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NONREALIZABILITY OF CERTAIN REPRESENTATIONS IN FUSION SYSTEMS

Published online by Cambridge University Press:  11 April 2023

BOB OLIVER*
Affiliation:
Université Sorbonne Paris Nord, LAGA, UMR 7539 du CNRS, 99, Av. J.-B. Clément, Villetaneuse 93430, France
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Abstract

For a finite abelian p-group A and a subgroup $\Gamma \le \operatorname {\mathrm {Aut}}(A)$, we say that the pair $(\Gamma ,A)$ is fusion realizable if there is a saturated fusion system ${\mathcal {F}}$ over a finite p-group $S\ge A$ such that $C_S(A)=A$, $\operatorname {\mathrm {Aut}}_{{\mathcal {F}}}(A)=\Gamma $ as subgroups of $\operatorname {\mathrm {Aut}}(A)$, and . In this paper, we develop tools to show that certain representations are not fusion realizable in this sense. For example, we show, for $p=2$ or $3$ and $\Gamma $ one of the Mathieu groups, that the only ${\mathbb {F}}_p\Gamma $-modules that are fusion realizable (up to extensions by trivial modules) are the Todd modules and in some cases their duals.

Information

Type
Research Article
Copyright
© The Author(s), 2023. Published by Cambridge University Press on behalf of Australian Mathematical Publishing Association Inc.
Figure 0

Table 1 The number of orbits in the action on X by each element of order $2$ or $3$ in $\Gamma $. For example, a ${\mathbf {2B}}$-element in $M_{12}$ acts with four orbits of length $2$ and four fixed points.

Figure 1

Table 2 In all cases, $A_0$ is an $\mathbb {F}_2\Gamma $-module such that $C_{A_0}(\Gamma )=0$ and $[\Gamma ,A_0]=A_0$, and the characters are taken with respect to $\mathbb {F}_2$. The bounds for ${\mathscr {J}}_{A_0}(\tau )$ all follow from Lemmas 3.1(a) and A.1(a).

Figure 2

Table 3 In all cases, $A_0$ is an $\mathbb {F}_3\Gamma $-module such that $C_{A_0}(\Gamma )=0$ and $[\Gamma ,A_0]=A_0$, and the characters are taken with respect to $\mathbb {F}_3$. Thus when $\Gamma \cong 2M_{22}$, the character values for the simple 10-dimensional $\overline {\mathbb {F}}_3\Gamma $-module are doubled here since it can only be realized over $\mathbb {F}_9$. When $\Gamma \cong M_{11}$, the bounds for ${\mathscr {J}}_{A_0}(\tau )$ apply only when $A_0$ is not the $10$-dimensional permutation module. The bounds for ${\mathscr {J}}_{A_0}(\tau )$ all follow from Lemmas 3.1 and A.1(c), except when $\Gamma \cong M_{11}$ or $2M_{12}$ where Lemma A.1(d) is used.

Figure 3

Table 4 Let $S=A\langle {s,t}\rangle $, where $A=\langle {v_1,v_2,v_3}\rangle \cong C_{2^n}\times C_{2^n}\times C_{2^n}$, the elements s and t act on A as described in the table, and also $t^2=1$ and $s^4\in \langle {v_1v_3}\rangle $. Set $T=\operatorname {\mathrm {Aut}}_S(A)=\langle {c_s,c_t}\rangle \cong D_8$.

Figure 4

Table 5 Centralizers and commutators involving some of the abelian subgroups $H\le \langle {s,t}\rangle $. Here, $\varepsilon =2^{n-1}$ and $\delta =2^{n-2}$.

Figure 5

Table 6 Commutators $[g,x]=g(x)-x$ for $g\in T$ and $x \in $Gol$_{\mathbf {23}}$. The first six elements in the top row form a basis for $C_{\boldsymbol{ {Gol}}_{\mathbf {22}}} (\mathfrak {tr}_{h_{1}} )$, and together with the seventh they form a basis for $C_{\boldsymbol{ {Gol}}_{\mathbf {23}}} (\mathfrak {tr}_{h_{1}} )$.

Figure 6

Table 7 The classes of these four elements x form a basis for $\boldsymbol{ {Gol}}_{\mathbf {\mathit {n}}}/C_{\boldsymbol{ {Gol}}_{\mathbf {\mathit {n}}}}(\mathfrak {tr}_{h_{1}} )$.