9 Moment growth for the zeta function
For fixed \(\sigma \in \mathbf{R}\) and \(A \geq 0\), we define \(M(\sigma ,A)\) to be the least (fixed) exponent for which the bound
holds for all unbounded \(T {\gt} 1\).
Such moments may be interpreted as the “average" order of the Riemann zeta function. It is not difficult to show that \(M(\sigma ,A)\) is a well-defined (fixed) real number. A non-asymptotic definition is that it is the least constant such that for every \(\varepsilon {\gt}0\) there exists \(C{\gt}0\) such that
holds for all \(T \geq C\).
\(M(\sigma ,A)\) is convex in \(\sigma \).
For any \(\sigma \), \(a (M(\sigma ,1/a)-1)\) is convex non-increasing in \(a\).
\(M(\sigma ,A)=1\) for all \(A \geq 0\) and \(\sigma \geq 1\).
\(M(\sigma ,A) \geq 1\) for all \(A \geq 0\) and \(1/2 \leq \sigma \leq 1\).
\(M(\sigma ,0) = 1\) for all \(\sigma \).
\(M(1-\sigma ,A) = M(1-\sigma ,A) + (1/2-\sigma ) A\) for all \(\sigma \in \mathbf{R}\) and \(A \geq 0\).
For any \(\sigma \), \(a(M(\sigma ,1/a)-1)\) converges to \(\mu (\sigma )\) as \(a \to 0\). In particular (by previous properties), \(M(\sigma ,A) \leq A \mu (\sigma ) + 1\) for all \(\sigma \geq 0\) and \(A \geq 0\), and also \(M(\sigma ,A) \leq M(\sigma ,A_0) + \mu (\sigma )(A-A_0)\) for \(\sigma \geq 0\) and \(A \geq A_0 \geq 0\).
The claim (i) follows from the Phragmen-Lindelöf principle. The claim (ii) follows from Hölder. The claim (iii) follows from standard upper and lower bounds on \(\zeta (\sigma +it)\) for \(\sigma \geq 1\). The claim (iv) follows from (i)-(iii), and (v) is trivial. The claim (vi) follows easily from the functional equation.
For (vii), the bound \(M(\sigma ,A) \leq A \mu (\sigma ) + 1\) is trivial, which implies that
Suppose for contradiction that
thus there is \(\delta {\gt}0\) such that
for all \(A\geq 0\). By convexity, this gives
for all sufficiently small \(\varepsilon \), and then by the Cauchy integral formula and Hölder’s inequality we can conclude that
for unbounded \(|t|\), leading to
Sending \(A\) to infinity and \(\varepsilon \) to zero, we obtain a contradiction.
If the Lindelöf hypothesis holds, then \(M(\sigma ,A) = 1 + \max (1/2-\sigma ,0) A\) for all \(\sigma \in \mathbf{R}\) and \(A \geq 0\). Conversely, if \(M(1/2, A) = 1\) for arbitrarily large \(A \ge 0\), then the Lindelöf hypothesis is true.
Note from Lemma 9.2 that we always have the lower bound \(M(\sigma ,A) \geq 1 + \max (1/2-\sigma ,0) A\). Thus there are not expected to be any further lower bound results for \(M(\sigma ,A)\), and we focus now on upper bounds. Compared to the pointwise estimates \(\mu (\sigma )\) of \(\zeta (\sigma + it)\), which are currently open for all \(0 {\lt} \sigma {\lt} 1\), more are known about moment estimates \(M(\sigma , A)\). In particular,
One has \(M(1/2,A)=1\) for all \(0 \leq A \leq 4\).
From Lemma 9.2 and Lemma 9.4 we may restrict attention to the region \(1/2 \leq \sigma \leq 1\) and \(A \geq 4\).
9.1 Relationship to zeta large value estimates
We can relate \(M(\sigma ,A)\) to \(\mathrm{LV}_\zeta (\sigma ,\tau )\):
If \(1/2 \leq \sigma _0 \leq 1\) and \(A \geq 1\), then
In particular, one has
whenever \(\sigma \geq 1/2\) and \(\tau \geq 2\).
