3.3.1 Tensor Linear Functional Domain Space
Explore how tensor linear functionals operate within their domain space, mapping multilinear structures to scalars in mathematical analysis.
Tensor Linear Functional Domain Space is the vector space V that a linear functional ω : V → F takes its input from, examined specifically for how the domain governs the general functional-theoretic facts established in tensor linear functional structure: how the dimension of the domain fixes the codimension of a functional's kernel, how restricting a functional to a subspace of the domain relates to the annihilator construction, and how the domain determines which subspaces are even candidates for a given functional's kernel or annihilator.
Domain Dimension and Kernel Codimension
The Governing Formula
For a nonzero functional ω on domain V, the kernel identity dim(ker(ω)) = dim(V) - 1 is a direct function of the domain's dimension: doubling the dimension of the domain, while keeping ω nonzero, doubles neither the kernel's dimension nor the codimension, since codimension is fixed at exactly 1 regardless of dim(V), so long as dim(V) ≥ 1.
Degenerate Case of a Zero-Dimensional Domain
If dim(V) = 0, then V = {0} and the only functional on V is the zero functional, since there is no nonzero vector to assign a nonzero value to consistently with linearity; the kernel-codimension formula is vacuous in this degenerate case, and functional structure becomes meaningful only once the domain has dimension at least 1.
Restriction of a Functional to a Subspace of the Domain
The Restriction Map
Given a subspace U ⊆ V and a functional ω ∈ V*, the restriction ω|_U : U → F is again a linear functional, now with the smaller domain U. This restriction is exactly the pullback ι*(ω) along the inclusion map ι : U → V, and it is how a single functional on a large domain produces a corresponding functional on any smaller domain contained within it.
Relation to the Annihilator
The functional ω restricts to the zero functional on U, ω|_U = 0, precisely when ω ∈ U°, the annihilator of U; the domain-restriction operation and the annihilator construction are two views of the same underlying fact, that ω vanishes on every vector of the smaller domain U. This connects the domain of a functional directly to the subspace-annihilator relationship: annihilation is nothing more than the statement that a functional's restriction to a given domain is identically zero.
Domain-Dependence of Kernel Candidacy
Not Every Subspace Is a Kernel
A subspace W ⊆ V arises as ker(ω) for some nonzero ω ∈ V* if and only if dim(W) = dim(V) - 1; subspaces of any other dimension cannot be the kernel of a nonzero functional on that particular domain V, since the kernel-codimension formula fixes codimension at exactly 1. Whether a given subspace can serve as a kernel is therefore a question that depends jointly on the subspace and on the specific domain V it sits inside.
Same Subspace, Different Domains
A fixed subspace W of dimension k may be a valid kernel candidate relative to one ambient domain V, with dim(V) = k + 1, but fail to be a valid kernel candidate relative to a larger domain V' ⊃ V with dim(V') > k + 1; kernel candidacy is a relation between a subspace and its specific ambient domain, not an intrinsic property of the subspace alone.
Domain and the Extension of a Functional
Extending From a Subspace Back to the Full Domain
Given a functional ψ defined only on a subspace U ⊆ V, it is always possible to extend ψ to a functional ω on the full domain V satisfying ω|_U = ψ, by choosing a complementary subspace W with V = U ⊕ W and defining ω to agree with ψ on U and to take arbitrary, for instance zero, values on W. This extension is generally not unique, since different choices of complement W or different values assigned on W produce different extensions ω, all agreeing with ψ when restricted back down to the original smaller domain U.
Contrast With Restriction
Restriction from V down to U is a single, well-defined operation, producing exactly one functional ω|_U from a given ω, whereas extension from U up to V is a one-to-many process; this asymmetry mirrors the general asymmetry of the annihilator and pullback constructions, in which passing to a smaller domain is unambiguous while passing to a larger domain requires an additional, non-canonical choice.