Documentation

TauCeti.Algebra.Lie.Orthogonal.TypeD.SpinCarrier.Basic

The full-weight type-D spin carrier #

For 4 ≤ n, this file specializes the type-Dₙ spin representation to the canonical split quadratic space M* × M, where M = Fin n → ℚ. Its exterior coordinate lattice has basis indexed by the sign sets Finset (Fin n) and is stable under the type-D Serre Kostant form. The corresponding spin weights span the full simply connected character lattice.

These data are fed into the Kostant toral-closure construction. The result is an explicit affine group scheme over ℤ, cut out inside GL_(2^n) by the largest Hopf ideal killed by the numbered simple-root subgroups and the represented rank-n split torus. In particular, the construction uses the full spin module rather than one half-spin summand, so its weights see both spinor cosets of the type-D root lattice.

Those data are then carried onto matrix-valued points: the numbered root subgroups and the weight torus become homomorphisms into TauCeti.TypeDSpinCarrier.points, and conjugating one by the other rescales its parameter through a character. That character is named: it is the positive or negative i-th simple root of TauCeti.DynkinType.simplyConnectedRootDatum at TauCeti.DynkinType.D n, the uniform pinned datum a consumer reaches holding only a Dynkin type. That naming is what makes the carrier's pinning conventions statable without reference to its 2 ^ n-dimensional spin realization.

No smoothness, reductivity, maximality of the torus, or identification of the carrier's whole root datum is asserted here: the equations below concern the simple root characters alone, and exhibit neither a Borel subgroup nor a root subgroup for a non-simple root. Those are subsequent steps in the pinned Chevalley--Demazure construction.

Main declarations #

Main results #

References #

The carrier API follows the formal template of TauCeti.Algebra.Lie.E6.Minuscule.GroupScheme and TauCeti.Algebra.Lie.Symplectic.StandardCarrier.Scheme, and the pinning equations below follow that of TauCeti.Algebra.Lie.Symplectic.StandardCarrier.RootDatum; the split spin representation, exterior lattice, and type-D weights are specific to this construction. This advances Layer 9, "The Chevalley--Demazure construction", of the ReductiveGroups roadmap and supplies the type-D carrier required by milestone L0 of the CFSGStatement roadmap.

The split spin representation and its lattice #

@[reducible, inline]

The canonical split polarization used by the type-Dₙ spin carrier.

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    The coordinate basis of the first isotropic summand in the split polarization.

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      The rational spin representation of the type-Dₙ Serre presentation, extended to its universal enveloping algebra.

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        The integral exterior coordinate lattice in the split spin module.

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          The dimension of the full spin module, expressed as the cardinality of its exterior basis.

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            The exterior coordinate basis, reindexed by a finite ordinal for the general-linear carrier.

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              @[reducible, inline]
              noncomputable abbrev TauCeti.TypeDSpinCarrier.signSet (n : ℕ) (i : Fin (dimension n)) :

              The sign set represented by a finite-ordinal spin-basis index.

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                @[reducible, inline]
                noncomputable abbrev TauCeti.TypeDSpinCarrier.basisWeight (n : ℕ) (i : Fin (dimension n)) :
                Fin n → ℤ

                The simply connected type-Dₙ weight of a finite-ordinal spin-basis vector.

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                  @[simp]

                  A reindexed lattice-basis vector is the exterior basis vector of its sign set.

                  Every represented numbered root generator is nilpotent.

                  Every represented numbered root generator has nilpotency class at most two: it squares to zero.

                  The represented positive and negative simple generators at a common type-D node, together with the represented Cartan generator, form an sl_2 triple.

                  The type-D Serre Kostant form preserves the split exterior coordinate lattice.

                  The generic Kostant form for the numbered type-D generators preserves the split exterior coordinate lattice.

                  Every finite-ordinal exterior basis vector has its named integral type-D spin weight.

                  The weights of the full spin basis span the simply connected type-D character lattice.

                  The closed carrier and its pinned generators #

                  The Hopf ideal cutting out the full-weight type-Dₙ spin carrier inside GL_(2^n).

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                    The defining ideal is the one supplied by the generic Kostant toral-closure construction.