We first show the lower bound, or equivalently that
whenever \(\tau \geq 2\) and \(\sigma \geq 1/2\). Accordingly, let \(N\) be unbounded, \(T = N^{\tau +o(1)}\), \(I \subset [N,2N]\), and \(W\) be a \(1\)-separated subset of \([T,2T]\) such that
for \(t \in W\). By standard Fourier analysis (or by Perron’s formula and contour shifting), this gives
and hence by Hölder
so on summing in \(r\)
By Definition 9.1, the left-hand side is \(\ll T^{M(\sigma _0,A)+o(1)}\). Since \(T = N^{\alpha +o(1)}\), we obtain
giving the claim.
For the converse bound, let \(M\) be the right-hand side of 1. From Lemma 8.9 we have \(M \geq 1\). By [ 144 , § 8.1 ] it will suffice to show that for any \(V{\gt}0\) and any \(1\)-separated \(W \subset [T,2T]\) with
for all \(t \in W\), one has
The claim is clear if \(V \geq T^C\) or \(V \leq T^C\) for some sufficiently large \(C\), so we may assume that \(V = T^{O(1)}\). We also clearly can assume \(|W|\geq 1\). Using the Riemann–Siegel formula [ 144 , Theorem 4.1 ] and dyadic decomposition, we have either
or
for some \(I \subset [N,2N]\) and \(1 \leq N \ll T^{1/2}\), and all \(t \in W\). In either case, we can perform summation by parts and conclude that
or
for some \(I'\) in \([N,2N]\) and all \(t \in W\). As \(\sigma _0 \geq 1/2\), the letter hypothesis is stronger than the former, so we may assume the former. If \(N = T^{o(1)}\) then this would imply that \(V \ll T^{o(1)}\), and we would be done from the trivial bound \(R \ll T\) since \(M \geq 1\). Hence, after passing to a subsequence, we can assume that \(N = T^{1/\tau +o(1)}\) for some \(2 {\lt} \tau {\lt} \infty \). We can also assume that \(V = N^{\sigma -\sigma _0+o(1)}\) for some \(\sigma \in \mathbf{R}\). If \(\sigma \leq \sigma _0\) then \(V \ll T^{o(1)}\) and we are done as before, so we may assume \(\sigma {\gt} \sigma _0\); in particular, \(\sigma \geq 1/2\). From Lemma 8.2 we have
and hence by definition of \(M\)
as required.
One has \(\mathrm{LV}_\zeta (\sigma ,\tau ) \leq \tau - 4 (\sigma -1/2)\) for all \(1/2 \leq \sigma \leq 1\) and \(\tau \geq 2\).
We have an important twelfth moment estimate of Heath-Brown:
From Lemma 8.11 with the exponent pair \((1/2,1/2)\) from Lemma 5.10 we have
If \(2\tau - 12 (\sigma -1/2) \geq 0\), the claim is immediate; if instead \(2\tau - 12 (\sigma -1/2) {\lt} 0\), use Lemma 8.4.
We also have a variant bound, which is slightly better when \(\tau \) is close to \(6(\sigma -1/2)\):
For \(\tau \geq 2\) and \(1/2 \leq \sigma \leq 1\), one has
Let \((N,T,V,(a_n)_{n \in [N,2N]},J,W)\) be a zeta large value pattern with \(N\), \(V = N^{\sigma +o(1)}\), \(T = N^{\tau +o(1)}\) and \(W = N^{\mathrm{LV}_\zeta (\sigma ,\tau )+o(1)}\). Our task is to show that
Write \(a(n) = 1_I(n)\). By a Fourier analytic expansion we can bound
for some fixed \(\varepsilon {\gt}0\) and all \(t \in W\), hence
In particular, we can truncate to large values of \(\zeta (1/2+it_1)\), in the sense that
Summing in \(t\) and using the \(1\)-separation to bound the sum of \(1/(1+|t_1-t|)\) by \(T^{o(1)}\), we conclude that
Hence by dyadic pigeonholing we have
for some \(V' \geq T^{-o(1)} N^{-1/2} V\), and thus
for all \(t'\) in some \(1\)-separated subset \(W'\) of \([T/4, 3T]\) with
Applying [ 103 , Theorem 2 ] (treating different cases using the bounds [ 103 , (7), (8), (9) ] ), we have the bound
and thus
and the claim now follows from the lower bound on \(V'\).
