diff --git a/main.tex b/main.tex
index 727da0b4fb21298ea58680d313e8141c72a97116..f73822987e690704c35d31f3547cbec429a49b8f 100644
--- a/main.tex
+++ b/main.tex
@@ -56,6 +56,16 @@ $0 \leq \chern^\beta_1(E) \leq \chern^\beta_1(F)$.
 Finally, there's a condition ensuring that the radius of the circular wall is
 strictly positive: $\chern^\beta_2(E) > 0$.
 
+For any fixed $\chern_0(E)$, the inequality
+$0 \leq \chern^{\beta_{-}}_1(E) \leq \chern^{\beta_{-}}_1(F)$,
+allows us to bound $\chern_1(E)$. Then, the other inequalities allow us to
+bound $\chern_2(E)$. The final part to showing the finiteness of pseudowalls
+would be bounding $\chern_0(E)$. This has been hinted at in [ref] and done
+explicitly by Benjamin Schmidt within a computer program which computes
+pseudowalls. Here we discuss these bounds in more detail, along with the methods
+used, followed by refinements on them which give explicit formulae for tighter
+bounds on $\chern_0(E)$ of potential destabilizers $E$ of $F$.
+
 
 \section{Section 1}