Lower-moment norm equivalence for renewal partial sums

Let (Xk)(X_k) be independent copies of a nondegenerate nonnegative random variable, let Sn=X1+⋯+XnS_n=X_1+\cdots+X_n, and set Zn=∑k=1neıSkZ_n=\sum_{k=1}^n e^{\imath S_k}. For p>0p>0, write ∥Zn∥p=(E∣Zn∣p)1/p\|Z_n\|_p=(\mathbb E|Z_n|^p)^{1/p}. Renewal-sum norm conjecture. One has

∥Zn∥p≍∥Zn∥2\|Z_n\|_p\asymp \|Z_n\|_2

for p<2p<2. The preceding argument establishes the analogous equivalence for p≥2p\geq 2, while the lower-moment range is left as a conjectural extension.

References

Primary source

Jerzy Szulga, “Improper Poisson integral of the sinc function”, arXiv:2504.05574 (2025).

Progress summary

Refreshed
Claimed solved

A posted argument claims to prove the conjecture in all cases, but no independent source has checked it, so the problem is not verified as solved.

Szulga's 2025 paper studies renewal-point-process sums and indicates that broader questions are left as conjectures; it does not verify this norm equivalence.

Posted attempt

An unverified argument claims a complete proof: it interpolates between the known fourth-moment bound and the target lower moment when ∣EeıX1∣<1|\mathbb{E}e^{\imath X_1}|<1, and treats the boundary case ∣EeıX1∣=1|\mathbb{E}e^{\imath X_1}|=1 as deterministic. The argument has not been independently verified.

Current status (as of August 2026): A complete proof has been posted but remains unverified; no corroborated resolution of the lower-moment conjecture is recorded.

Sources

Solutions 1

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The conjecture follows from the fourth-moment estimate already proved in Lemma 2.1.1(3).

Let

Sk=X1+⋯+Xk,Zn=∑k=1neiSk,S_k=X_1+\cdots+X_k, \qquad Z_n=\sum_{k=1}^n e^{iS_k},

and first assume the source hypothesis

r=∣EeiX1∣<1.r=\left|\mathbb E e^{iX_1}\right|<1.

The cited lemma supplies a constant C4≥1C_4\ge1, independent of nn, such that

∥Zn∥4≤C4∥Zn∥2.\|Z_n\|_4\le C_4\|Z_n\|_2.

Fix any 0<p<20<p<2, and set

θ=p4−p,12=θp+1−θ4.\theta=\frac{p}{4-p}, \qquad \frac12=\frac{\theta}{p}+\frac{1-\theta}{4}.

Log-convexity of moments gives

∥Zn∥2≤∥Zn∥pθ∥Zn∥41−θ≤C41−θ∥Zn∥pθ∥Zn∥21−θ.\|Z_n\|_2 \le\|Z_n\|_p^\theta\|Z_n\|_4^{1-\theta} \le C_4^{1-\theta} \|Z_n\|_p^\theta\|Z_n\|_2^{1-\theta}.

This interpolation inequality follows directly from Hölder's inequality and remains valid even when 0<p<10<p<1. If ∥Zn∥2>0\|Z_n\|_2>0, rearrangement yields

C4−(4−2p)/p∥Zn∥2≤∥Zn∥p≤∥Zn∥2,C_4^{-(4-2p)/p}\|Z_n\|_2 \le\|Z_n\|_p \le\|Z_n\|_2,

where the upper bound is monotonicity of moments on a probability space. If ∥Zn∥2=0\|Z_n\|_2=0, both sides vanish. Hence

∥Zn∥p≍∥Zn∥2(0<p<2)\|Z_n\|_p\asymp\|Z_n\|_2 \qquad(0<p<2)

uniformly in nn.

The boundary case omitted by the source hypothesis is also immediate. If r=1r=1, equality for the expectation of the unit-modulus random variable eiX1e^{iX_1} implies

eiX1=λalmost surelye^{iX_1}=\lambda\quad\text{almost surely}

for some ∣λ∣=1|\lambda|=1. Thus

Zn=∑k=1nλkZ_n=\sum_{k=1}^n\lambda^k

is deterministic, and ∥Zn∥p=∥Zn∥2\|Z_n\|_p=\|Z_n\|_2 for every p>0p>0. Therefore the requested equivalence holds for every increment distribution, including the lattice boundary case.