From 401a9233b93e98a87237c652abdcde3b3fe720d3 Mon Sep 17 00:00:00 2001 From: Maria Marchwicka Date: Sat, 8 Jun 2019 14:14:33 +0200 Subject: [PATCH] matrix slice knot --- lectures_on_knot_theory.tex | 72 ++++++++----------------------------- 1 file changed, 14 insertions(+), 58 deletions(-) diff --git a/lectures_on_knot_theory.tex b/lectures_on_knot_theory.tex index 48b7937..02cf441 100644 --- a/lectures_on_knot_theory.tex +++ b/lectures_on_knot_theory.tex @@ -1067,48 +1067,11 @@ $. Suppose $g(K) = 0$ ($K$ is slice). Then $H_1(\Sigma, \mathbb{Z}) \cong H_1(Y, \mathbb{Z})$. Let $g_{\Sigma}$ be the genus of $\Sigma$, $\dim H_1(Y, \mathbb{Z}) = 2g_{\Sigma}$. Then the Seifert form $V$ on 4\\ ?????\\ has a subspace of dimension $g_{\Sigma}$ on which it is zero: -\[ -V = -\begin{pmatrix} - \begin{array}{c|c} - 0 & * \\ - \hline - * & * - \end{array} -\end{pmatrix} -\] -\begin{align*} - \newcommand*{\AddLeft}[1]{% - \vadjust{% - \vbox to 0pt{% - \vss - \llap{$% - {#1}\left\{ - \vphantom{ - \begin{matrix}1\\\vdots\\0\end{matrix} - } - \right.\kern-\nulldelimiterspace - \kern0.5em - $}% - \kern0pt - }% - }% - } -V = \qquad -\begin{pmatrix} - 0 & \cdots & 0 & * & \cdots & * \\ - \vdots & & \vdots & \vdots & &\vdots \\ - 0 & \cdots & 0 & * & \cdots & * - \AddLeft{g_{\Sigma}}\\ - * & \cdots & * & * & \cdots & * \\ - \vdots & & \vdots & \vdots & &\vdots \\ - * & \cdots & * & * & \cdots & * - \end{pmatrix}_{2g_{\Sigma} \times 2g_{\Sigma}} -\end{align*} \begin{align*} -\newcommand\coolover[2]{\mathrlap{\smash{\overbrace{\phantom{% - \begin{matrix} #2 \end{matrix}}}^{\mbox{$#1$}}}}#2} +\newcommand\coolover[2]% + {\mathrlap{\smash{\overbrace{\phantom{% + \begin{matrix} #2 \end{matrix}}}^{\mbox{$#1$}}}}#2} \newcommand\coolunder[2]{\mathrlap{\smash{\underbrace{\phantom{% \begin{matrix} #2 \end{matrix}}}_{\mbox{$#1$}}}}#2} \newcommand\coolleftbrace[2]{% @@ -1120,25 +1083,18 @@ V = \qquad \overbrace{XYZ}^{\mbox{$R$}}\\ \\ \\ \\ \\ \\ \underbrace{pqr}_{\mbox{$S$}} \end{matrix}}% + V = \begin{matrix}% matrix for left braces -\vphantom{a}\\ - \coolleftbrace{A}{e \\ y\\ y}\\ - \coolleftbrace{B}{y \\i \\ m} + \coolleftbrace{g_{\Sigma}}{ \\ \\ \\} + \\ \\ \\ \\ \end{matrix}% -\begin{bmatrix} -a & \coolover{R}{b & c & d} & x & \coolover{Z}{x & x}\\ - e & f & g & h & x & x & x \\ - y & y & y & y & y & y & y \\ - y & y & y & y & y & y & y \\ - y & y & y & y & y & y & y \\ - i & j & k & l & x & x & x \\ - m & \coolunder{S}{n & o} & \coolunder{W}{p & x & x} & x -\end{bmatrix}% -\begin{matrix}% matrix for right braces - \coolrightbrace{x \\ x \\ y\\ y}{T}\\ - \coolrightbrace{y \\ y \\ x }{U} -\end{matrix} +\begin{pmatrix} + \coolover{g_{\Sigma}}{0 & \dots & 0 } & * & \dots & *\\ + \sdots & & \sdots & \sdots & & \sdots \\ + 0 & \dots & 0 & * & \dots & *\\ + * & \dots & * & * & \dots & *\\ + \sdots & & \sdots & \sdots & & \sdots \\ + * & \dots & * & * & \dots & * + \end{pmatrix}_{2g_{\Sigma} \times 2g_{\Sigma}} \end{align*} - - \end{document}