This is an optional argument for the schurRing and symmetricRing functions. When the exterior or symmetric powers of a symmetric function g are computed, the result depends on whether g is interpreted as a virtual representation of a general linear, symmetric, symplectic, or orthogonal group. The option GroupActing specifies the interpretation to be considered. Its possible values are "GL" (the default), "Sn", "SL", "Sp", "O", and "RatGL".
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The first example computes the decomposition of \Lambda^3(Sym^2(V)) into irreducible GL(V)-representations, while the second one computes the second symmetric power of the sign representation of the symmetric group S_2.
Multiplication differs sharply between the "GL" and "Sn" interpretations. Under "GL", the product is the Littlewood-Richardson tensor product of polynomial representations, which is degree-additive in the partitions. Under "Sn", multiplication is the ordinary tensor product of characters of a single symmetric group, so only partitions of the same size may be multiplied, and the product is expanded in the Kronecker coefficients:
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The values "Sp" and "O" select the stable (universal) character ring of the symplectic and orthogonal groups, respectively. The basis elements are indexed by partitions, with sp_\lambda (respectively o_\lambda) standing for the irreducible symplectic (respectively orthogonal) character associated to \lambda. Multiplication in these rings is the Newell-Littlewood product, implemented by conversion to the Schur basis via Koike's branching formulas and back:
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Exterior and symmetric powers are likewise reinterpreted. In the orthogonal ring, exterior powers of the second fundamental character mix several Newell-Littlewood terms:
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Setting GroupActing => "SL" forces the top-row reduction s_\lambda = s_{(\lambda_1 - \lambda_n, \ldots, \lambda_{n-1} - \lambda_n)}, reflecting the fact that the determinant representation is trivial in SL. Long partitions collapse accordingly:
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Finally, GroupActing => "RatGL" produces the ring of rational (mixed) polynomial representations of GL(V), whose characters are indexed by pairs of partitions (bipartitions), and whose tensor product is again a Littlewood-Richardson-style rule:
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Stable rings (no dimension specified) allow arbitrarily many parts in the partition labels; a concrete dimension can be supplied to restrict the partitions and to model a finite-dimensional group.
The object GroupActing is a symbol.
The source of this document is in /build/reproducible-path/macaulay2-1.26.05+ds/M2/Macaulay2/packages/SchurRings.m2:7927:0.