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A nonaligned one-dimensional micro window has resonance error

Example

Let a(y)=1 on [0,1/2) and a(y)=2 on [1/2,1), extended with period one. At phase θ=0 and nonaligned ratio r=δ/ϵ=3/2, the exact sampled harmonic tensor is Ar=6/5, whereas A∗=4/3. The discrepancy is 2/15>0 even though the continuum coefficient is periodic.

Facts & Assumptions

Given: The two-phase periodic scalar coefficient, phase zero, and sample ratio r=3/2.

[F1]

One-dimensional nonaligned micro sampling resonance bound: the sampled tensor is the reciprocal of the average reciprocal coefficient and obeys ∣Ar−A∗∣≤2Λ2/(λr).

[F2]

A C^1 diffeomorphism satisfies the change-of-variables formula for nonnegative Lebesgue measurable functions: the affine pullback y↦3y/2 preserves measurability and null sets, so the sampled reciprocal integral is well defined on the stated coefficient class.

Proof

1.1F1F2algebra

By [F2], the sample pullback and its reciprocal are measurable on [0,1]. Over 0≤t≤3/2, the reciprocal coefficient equals 1 for lengths 1/2, 1/2, and 1/2 on the successive intervals [0,1/2), [1/2,1), and [1,3/2), except that its value on the middle interval is 1/2. Thus its integral is 1/2+1/4+1/2=5/4; dividing by r=3/2 gives ∫01a(3y/2)−1dy=5/6, so Ar=6/5. The full-period reciprocal mean is (1+1/2)/2=3/4, hence A∗=4/3.

2.1F1step 1.1algebra∎

Therefore ∣Ar−A∗∣=∣6/5−4/3∣=2/15. Here λ=1, Λ=2, and 1/r=2/3, so the bound in [F1] is 2⋅4⋅(2/3)=16/3; indeed 2/15≤16/3. The example verifies both nonzero resonance and the stated conservative estimate.

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