                    The full-weight type-Dₙ spin carrier over ℤ, obtained as the smallest closed subgroup scheme containing the represented numbered root subgroups and weight torus.

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                      The quotient-spectrum presentation of the type-Dₙ spin carrier.

                      The type-Dₙ carrier is the generic Kostant toral closure for its spin representation.

                      The canonical inclusion of the type-Dₙ spin carrier into GL_(2^n).

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                        The canonical inclusion is the generic Kostant toral-closure inclusion, read across the carrier's presentation as that closure.

                        The type-Dₙ spin carrier is a closed subgroup scheme of its ambient general linear group.

                        A positive or negative numbered simple-root subgroup of the type-Dₙ spin carrier.

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                          The root subgroup is the generic Kostant root subgroup, transported across the carrier's quotient-spectrum presentation.

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                          Including a numbered root subgroup into the ambient general linear group recovers its represented Kostant root subgroup.

                          The represented rank-n split weight torus in the type-Dₙ spin carrier.

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                            The represented weight torus is the generic factored Kostant torus at the type-Dₙ spin data.

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                            Including the weight torus into the ambient general linear group recovers the diagonal torus of the spin weights.

                            The full spin weights make the represented split torus a closed subgroup scheme of the carrier.

                            Two morphisms out of the type-Dₙ spin carrier agree when they agree on its numbered root subgroups and represented split torus.

                            Matrix-valued points #

                            noncomputable def TauCeti.TypeDSpinCarrier.points (n : ℕ) (hn : 4 ≤ n) (A : Type v) [CommRing A] :

                            The matrix-valued points of the type-Dₙ spin carrier.

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                              The carrier points are exactly the invertible matrices cut out by the defining Hopf ideal.

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                              theorem TauCeti.TypeDSpinCarrier.mem_points_iff (n : ℕ) (hn : 4 ≤ n) (A : Type v) [CommRing A] (g : GL (Fin (dimension n)) A) :

                              A matrix is a carrier point exactly when its associated convolution point kills the defining Hopf ideal.

                              noncomputable def TauCeti.TypeDSpinCarrier.rootSubgroupPoints (n : ℕ) (hn : 4 ≤ n) (k : Fin n ⊕ Fin n) (A : Type v) [CommRing A] :
                              Multiplicative A →* ↥(points n hn A)

                              The parametrized numbered root subgroup inside the type-Dₙ spin carrier points. The parameter is read through the canonical multiplicative copy of the additive group of A.

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                                A numbered root-subgroup point is its represented divided-power exponential matrix.

                                noncomputable def TauCeti.TypeDSpinCarrier.weightTorusPoints (n : ℕ) (hn : 4 ≤ n) (A : Type v) [CommRing A] :
                                (Fin n → Aˣ) →* ↥(points n hn A)

                                The split spin weight torus inside the type-Dₙ spin carrier points.

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                                  @[simp]

                                  A weight-torus point is the diagonal matrix obtained by evaluating each spin weight.

                                  The pinning equation #

                                  @[simp]

                                  Conjugation by the spin weight torus acts on each numbered root subgroup through its positive or negative simple-root character, on matrix-valued points. A torus point s carries the root-subgroup point of parameter u to the one of parameter α_k(s) u.

                                  The numbered root subgroups sit at the named simple roots #

                                  The two identifications the equations below rewrite with, TauCeti.TypeDStd.rootGeneratorWeight_inl_eq_root_simpleIndex and its lowering counterpart, are proved beside the weight they name, in TauCeti/Algebra/Lie/Orthogonal/TypeD/Root/Generators.lean.

                                  None of the equations below is a simp lemma. Their right-hand sides name the character through TauCeti.DynkinType.simplyConnectedRootDatum, which simp unfolds at the D n branch, so they are not simp-normal; the numbered equations above are, and these are explicit rewrite lemmas for a consumer holding a Dynkin type, as in TauCeti.SpStd.weightTorus_conj_rootSubgroup_root_simpleIndex.

                                  On matrix-valued points, conjugation by the spin weight torus rescales the i-th raising root subgroup through the i-th simple root of the pinned type-Dₙ datum.

                                  On matrix-valued points, conjugation by the spin weight torus rescales the i-th lowering root subgroup through the negative of the i-th simple root of the pinned type-Dₙ datum.