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  1. We introduce the notions of symmetric and symmetrizable representations of SL 2 ⁡<#comment/> ( Z ) {\operatorname {SL}_2(\mathbb {Z})} . The linear representations of SL 2 ⁡<#comment/> ( Z ) {\operatorname {SL}_2(\mathbb {Z})} arising from modular tensor categories are symmetric and have congruence kernel. Conversely, one may also reconstruct modular data from finite-dimensional symmetric, congruence representations of SL 2 ⁡<#comment/> ( Z ) {\operatorname {SL}_2(\mathbb {Z})} . By investigating a Z / 2 Z \mathbb {Z}/2\mathbb {Z} -symmetry of some Weil representations at prime power levels, we prove that all finite-dimensional congruence representations of SL 2 ⁡<#comment/> ( Z ) {\operatorname {SL}_2(\mathbb {Z})} are symmetrizable. We also provide examples of unsymmetrizable noncongruence representations of SL 2 ⁡<#comment/> ( Z ) {\operatorname {SL}_2(\mathbb {Z})} that are subrepresentations of a symmetric one. 
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  2. Let V V be a vertex operator superalgebra with the natural order 2 automorphism σ \sigma . Under suitable conditions on V V , the σ \sigma -fixed subspace V 0 ¯ V_{\bar 0} is a vertex operator algebra and the V 0 ¯ V_{\bar 0} -module category C V 0 ¯ \mathcal {C}_{V_{\bar 0}} is a modular tensor category. In this paper, we prove that C V 0 ¯ \mathcal {C}_{V_{\bar 0}} is a fermionic modular tensor category and the Müger centralizer C V 0 ¯ 0 \mathcal {C}_{V_{\bar 0}}^0 of the fermion in C V 0 ¯ \mathcal {C}_{V_{\bar 0}} is generated by the irreducible V 0 ¯ V_{\bar 0} -submodules of the V V -modules. In particular, C V 0 ¯ 0 \mathcal {C}_{V_{\bar 0}}^0 is a super-modular tensor category and C V 0 ¯ \mathcal {C}_{V_{\bar 0}} is a minimal modular extension of C V 0 ¯ 0 \mathcal {C}_{V_{\bar 0}}^0 . We provide a construction of a vertex operator superalgebra V l V^l for each positive integer l l such that C ( V l ) 0 ¯ \mathcal {C}_{{(V^l)_{\bar 0}}} is a minimal modular extension of C V 0 ¯ 0 \mathcal {C}_{V_{\bar 0}}^0 . We prove that these modular tensor categories C ( V l ) 0 ¯ \mathcal {C}_{{(V^l)_{\bar 0}}} are uniquely determined, up to equivalence, by the congruence class of l l modulo 16. 
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