Let ζ denote the Riemann zeta function. The assertion is an unconditional, completely explicit zero-free region for the low-lying part of the critical strip, of height 6:
0<Res<1 and ∣Ims∣≤6⟹ζ(s)=0.
The first nontrivial zero occurs at height ≈14.13, so this is a proper truncation of the region in which zeros must be sought.
The proof is a quantitative estimate on the completed zeta function. Write Λ(s)=π−s/2Γ(s/2)ζ(s) and Λ0(s)=Λ(s)+s1+1−s1 for its entire part, which is the Mellin transform
Λ0(s)=21∫0∞f(t)ts/2−1dt
of the modified Jacobi theta kernel f, with f(t)=θ(t)−1 for t>1 and f(t)=t−1/2(θ(1/t)−1) for 0<t<1.
Comparison with a geometric series gives ∣θ(t)−1∣≤1021e−πt for t≥1, so for 0<Res<1 the Mellin integrand is dominated by 1021t−1/2e−πt on (1,∞) and by 1021t−3/2e−π/t on (0,1]; the substitution t↦1/t identifies the second integral with the first. Hence
∥Λ0(s)∥≤1021∫1∞u−1/2e−πudu≤0.0268,
the tail integral being estimated by the elementary inequality u−1/2≤1−2u−1+83(u−1)2. On the other hand, in the rectangle 0<Res<1, ∣Ims∣≤6 one has ∥s∥∥1−s∥≤36⋅37<36.5, so
s1+1−s1=∥s∥∥1−s∥1>36.51>0.0268.
Therefore Λ(s)=Λ0(s)−s1−1−s1 cannot vanish in the rectangle, and since π−s/2Γ(s/2)=0 for Res>0, neither can ζ(s).
Height 6 is close to the ceiling of this method: with the exact constants 2/(1−e−π) and ∫1∞u−1/2e−πudu=0.012178… one gets ∥Λ0∥≤0.02547, which fails once ∥s∥∥1−s∥≥39.3, i.e. above height ≈6.2.
Formalization note.riemannZeta is Mathlib's zeta function; |s.im| is the absolute value of the imaginary part of s.
Preamble
import Mathlib.NumberTheory.LSeries.RiemannZeta
import Mathlib.NumberTheory.LSeries.Nonvanishing
open Complex
Formal statement
theorem zeta_ne_zero_of_mem_strip_of_abs_im_le_six (s : ℂ) (h0 : 0 < s.re) (h1 : s.re < 1)
(him : |s.im| ≤ 6) : riemannZeta s ≠ 0 := by sorry
Source
Standard theory of the completed Riemann zeta function; the quantitative form given here (bounding the entire part of the completed zeta function against its pole terms, with the substitution t -> 1/t on (0,1) and the tail bound for the incomplete Gamma integral) is elementary. See e.g. Titchmarsh, The Theory of the Riemann Zeta-Function, 2nd ed., Ch. II.