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Sine-window normalization and positive prefix weights

Statement

For a power of two T≥2 and integers 0≤a≤b≤T, WT(a,b)=b−a2−sin⁡(2πb/T)−sin⁡(2πa/T)4sin⁡(π/T). In particular, WT(0,T)=T/2, so ∣ΨT⟩ is normalized, and every nonempty interval has WT(a,b)≥T−2.

Facts & Assumptions

Given: The sine window and interval mass in Finite sine-window phase state.

[F1]

Finite geometric sum for phase-estimation amplitudes: finite geometric sums satisfy ∑j=0n−1zj=(1−zn)/(1−z) when z≠1.

[F2]

Finite sine-window phase state: WT(a,b) is the sum of the indicated nonnegative sine squares.

[F3]

Double-angle and quadratic power-reduction identities: sin⁡2x=(1−cos⁡(2x))/2.

[F5]

Sine chord and linear bounds: sin⁡(πu)≥2u for 0≤u≤1/2.

Proof

1.1F1F2F3F4F5algebra

Put z=e2πi/T. By [F4], zT=e2πi=1. Also [F5] gives sin⁡(π/T)≥2/T>0, so 1−z≠0. Reindexing [F1] gives ∑τ=ab−1e2πi(τ+1/2)/T=e2πi(a+1/2)/T1−zb−a1−z=eiπ(a+b)/Tsin⁡(π(b−a)/T)sin⁡(π/T). The real part of the last expression is [sin⁡(2πb/T)−sin⁡(2πa/T)]/[2sin⁡(π/T)] by the sine addition formula [F4]. Applying [F3] to the defining sum [F2] proves the displayed formula for WT(a,b).

2.1step 1.1algebra

Setting a=0,b=T in the formula of step 1.1 makes its sine difference zero, so WT(0,T)=T/2. The squared norm of ∣ΨT⟩ is (2/T)WT(0,T)=1.

3.1F2F5F6algebra∎

If a<b, choose an integer τ in [a,b). Then τ+1/2 lies between 1/2 and T−1/2, so its angle lies in [π/(2T),π−π/(2T)]. The chord bound [F5] gives sin⁡(π/(2T))≥1/T, and [F6] reflects this lower bound to the upper half of the interval. That summand is at least T−2 and all other summands are nonnegative by [F2].

Depends on

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Sources