix} d_z $  \\[6em]
+        \end{bmatrix}$ \\[3em]
     \sym E 2 &
-        $\left[
-            \begin{aligned}
-                \numberedHexagon{$\Delta_{d_{x^2-y^2}}$}{-1}{-1}{2}{-1}{-1}{2} \\
+        $\begin{bmatrix}
+            \hspace{0.03cm}
+            \numberedHexagon{$\Delta_{d_{x^2-y^2}}$}{-1}{-1}{2}{-1}{-1}{2}
+            \hspace{0.03cm}
+            &
+            \hspace{0.03cm}
             \numberedHexagon{$\Delta_{d_{xy}}$}{1}{-1}{0}{1}{-1}{0}
-            \end{aligned}
-        \right] $
-        & ---
-        & \hspace{0.5cm}
-        $\begin{gathered}
-            \begin{bmatrix}
-                \Delta_{d_{xy}} \\
-                \Delta_{d_{x^-y^2}}
-            \end{bmatrix} \Psi \\
-            \Delta_f \begin{bmatrix}
-                d_x \\
-                d_y
-            \end{bmatrix} \\
-            \begin{bmatrix}
-            \Delta_{p_y} d_x
-                - \Delta_{p_x} d_y \\
-            \Delta_{p_x} d_x
-            + \Delta_{p_y} d_y
-        \end{bmatrix}
-        \end{gathered}$
-        \hspace{0.5cm}
-            \\[6em] \hline
+            \hspace{0.03cm}
+        \end{bmatrix}$
+        & --- \\[3em] \hline
 \end{tabular}
     \caption{
         \captiontitle{Basis functions of irreducible representations}
@@ -364,8 +338,7 @@ presented in the following.
         The second column is the basis function in real space, for example, as
         the bond pairing on nearest neighbour bonds. The third column is the
         two-spin basis function, in terms of the typical superconducting psuedo-
-        vector formulation $(\Psi, \bvec d)$. The fourth column is the total
-        spatial and two-spin basis function, calculated as decribed in the text.}
+        vector formulation $(\Psi, \bvec d)$.}
     \label{tab:irrep_basis_fns}
 \end{table}