From 3595122db902d676be3d14663eddf99231c0ab3e Mon Sep 17 00:00:00 2001 From: Luke Naylor <l.naylor@sms.ed.ac.uk> Date: Thu, 20 Jun 2024 16:10:10 +0100 Subject: [PATCH] Move pseudo semistab charact curve material to main content --- tex/characteristic-curves.tex | 128 ---------------------------------- tex/content.tex | 128 ++++++++++++++++++++++++++++++++++ 2 files changed, 128 insertions(+), 128 deletions(-) diff --git a/tex/characteristic-curves.tex b/tex/characteristic-curves.tex index c3ba84e..e3a9a00 100644 --- a/tex/characteristic-curves.tex +++ b/tex/characteristic-curves.tex @@ -212,131 +212,3 @@ This fact, along with the hindsight knowledge that non-vertical walls are circles with centers on the $\beta$-axis, gives an alternative view to see that the circular walls must be nested and non-intersecting. -\subsection{Characteristic Curves for Pseudo-semistabilizers} - -These characteristic curves introduced are convenient tools to think about the -numerical conditions that can be used to test for pseudo-semistabilizers, and -for solutions to the problems -(\ref{problem:problem-statement-1},\ref{problem:problem-statement-2}) -tackled in this article (to be introduced later). -In particular, problem (\ref{problem:problem-statement-1}) will be translated to -a list of numerical inequalities on it's solutions $u$. -% ref to appropriate Lemma when it's written - -The next Lemma is a key to making this translation and revolves around the -geometry and configuration of the characteristic curves involved in a -semistabilizing sequence. - -\begin{lemma}[Numerical tests for left-wall pseudo-semistabilizers] -\label{lem:pseudo_wall_numerical_tests} -Let $v$ and $u$ be Chern characters with $\Delta(v), -\Delta(u)\geq 0$, and $v$ has non-negative rank (and $\chern_1(v)>0$ if rank 0). -Let $P$ be a point on $\Theta_v^-$. - -\noindent -The following conditions: -\begin{enumerate} -\item $u$ is a pseudo-semistabilizer of $v$ at some point on $\Theta_v^-$ above - $P$ -\item $u$ destabilizes $v$ going `inwards', that is, - $\nu_{\alpha,\beta}(u)<\nu_{\alpha,\beta}(v)$ outside the pseudo-wall, and - $\nu_{\alpha,\beta}(u)>\nu_{\alpha,\beta}(v)$ inside. -\end{enumerate} - -\noindent -are equivalent to the following more numerical conditions: -\begin{enumerate} - \item $u$ has positive rank - \item $\beta(P)<\mu(u)<\mu(v)$, i.e. $V_u$ is strictly between $P$ and $V_v$. - \item $\chern_1^{\beta(P)}(u) \leq \chern_1^{\beta(P)}(v)$, $\Delta(v-u) \geq 0$ - \item $\chern_2^{P}(u)>0$ -\end{enumerate} -\end{lemma} - -\begin{proof} -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-semistabilizer of $v$. -Firstly, consequence 3 is part of the definition for $u$ being a -pseudo-semistabilizer at a point with same $\beta$ value of $P$ (since the -pseudo-wall surrounds $P$). -If $u$ were to have 0 rank, it's tilt slope would be decreasing as $\beta$ -increases, contradicting supposition b. So $u$ must have strictly non-zero rank, -and we can consider it's characteristic curves (or that of $-u$ in case of -negative rank). -$\nu_Q(v)=0$, and hence $\nu_Q(u)=0$ too. This means that $\Theta_{\pm u}$ must -intersect $\Theta_v^-$ at $Q$. Considering the shapes of the hyperbolae alone, -there are 3 distinct ways that they can intersect, as illustrated in Fig -\ref{fig:hyperbol-intersection}. These cases are distinguished by whether it is -the left, or the right branch of $\Theta_u$ involved, as well as the positions -of the base. However, considering supposition b, only case 3 (green in -figure) is possible. This is because we need $\nu_{P}(u)>0$ (or $\nu_{P}(-u)>0$ in -case 1 involving $\Theta_u^+$), to satisfy supposition b. -Recalling how the sign of $\nu_{\alpha,\beta}(\pm u)$ changes (illustrated in -Fig \ref{fig:charact_curves_vis}), we can eliminate cases 1 and 2. - -\begin{sagesilent} -from characteristic_curves import \ -hyperbola_intersection_plot, \ -correct_hyperbola_intersection_plot -\end{sagesilent} - -\begin{figure} -\begin{subfigure}[t]{0.48\textwidth} - \centering - \sageplot[width=\textwidth]{hyperbola_intersection_plot()} - \caption{Three ways the characteristic hyperbola for $u$ can intersect the left - branch of