Analytic Number Theory Exponent Database

12 Zero density energy theorems

Definition 12.1 Zero density exponents
#

For 1/2σ1 and T>0, let N(σ,T) denote the additive energy E1(Σ) of the imaginary parts of the zeroes ρ of the Riemann zeta function with Re(ρ)σ and |Im(ρ)|T. For fixed 1/2σ1, the zero density exponent A(σ)[,) is the infimum of all exponents A for which one has

N(σδ,T)TA(1σ)+o(1)

for all unbounded T and infinitesimal δ>0.

The exponent A(σ) is also essentially referred to as B(σ) in [ 77 ] (though without the technical shift by δ in that reference).

Implemented at zero_density_energy_estimate.py as:
Zero_Density_Energy_Estimate

Lemma 12.2 Basic properties of A
  • We have the trivial bounds

    2A(σ),4A(σ)11σA(σ)3A(σ)

    for any 1/2σ1.

  • σ(1σ)A(σ) is non-increasing, with A(1/2)=6 and A(1)=.

  • If the Riemann hypothesis holds, then A(σ)= for all 1/2<σ1.

Implemented at zero_density_energy_estimate.py as:
add_trivial_zero_density_energy_estimates(hypotheses)

Proof

Upper bounds on A(σ) can be obtained from large value energy theorems via the following relation.

Lemma 12.3 Zero density energy from large values energy

Let 1/2<σ<1. Then

A(σ)(1σ)max(supτ1LVζ(σ,τ)/τ,lim supτLV(σ,τ)/τ).
Proof
Corollary 12.4

Let 1/2<σ<1 and τ0>0 be fixed. Then

A(σ)(1σ)max(sup2τ<τ0LVζ(σ,τ)/τ,supτ0τ2τ0LV(σ,τ)/τ)

Implemented at zero_density_energy_estimate.py as:
lver_to_energy_bound(LVER, LVER_zeta, sigma_interval)

Proof

12.1 Known additive energy bounds

Proposition 12.5 Additive energy under the Lindelof hypothesis

Let 1/2σ1 be fixed. Then one has

A(σ)84σ

and A(σ)0 if σ>3/4.

Proof

[ 80 , Theorem 2 ] Let 1/2σ1 be fixed. Then one can bound A(σ) by

1011σ(2σ)(1σ) for 1/2σ2/3;1819σ(42σ)(1σ) for 2/3σ3/4;124σ1 for 3/4σ1.

Recorded in literature.py as:
add_zero_density_energy_heath_brown_1979()
Derived in derived.py as:
prove_heath_brown_energy_estimate()

Proof

We found the following estimates with the use of computer-aided proof discovery, which improve on Theorem 12.6 in various ranges of σ. First, by using Theorem 10.20 in place of Corollary 10.21 in the proof of the previous theorem, it is possible to obtain an improved additive energy estimate for σ3/4. A human-readable proof is contained in the following theorem.

Theorem 12.7

For 3/4σ5/6 one has

A(σ)max(1819σ2(3σ1)(1σ),4(109σ)5(4σ1)(1σ)).

Derived in derived.py as:
prove_improved_heath_brown_energy_estimate()

Proof

Using Theorem 10.27, it is possible to obtain improved energy estimates near σ=3/4, which are given by the next two theorems.

Theorem 12.8

For 7/10σ3/4, one has

A(σ)max(5(1819σ)2(5σ+3)(1σ),2(4544σ)(2σ+15)(1σ)).

Derived in derived.py as:
prove_zero_density_energy_2()

Proof
Theorem 12.9

For 3/4σ4/5, one has

A(σ)max(197220σ8(5σ1)(1σ),3(2930σ)5(5σ1)(1σ),4(109σ)5(4σ1)(1σ))

Derived in derived.py as:
prove_zero_density_energy_3()

Proof

Modest improvements are possible by incorporating more large value estimates; these are recorded in the next few theorems.

Theorem 12.10

For 664/877σ31/40, one has

A(σ)max(7291σ7(11σ8)(1σ),5(1819σ)2(5σ+3)(1σ)).

Derived in derived.py as:
prove_zero_density_energy_4()

Proof
Theorem 12.11

For 42/55σ79/103, one has

A(σ)max(1819σ6(15σ11)(1σ),3(1819σ)4(4σ1)(1σ)).

Derived in derived.py as:
prove_zero_density_energy_5()

Proof
Theorem 12.12

For 79/103σ84/109, one has

A(σ)max(1819σ2(37σ27)(1σ),5(1819σ)2(13σ3)(1σ)).

Derived in derived.py as:
prove_zero_density_energy_6()

Proof
Theorem 12.13
#

For 84/109σ5/6, one has

A(σ)max(1819σ9(3σ2)(1σ),4(109σ)5(4σ1)(1σ)).

Derived in derived.py as:
prove_zero_density_energy_7()

Theorem 12.14
#

For 165/226σ42/55 one has

A(σ)max(457546σ2(6158σ)(1σ),5(1819σ)2(5σ+3)(1σ)).

Derived in derived.py as:
prove_zero_density_energy_12()

Table 12.1 records the sharpest known unconditional upper bounds on A(σ) for 1/2σ1 (except when close to σ=1, when sharper estimates are available by applying Lemma 12.2 with known zero-density bounds).

Table 12.1 Current best upper bound on A(σ)

A(σ) bound

Range

Reference

1011σ(2σ)(1σ)

12σ23=0.6666

Theorem 12.6

1819σ(42σ)(1σ)

23σ710=0.7

Theorem 12.6

5(1819σ)2(5σ+3)(1σ)

710σ53942121460=0.7255

Theorem 12.8

2(4544σ)(2σ+15)(1σ)

53942121460σ165226=0.7300

Theorem 12.8

457546σ2(6158σ)(1σ)

165226σ5831+600018240=0.7373

Theorem 12.14

5(1819σ)2(5σ+3)(1σ)

5831+600018240σ4255=0.7636

Theorem 12.14, 12.10

1819σ6(15σ11)(1σ)

4255σ97127=0.7637

Theorem 12.11

3(1819σ)4(4σ1)(1σ)

97127σ79103=0.7669

Theorem 12.11

1819σ2(37σ27)(1σ)

79103σ3343=0.7674

Theorem 12.12

5(1819σ)2(13σ3)(1σ)

3343σ84109=0.7706

Theorem 12.12

1819σ9(3σ2)(1σ)

84109σ12731286891184=0.7721

Theorem 12.13

4(109σ)5(4σ1)(1σ)

12731286891184σ56=0.8333

Theorem 12.7, 12.9, 12.13

124σ1

56σ1

Theorem 12.6

\includegraphics[width=0.5\textwidth ]{chapter/zero_density_energy_estimate.png}
Figure 12.1 Comparison of bounds on A(σ) under various assumptions.