Quelle  note5.38.tex   Sprache: Latech

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\begin{document}

\title{Algebra 5.38}
\author{Michael Vaughan-Lee}
\date{June 2013}
\maketitle

Algebra 5.38 has$\allowbreak $ $\gcd (p-1,3)(p^{2}+3p+10)+p+6$ immediate
descendants of order $p^{7}$. Of these $\frac{1}{2}((p^{2}+3p+11)\gcd
(p-1,3)+1)$ come from one 4 parameter family of algebras, and $\frac{1}{2}%
(\gcd (p-1,3)(p^{2}+p+1)+5)$ come from another four parameter family. In
both cases we take the four parameters as entries in a $2\times 2$ matrix%
\[
A=\left( 
\begin{array}{cc}
x & y \\ 
z & t%
\end{array}%
\right) , 
\]%
and in both cases we consider the orbits of matrices $A$ of this form over GF%
$(p)$ under an action of the subgroup of GL$(2,p)$ consisting of
non-singular matrices of the form%
\[
\left( 
\begin{array}{ll}
\alpha & \beta \\ 
\beta & \alpha%
\end{array}%
\right) \text{ or }\left( 
\begin{array}{ll}
\alpha & \beta \\ 
-\beta & -\alpha%
\end{array}%
\right) . 
\]

In the first case two matrices $A$ and $B$ give isomorphic Lie rings if and
only if%
\[
B=\left( 
\begin{array}{ll}
\alpha  & \beta  \\ 
\beta  & \alpha 
\end{array}%
\right) A\left( 
\begin{array}{ll}
(\alpha ^{4}-\beta ^{4}) & 2\alpha \beta (\alpha ^{2}-\beta ^{2}) \\ 
2\alpha \beta (\alpha ^{2}-\beta ^{2}) & \alpha ^{4}-\beta ^{4}%
\end{array}%
\right) ^{-1}
\]%
or 
\[
B=\left( 
\begin{array}{ll}
\alpha  & \beta  \\ 
-\beta  & -\alpha 
\end{array}%
\right) A\left( 
\begin{array}{ll}
-(\alpha ^{4}-\beta ^{4}) & -2\alpha \beta (\alpha ^{2}-\beta ^{2}) \\ 
2\alpha \beta (\alpha ^{2}-\beta ^{2}) & \alpha ^{4}-\beta ^{4}%
\end{array}%
\right) ^{-1}
\]%
for some $\alpha ,\beta $. In the second case, two matrices $A$ and $B$ give
isomorphic Lie rings if and only if%
\[
B=\left( 
\begin{array}{ll}
\alpha  & \beta  \\ 
\omega \beta  & \alpha 
\end{array}%
\right) A\left( 
\begin{array}{ll}
\alpha ^{4}-\omega ^{2}\beta ^{4} & 2\alpha \beta (\alpha ^{2}-\omega \beta
^{2}) \\ 
2\omega \alpha \beta (\alpha ^{2}-\omega \beta ^{2}) & \alpha ^{4}-\omega
^{2}\beta ^{4}%
\end{array}%
\right) ^{-1}
\]%
or 
\[
B=\left( 
\begin{array}{ll}
\alpha  & \beta  \\ 
-\omega \beta  & -\alpha 
\end{array}%
\right) A\left( 
\begin{array}{ll}
-(\alpha ^{4}-\omega ^{2}\beta ^{4}) & -2\alpha \beta (\alpha ^{2}-\omega
\beta ^{2}) \\ 
2\omega \alpha \beta (\alpha ^{2}-\omega \beta ^{2}) & \alpha ^{4}-\omega
^{2}\beta ^{4}%
\end{array}%
\right) ^{-1}
\]%
for some $\alpha ,\beta $.

A simple loop over all possible $A$ and all possible $\alpha ,\beta $ can
find representatives for the orbits. You can shorten the search slightly by
noting that in both cases if we take $\alpha =-1$, $\beta =0$ then $B=-A$.

\end{document}