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Commit 21fe448a authored by Luke Naylor's avatar Luke Naylor
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Complete proof of numerical condition equivalence in rank 0 case

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......@@ -162,11 +162,10 @@ are equivalent to the following more numerical conditions:
\end{enumerate}
\end{lemma}
\begin{proof}
\begin{proof}[Proof for $\chern_0(v)>0$ case.]
Let $u,v$ be Chern characters with
$\Delta(u),\Delta(v) \geq 0$, and $v$ has positive rank.
For the forwards implication, assume that the suppositions of the Lemma are
satisfied. Let $Q$ be the point on $\Theta_v^-$ (above $P$) where $u$ is a
pseudo-semistabiliser of $v$.
......@@ -244,10 +243,47 @@ Therefore, it's also a pseudo-semistabiliser further along the circle at $Q$
(supposition a).
Finally, consequence 4 along with $P$ being to the left of $V_u$ implies
$\nu_P(u) > 0$ giving supposition b.
\end{proof}
\begin{sagesilent}
from rank_zero_case_curves import pseudo_semistab_char_curves_rank_zero
\end{sagesilent}
\begin{figure}
\centering
\sageplot[width=\textwidth]{pseudo_semistab_char_curves_rank_zero}
\caption{characteristic curves configuration for pseudo-semistabiliser of $v$
with rank 0 destabilising `downwards'}
\label{fig:hyperbol-intersection-rank-zero}
\end{figure}
\begin{proof}[Proof for $\chern_0(v)=0$ case.]
Let $u,v$ be Chern characters with
$\Delta(u),\Delta(v) \geq 0$, and $\chern_0(v)=0$ but $\chern_1(v)>0$.
So $\Theta_v^-$ is the vertical line at $\beta = \beta_{-}(v)$, and
$\mu(v) = +\infty$.
For the forward implication, assume suppositions a and b hold.
Let $Q$ be the point above $P$ on $\Theta_v^-$ where $u$ is a
pseudo-semistabiliser of $v$. So $\Theta_u$ intersects $\Theta_v^-$ at $Q$.
Suppose, seeking a contradiction that $\chern_0(u)=0$,
then $\Theta_u = \Theta_u^-$ is also a vertical line,
and must then be the same line as $\Theta_v^-$ to intersect $Q$.
This would imply $\QQ u = \QQ v$ and then $u$ would not destabilise $v$ at any
stability condition.
So we must have either $\chern_0(u) < 0$, in which case $\Theta_u^+$ is the
branch of $\Theta_u$ going through $Q$; or $\chern_0(u) > 0$, in which it is
$\Theta_u^-$ instead.
The latter case is the only one which could satisfy supposition b, about $u$
destabilising $v$ going `down' $\Theta_v^-$.
Which then forces the configuration of characteristic curves shown in Figure
\ref{fig:hyperbol-intersection-rank-zero}.
The positions of the characteristic curves ensures the numerical conditions 1, 2
and 5. The other conditions follow from the definition of $u$ being a
pseudo-semistabiliser of $v$.
The case with rank 0 can be handled the same way.
% TODO expand this case too
Conversely, suppose that the numerical conditions 1-5 are satisfied,
then this forces the configuration of characteristic curves shown in Figure
\ref{fig:hyperbol-intersection-rank-zero}.
This ensures that $u$ is a pseudo-semistabiliser of $v$ at $u$ destabilising
going down $\Theta_v^-$.
\end{proof}
\begin{remark}
......@@ -295,7 +331,7 @@ The case with rank 0 can be handled the same way.
\section{The Problem: Finding Pseudo-walls}
As hinted in the introduction (\ref{sec:intro}), the main motivation of the
As hinted in the introduction to this Part \ref{part:fin-walls}, the main motivation of the
results in this article are not only the bounds on pseudo-semistabiliser
ranks;
but also applications for finding a list (comprehensive or subset) of
......
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