13 Zero free regions
A zero of the Riemann zeta function is a complex number \(\rho = \beta + i\gamma \) for which \(\zeta (\rho ) = 0\).
There are infinitely many “trivial" zeros of the form \(\rho = -2n\) for integer \(n \ge 1\); these zeros are well understood.
There are a countably infinite number of “non-trivial zeros lying inside the critical strip \(0 {\lt} \Re z {\lt} 1\).
A zero-free region of the Riemann zeta function is a set \(D \subset \mathbb {C}\) for which \(\zeta (s) \ne 0\) for all \(s \in D\).
The following properties hold:
(Symmetry about the real axis) If \(\zeta (\sigma + it) \ne 0\) then \(\zeta (\sigma - it) \ne 0\).
(Symmetry about the critical line \(\Re s = 1/2\)) For \(0 \le \sigma \le 1\), if \(\zeta (\sigma + it) \ne 0\) then \(\zeta (1 - \sigma + it) \ne 0\).
(Non vanishing for \(\Re s {\gt} 1\)) If \(\Re s {\gt} 1\) then \(\zeta (s) \ne 0\).
Claim (i) follows directly from the property \(\overline{\zeta (s)} = \zeta (\overline{s})\). Claim (ii) follows from the functional equation
and claim (iii) follows from the Euler product formula
A well-known conjecture regarding the non-trivial zeroes of \(\zeta (s)\) is the Riemann hypothesis.
If \(\rho \) is a non-trivial zero of the Riemann zeta function, then \(\Re \rho = 1/2\).
In light of Lemma 13.2, for the rest of the chapter we will focus on the quadrant
The first non-trivial zero-free region was due to de la Vallée Poussin [ 56 ] and Hadamard [ 89 ] , who showed independently that:
One has \(\zeta (1 + it) \ne 0\) for any real \(t\).
For \(\Re s {\gt} 1\), one has
where the outer sum runs through all primes. Applying this formula at \(s = \sigma , \sigma + it\) and \(\sigma + 2it\) (\(t \ne 0\)), and since \(3 + 4\cos \theta + \cos 2\theta = 2(1 + \cos \theta )^2 \ge 0\), one has
It follows that \(|\zeta (\sigma )^3 \zeta (\sigma + it)^4 \zeta (\sigma + 2it)| \ge 1\). Now as \(\sigma \to 1\) from above (and \(t\) remains fixed), one has
since \(\zeta \) has a simple pole at \(s = 1\) and no pole at \(\sigma + 2it\). If \(\zeta (1 + it) = 0\), then \(\zeta (\sigma + it) \ll \sigma - 1\) so that \(|\zeta (\sigma )^3 \zeta (\sigma + it)^4 \zeta (\sigma + 2it)| \ll \sigma - 1\), a contradiction.
This was used to prove the prime number theorem \(\pi (x) \sim x/\log x\) as \(x \to \infty \) (in fact the two statements are equivalent).
13.1 Relation to growth rates of zeta
Using estimates of \(\zeta (\sigma + it)\) close to the line \(\sigma = 1\), one can extend the zero free region slightly inside the critical strip.
Suppose and \(0 {\lt} g(t) \le 1 {\lt} f(t)\) are real-valued functions for \(t \ge 0\), with \(f(t)\) non-decreasing and tending to infinity with \(t\), and \(g(t)\) non-increasing. Suppose further that \(e^{f(t)}/g(t) = o(f(t))\). If
then \(\zeta (\sigma + it) \ne 0\) for
where \(A {\gt} 0\) is an absolute constant.
See [ 277 , Theorem 3.10 ] .
One has \(\zeta (\sigma + it) \ne 0\) if
for an absolute constant \(A {\gt} 0\) and \(t\) sufficiently large.
Thanks to the convexity bound \(\mu (\sigma ) \le (1-\sigma )/2\), one may take \(g(t) = 1/2\), \(f(t) = t^{1/4 + o(1)}\) in Lemma 13.5. The result follows.
This classical result has been improved in a number of works, most of which make crucial use of non-trivial estimates of certain types of exponential sums.
One has \(\zeta (\sigma + it) \ne 0\) if
for an absolute constant \(A {\gt} 0\) and \(t\) sufficiently large.
Follows from the zeta bound corresponding to
for integer \(k\ge 3\), which is generated by the van der Corput exponent pair \(A^{k - 2}B(0, 1) = (\frac{1}{2^k - 2}, 1 - \frac{k - 1}{2^k - 2})\). However, one needs to make explicit the \(o(1)\) term in the bound \(\zeta (\sigma + it) \ll t^{\mu (\sigma ) + o(1)}\). In particular, by [ 277 , Theorem 5.14 ] , one has
Taking
and using the Phragmén Lindelöf principle, one has
so we may take \(f(t) = (\log t)^5\) and \(g(t) = (\log \log t)^2/\log t\) in Lemma 13.5.
One has \(\zeta (\sigma + it) \ne 0\) if
for \(t\) sufficiently large.
One has \(\zeta (\sigma + it) \ne 0\) if
for an absolute constant \(A {\gt} 0\) and \(t\) sufficiently large.
Via estimates of Vinogradov’s integral, one may obtain an estimate of the form (see e.g. Richert [ 248 ] )
where \(B {\gt} 0\) is a constant and \(t\) sufficiently large. Take
so that
The result follows from applying Lemma 13.5.