5.20.2 Tensor Product Linear Map Domain Relation
The tensor product relates linear maps through domain interactions, defining how algebraic structures intertwine in multilinear algebra.
Tensor Product Linear Map Domain Relation is the fact that the domain of the induced map f ⊗ g : V ⊗ W → V′ ⊗ W′ is exactly the tensor product V ⊗ W of the domains of the individual maps f : V → V′ and g : W → W′, so that the tensor product operation on linear maps always takes as input the tensor product of the original input spaces rather than any other combination of them. This relation, the domain-side counterpart of the codomain relation, fixes precisely what kind of object f ⊗ g is allowed to act on, and it governs how domains combine under composition, restriction to subspaces, and duality.
Statement of the Relation
The Basic Domain Correspondence
Given f : V → V′ and g : W → W′, the induced map has signature
with domain V ⊗ W, the tensor product of the two individual domains V and W. This is forced by the definition of f ⊗ g on simple tensors, (f ⊗ g)(v ⊗ w) = f(v) ⊗ g(w), since the input v ⊗ w must already be an element of V ⊗ W for the expressions f(v) and g(w) to make sense.
Consistency with the Universal Property
The domain relation traces back to how f ⊗ g is constructed: the bilinear map β(v, w) = f(v) ⊗ g(w) has domain V × W, and the universal property of the tensor product converts this bilinear map, uniquely, into a linear map whose domain is the tensor product V ⊗ W of exactly those two spaces — no other domain is produced by the construction.
Domain Behavior Under Special Cases
Identity on One Factor
When f = id_V, the domain relation specializes to id_V ⊗ g : V ⊗ W → V ⊗ W′, with domain V ⊗ W reflecting that the first factor's space, V, is unchanged as an input space while only the second factor's domain space, W, is subject to g.
Domain Behavior Under Composition
If f₁ : V₁ → V₂ and f₂ : V₂ → V₃ are composable, then for any g : W → W′,
with domain V₁ ⊗ W correctly reflecting the domain V₁ of the first map in the composed chain, matching the identity (f₂ ∘ f₁) ⊗ g = (f₂ ⊗ id) ∘ (f₁ ⊗ g).
Diagram of the Domain Correspondence
Restriction of the Domain
Restricting to a Subspace of the Domain
If V₀ ⊆ V is a subspace, the domain relation restricts coherently: V₀ ⊗ W is naturally identified with a subspace of V ⊗ W, and (f ⊗ g)|_{V₀ ⊗ W} = (f|_{V₀}) ⊗ g, so the domain relation is compatible with restricting the tensor product map to a tensor product of subspaces of the original domain.
Kernel Considerations Tied to the Domain
Because the domain of f ⊗ g is V ⊗ W in full, the kernel of f ⊗ g is a subspace of this entire domain and, for finite-dimensional spaces, equals ker(f) ⊗ W + V ⊗ ker(g), a description only meaningful because the domain relation guarantees f ⊗ g is defined on the whole of V ⊗ W rather than some smaller or unrelated space.
Interaction with Duality
Domain Relation for Dual Maps
For the transpose map f* : V′* → V* of f : V → V′, the domain relation for f* ⊗ g* reads f* ⊗ g* : V′* ⊗ W′* → V* ⊗ W*, with domain V′* ⊗ W′* built from the domains of the individual transposes, illustrating that the domain relation applies uniformly regardless of whether the maps involved are "original" maps or their duals.
Significance of the Domain Relation
Guaranteeing Type-Correctness of Inputs
The domain relation guarantees, in advance and without needing to examine specific elements, exactly what kind of input a tensor product map f ⊗ g accepts, namely elements of V ⊗ W, which is essential for correctly composing tensor product maps in longer chains of transformations.
Foundation for Functorial Reasoning
Together with the codomain relation, the domain relation establishes that ⊗ acts functorially on pairs of linear maps, with both the input and output spaces of f ⊗ g determined entirely and predictably by the input and output spaces of f and g, supporting systematic reasoning about tensor constructions built from chains of linear maps.