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TauCeti.LinearAlgebra.End.IntegralExp

Integral exponentials on product lattices #

The product of two additive subgroups stable under divided powers is stable under the componentwise operator. After scalar extension to any commutative ring, its divided-power exponential is the product of the two exponentials. This allows integral representations to be combined without changing the root subgroup actions on their summands.

@[simp]

Divided powers of a componentwise endomorphism act componentwise.

theorem Module.End.dividedPower_prodMap_mem_prod {V : Type u_1} {W : Type u_2} [AddCommGroup V] [Module ℚ V] [AddCommGroup W] [Module ℚ W] (x : End ℚ V) (y : End ℚ W) (M : AddSubgroup V) (N : AddSubgroup W) (hM : ∀ (n : ℕ), ∀ v ∈ M, TauCeti.Associative.dividedPower n x • v ∈ M) (hN : ∀ (n : ℕ), ∀ w ∈ N, TauCeti.Associative.dividedPower n y • w ∈ N) (n : ℕ) (v : V × W) (hv : v ∈ M.prod N) :

A product of divided-power-stable additive subgroups is divided-power-stable.

@[simp]
theorem Module.End.prodRight_baseChangeExp {V : Type u_1} {W : Type u_2} [AddCommGroup V] [Module ℚ V] [AddCommGroup W] [Module ℚ W] {R : Type u_3} [CommRing R] [Algebra ℤ R] (x : End ℚ V) (y : End ℚ W) (M : AddSubgroup V) (N : AddSubgroup W) (hM : ∀ (n : ℕ), ∀ v ∈ M, TauCeti.Associative.dividedPower n x • v ∈ M) (hN : ∀ (n : ℕ), ∀ w ∈ N, TauCeti.Associative.dividedPower n y • w ∈ N) (hx : IsNilpotent x) (hy : IsNilpotent y) (t : R) (z : TensorProduct ℤ R ↥(M.prod N)) :
have E := fun (z : TensorProduct ℤ R ↥(M.prod N)) => (TensorProduct.prodRight ℤ R R ↥M ↥N) ((LinearEquiv.baseChange ℤ R (↥(M.prod N)) (↥M × ↥N) (M.prodEquiv N).toIntLinearEquiv) z); E ((TauCeti.baseChangeExp (LinearMap.prodMap x y) (M.prod N) ⋯ t) z) = ((TauCeti.baseChangeExp x M hM t) (E z).1, (TauCeti.baseChangeExp y N hN t) (E z).2)

Scalar extension identifies the integral exponential on a product lattice with the componentwise exponentials. The coefficient ring may have arbitrary characteristic.