9.2 Known moment growth bounds
[ 144 , Theorem 8.4 ] We have \(M(\sigma ,A) = 1\) when \(A\) is equal to
Additionally, for \(\sigma =2/3\) one can take \(A = 9.6187\dots \), for \(\sigma = 7/10\) one can take \(A=11\), and for \(\sigma =5/7\) one can take \(A=12\).
[ 279 , Theorems 2.1, 2.2 ] We have
and also
In particular, we have
9.3 Large values of \(\zeta \) moments
It is also of interest to control large values of the moments.
For fixed \(1/2 \leq \sigma \leq 1\), \(A \geq 0\), and \(h \geq 0\), let \(M(\sigma ,A, \geq h)\) be the least (fixed) exponent for which the bound
holds for unbounded \(T\). Similarly, let \(M(\sigma ,A,\leq h)\) be the least exponent for which
holds for unbounded \(T\).
If \(1/2 \leq \sigma _0 \leq 1\), \(A \geq 1\), and \(h \geq 0\) are fixed, then
and
That is to say, any bound of the form
whenever \(\tau \geq 2\) and \(\sigma \geq 1/2, h\tau \), gives rise to a bound
Similarly for \(M(\sigma _0,A,\geq h)\), in which we replace the condition \(\sigma \geq h\tau \) by \(\sigma \leq h\tau \).
This is a routine modification of the proof of Lemma 9.5.
If \((k,\ell )\) is an exponent pair with \(k {\gt} 0\), then
and
where
From Lemma 8.11 with the exponent pair \((k,\ell )\) we have
In particular, for \(\sigma -1/2 \leq h\tau \) one has
and for \(\sigma -1/2 \geq h\tau \) one has
The claim then follows from Lemma 9.12.
[ 144 , (8.56) ] \(M(1/2, 6, \geq 11/72) \leq 1\) and \(M(1/2,24, \leq 11/72) \leq 15/4\).
[ 20 , Proposition 2 ] Suppose that \(M(1/2,A,\geq h) \leq 1\) for some \(A \geq 4\) and \(h \geq 0\). Then one has
whenever \(1/2 \leq \sigma \leq 1\), \(\tau {\gt} 0\), and \(0 \leq \alpha \leq 1-\sigma \) is such that
[ 20 , Proposition 5 ] Suppose that \(M(1/2,6,\geq h) \leq 1\) for some \(h \geq 0\). Then for any \(1/2 \leq \alpha {\lt} \sigma {\lt} 1\), one has
It is remarked in [ 20 ] that this proposition could lead to some improvements in current zero density estimate bounds.
[ 32 , Lemma A.1 ] Let \(1/2 \leq \sigma \leq 1\) and \(\tau \geq \frac{30\sigma -11}{8}\) be fixed. Let \(q_0, A_0, q_1, A_1, h\) be fixed quantities such that \(M(1/2,q_0, \geq h) \leq A_0\) and \(M(1/2,q_0, \leq h) \leq A_1\). Suppose that \(\rho \leq \mathrm{LV}(\sigma ,\tau )\) is such that
Then for any \(\alpha _1 \geq 0\) and \(0 \leq \alpha _2 \leq \tau \), one has
In [ 32 ] this lemma is applied with \((q_0,A_0) = (6,1)\) and \((q_1,A_1) = (19,3)\) with \(h = 2/13\), which follows from Corollary 9.13 applied to the exponent pair \((2/7,4/7) = BA(1/6,2/3)\) from Corollary 5.11.