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Distinct complex exponentials have full interval Gram rank

Statement

Let t>0, let z1,…,zn be pairwise distinct complex numbers, and let a1,…,an be nonzero complex numbers. The functions ajezjs on 0<s<t are linearly independent. Consequently the vectors (ajezjs)j=1n, as s varies in this interval, span Cn. Repeated identical exponents contribute only one direction per distinct exponent after combining the corresponding nonzero coordinate vector.

Statement references

Facts & Assumptions

[F1]

Give C its standard coordinate inner product and ordered basis (1). Its induced length ∥w∥=ww‾=∣w∣ is a complex norm by the inner-product norm corollary. With this one-vector ordered basis, the finite-dimensional completeness corollary makes it a complex Banach space. For fixed z∈C, scalar multiplication Mz(w)=zw is complex-linear, since Mz(au+bv)=aMz(u)+bMz(v); the finite-domain boundedness corollary therefore makes Mz:C→C bounded. Apply the bounded-operator exponential theorem with X=C and A=Mz. Its partial sums are multiplication by ∑r=0N(zs)r/r!, and evaluating the operator-norm limit at 1 identifies Ez(s)1=ezs. Evaluation is continuous because ∥B1∥≤∥B∥∥1∥=∥B∥ for a bounded operator B. The derivative and group conclusions give dkdskezs=zkezs for every nonnegative integer k and ezse−zs=1, so ezs≠0. Finite operator and ket conventions The induced length is a norm Every finite-dimensional normed space is Banach A linear map from a finite-dimensional normed space is bounded The exponential series of a bounded operator

[F2]

Finite coordinate vectors, their specified bases, and linear pairings use the operator conventions. Finite operator and ket conventions

[F4]

A subspace of a finite-dimensional vector space has a finite basis, and any independent subset extends to a basis of the ambient finite-dimensional space, without a choice principle. If dim_F V = n and U is a linear subspace of V, then U is finite-dimensional, dim_F U ≤ n, and dim_F U = n if and only if U = V, Statement claims 1 and 3.

Proof

Given: The finite data and hypotheses in the Statement, with the function-space and coordinate conventions of [F2] and [F3].

Goal: Prove independence of the functions and the stated spans, including the repeated-exponent case.

1.1F1F3algebra

The scalar hypotheses and specialization established in [F1] apply to each zj. If ∑jcjajezjs=0 throughout the interval, differentiate k=0,…,n−1 times at an interior point s0. This yields ∑jdjzjk=0, where dj=cjajezjs0. For each l, the polynomial pl(x)=∏j≠l(x−zj)/(zl−zj) has degree at most n−1 and values pl(zj)=δlj. Taking the corresponding linear combination of these equations gives dl=0. Since alezls0≠0, every cl=0, which is independence in C(0,t).

2.1F2F3F4step 1.1algebra

Put v(s)=(ajezjs)j=1n and W=span⁡{v(s):0<s<t}. If W were proper, [F4] would give a basis b1,…,br of W extending to a basis b1,…,bn of Cn, with r<n. For x=∑i=1nλibi define ℓ(x)=λr+1. Independence of the basis makes these coordinates unique; comparison of coordinates under addition and scalar multiplication makes ℓ linear. It vanishes on W and satisfies ℓ(br+1)=1. In the standard coordinate basis (ej), set cj=ℓ(ej); then ℓ(x)=∑jcjxj and some cj is nonzero. But ℓ(v(s))=∑jcjajezjs=0 for all s, contradicting step 1.1. Thus W=Cn.

3.1F2F3step 2.1algebra∎

For a finite list of exponents allowing repetitions, let w1,…,wm be its distinct values, and let ul have coordinate aj when zj=wl and zero otherwise. Each ul is nonzero, and their disjoint coordinate supports make them independent: in ∑lαlul=0, a nonzero coordinate in the lth group forces αl=0. The profile vector is ∑lewlsul. By step 2.1 with all amplitudes equal to one, the vectors (ewls)l=1m span Cm. The linear map (xl)l↦∑lxlul therefore carries their span onto span⁡{u1,…,um}, and is injective by independence. Hence the profile span has exactly one direction per distinct exponent, as asserted.

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