the characteristic hyperbola for $v$} - \label{fig:hyperbol-intersection} -\end{subfigure} -\hfill -\begin{subfigure}[t]{0.48\textwidth} - \centering - \sageplot[width=\textwidth]{correct_hyperbola_intersection_plot()} - \caption{Closer look at characteristic curves for valid case} - \label{fig:correct-hyperbol-intersection} -\end{subfigure} -\end{figure} - -Fixing attention on the only possible case (2), illustrated in Fig -\ref{fig:correct-hyperbol-intersection}. -$P$ is on the left of $V_{\pm u}$ (first part of consequence 2), so $u$ must -have positive rank (consequence 1) -to ensure that $\chern_1^{\beta(P)} \geq 0$ (since the pseudo-wall passed over -$P$). -Furthermore, $P$ being on the left of $V_u$ implies -$\chern_1^{\beta{P}}(u) \geq 0$, -and therefore $\chern_2^{P}(u) > 0$ (consequence 4) to satisfy supposition b. -Next considering the way the hyperbolae intersect, we must have $\Theta_u^-$ taking a -base-point to the right $\Theta_v$, but then, further up, crossing over to the -left side. The latter fact implies that the assymptote for $\Theta_u^-$ must be -to the left of the one for $\Theta_v^-$. Given that they are parallel and -intersect the $\beta$-axis at $\beta=\mu(u)$ and $\beta=\mu(v)$ respectively. We -must have $\mu(u)<\mu(v)$ (second part of consequence 2), -that is, $V_u$ is strictly to the left of $V_v$. - - -Conversely, suppose that the consequences 1-4 are satisfied. Consequence 2 -implies that the assymptote for $\Theta_u^-$ is to the left of $\Theta_v^-$. -Consequence 4, along with $\beta(P)<\mu(u)$, implies that $P$ must be in the -region left of $\Theta_u^-$. These two facts imply that $\Theta_u^-$ is to the -right of $\Theta_v^-$ at $\alpha=\alpha(P)$, but crosses to the left side as -$\alpha \to +\infty$, intersection at some point $Q$ above $P$. -This implies that the characteristic curves for $u$ and $v$ are in the -configuration illustrated in Fig \ref{fig:correct-hyperbol-intersection}. -We then have $\nu(u)=\nu(v)$ along a circle to the left of $V_u$ reaching it's -apex at $Q$, and encircling $P$. This along with consequence 3 implies that $u$ -is a pseudo-semistabilizer at the point on the circle with $\beta=\beta(P)$. -Therefore, it's also a pseudo-semistabilizer 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. - -The case with rank 0 can be handled the same way. - -\end{proof} - diff --git a/tex/content.tex b/tex/content.tex index df56379..153cb8f 100644 --- a/tex/content.tex +++ b/tex/content.tex @@ -1,3 +1,131 @@ +\subsection{Characteristic Curves for Pseudo-semistabilizers} + +These characteristic curves introduced are convenient tools to think about the +numerical conditions that can be used to test for pseudo-semistabilizers, and +for solutions to the problems +(\ref{problem:problem-statement-1},\ref{problem:problem-statement-2}) +tackled in this article (to be introduced later). +In particular, problem (\ref{problem:problem-statement-1}) will be translated to +a list of numerical inequalities on it's solutions $u$. +% ref to appropriate Lemma when it's written + +The next Lemma is a key to making this translation and revolves around the +geometry and configuration of the characteristic curves involved in a +semistabilizing sequence. + +\begin{lemma}[Numerical tests for left-wall pseudo-semistabilizers] +\label{lem:pseudo_wall_numerical_tests} +Let $v$ and $u$ be Chern characters with $\Delta(v), +\Delta(u)\geq 0$, and $v$ has non-negative rank (and $\chern_1(v)>0$ if rank 0). +Let $P$ be a point on $\Theta_v^-$. + +\noindent +The following conditions: +\begin{enumerate} +\item $u$ is a pseudo-semistabilizer of $v$ at some point on $\Theta_v^-$ above + $P$ +\item $u$ destabilizes $v$ going `inwards', that is, + $\nu_{\alpha,\beta}(u)<\nu_{\alpha,\beta}(v)$ outside the pseudo-wall, and + $\nu_{\alpha,\beta}(u)>\nu_{\alpha,\beta}(v)$ inside. +\end{enumerate} + +\noindent +are equivalent to the following more numerical conditions: +\begin{enumerate} + \item $u$ has positive rank + \item $\beta(P)<\mu(u)<\mu(v)$, i.e. $V_u$ is strictly between $P$ and $V_v$. + \item $\chern_1^{\beta(P)}(u) \leq \chern_1^{\beta(P)}(v)$, $\Delta(v-u) \geq 0$ + \item $\chern_2^{P}(u)>0$ +\end{enumerate} +\end{lemma} + +\begin{proof} +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-semistabilizer of $v$. +Firstly, consequence 3 is part of the definition for $u$ being a +pseudo-semistabilizer at a point with same $\beta$ value of $P$ (since the +pseudo-wall surrounds $P$). +If $u$ were to have 0 rank, it's tilt slope would be decreasing as $\beta$ +increases, contradicting supposition b. So $u$ must have strictly non-zero rank, +and we can consider it's characteristic curves (or that of $-u$ in case of +negative rank). +$\nu_Q(v)=0$, and hence $\nu_Q(u)=0$ too. This means that $\Theta_{\pm u}$ must +intersect $\Theta_v^-$ at $Q$. Considering the shapes of the hyperbolae alone, +there are 3 distinct ways that they can intersect, as illustrated in Fig +\ref{fig:hyperbol-intersection}. These cases are distinguished by whether it is +the left, or the right branch of $\Theta_u$ involved, as well as the positions +of the base. However, considering supposition b, only case 3 (green in +figure) is possible. This is because we need $\nu_{P}(u)>0$ (or $\nu_{P}(-u)>0$ in +case 1 involving $\Theta_u^+$), to satisfy supposition b. +Recalling how the sign of $\nu_{\alpha,\beta}(\pm u)$ changes (illustrated in +Fig \ref{fig:charact_curves_vis}), we can eliminate cases 1 and 2. + +\begin{sagesilent} +from characteristic_curves import \ +hyperbola_intersection_plot, \ +correct_hyperbola_intersection_plot +\end{sagesilent} + +\begin{figure} +\begin{subfigure}[t]{0.48\textwidth} + \centering + \sageplot[width=\textwidth]{hyperbola_intersection_plot()} + \caption{Three ways the characteristic hyperbola for $u$ can intersect the left + branch of the characteristic hyperbola for $v$} + \label{fig:hyperbol-intersection} +\end{subfigure} +\hfill +\begin{subfigure}[t]{0.48\textwidth} + \centering + \sageplot[width=\textwidth]{correct_hyperbola_intersection_plot()} + \caption{Closer look at characteristic curves for valid case} + \label{fig:correct-hyperbol-intersection} +\end{subfigure} +\end{figure} + +Fixing attention on the only possible case (2), illustrated in Fig +\ref{fig:correct-hyperbol-intersection}. +$P$ is on the left of $V_{\pm u}$ (first part of consequence 2), so $u$ must +have positive rank (consequence 1) +to ensure that $\chern_1^{\beta(P)} \geq 0$ (since the pseudo-wall passed over +$P$). +Furthermore, $P$ being on the left of $V_u$ implies +$\chern_1^{\beta{P}}(u) \geq 0$, +and therefore $\chern_2^{P}(u) > 0$ (consequence 4) to satisfy supposition b. +Next considering the way the hyperbolae intersect, we must have $\Theta_u^-$ taking a +base-point to the right $\Theta_v$, but then, further up, crossing over to the +left side. The latter fact implies that the assymptote for $\Theta_u^-$ must be +to the left of the one for $\Theta_v^-$. Given that they are parallel and +intersect the $\beta$-axis at $\beta=\mu(u)$ and $\beta=\mu(v)$ respectively. We +must have $\mu(u)<\mu(v)$ (second part of consequence 2), +that is, $V_u$ is strictly to the left of $V_v$. + + +Conversely, suppose that the consequences 1-4 are satisfied. Consequence 2 +implies that the assymptote for $\Theta_u^-$ is to the left of $\Theta_v^-$. +Consequence 4, along with $\beta(P)<\mu(u)$, implies that $P$ must be in the +region left of $\Theta_u^-$. These two facts imply that $\Theta_u^-$ is to the +right of $\Theta_v^-$ at $\alpha=\alpha(P)$, but crosses to the left side as +$\alpha \to +\infty$, intersection at some point $Q$ above $P$. +This implies that the characteristic curves for $u$ and $v$ are in the +configuration illustrated in Fig \ref{fig:correct-hyperbol-intersection}. +We then have $\nu(u)=\nu(v)$ along a circle to the left of $V_u$ reaching it's +apex at $Q$, and encircling $P$. This along with consequence 3 implies that $u$ +is a pseudo-semistabilizer at the point on the circle with $\beta=\beta(P)$. +Therefore, it's also a pseudo-semistabilizer 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. + +The case with rank 0 can be handled the same way. + +\end{proof} + \section{The Problem: Finding Pseudo-walls} As hinted in the introduction (\ref{sec:intro}), the main motivation of the -- GitLab