ConceptComplete

Distribution of Primes in Short Intervals

Understanding how primes are distributed at fine scales -- in short intervals [x,x+y][x, x+y] -- requires going beyond the prime number theorem. The key tools are zero-density estimates for ΞΆ(s)\zeta(s) and explicit formulas.


Prime Gaps

Definition6.1Prime Gaps and CramΓ©r's Conjecture

The nn-th prime gap is gn=pn+1βˆ’png_n = p_{n+1} - p_n. The PNT implies gn=o(pn)g_n = o(p_n), and unconditionally gnβ‰ͺpn0.525g_n \ll p_n^{0.525} (Baker-Harman-Pintz, 2001). CramΓ©r's conjecture asserts gn=O((log⁑pn)2)g_n = O((\log p_n)^2). Under RH: gnβ‰ͺpn1/2log⁑png_n \ll p_n^{1/2}\log p_n. Maynard and Ford-Green-Konyagin-Tao proved that large gaps gn≫log⁑pnβ‹…log⁑log⁑pnβ‹…log⁑log⁑log⁑log⁑pnlog⁑log⁑log⁑png_n \gg \log p_n \cdot \frac{\log\log p_n \cdot \log\log\log\log p_n}{\log\log\log p_n} occur infinitely often.

Definition6.2Primes in Short Intervals

The interval [x,x+y][x, x+y] contains ∼y/log⁑x\sim y/\log x primes if y/xβ†’βˆžy/x \to \infty slowly enough. Huxley (1972) proved Ο€(x+y)βˆ’Ο€(x)∼y/log⁑x\pi(x+y) - \pi(x) \sim y/\log x for yβ‰₯x7/12+Ξ΅y \geq x^{7/12+\varepsilon}. Under RH, this holds for yβ‰₯x1/2+Ξ΅y \geq x^{1/2+\varepsilon}. The short interval PNT ψ(x+y)βˆ’Οˆ(x)∼y\psi(x+y) - \psi(x) \sim y depends on controlling the contribution of zeta zeros near Οƒ=1\sigma = 1.


Zero-Density Estimates

ExampleZero-Density Theorems

Let N(Οƒ,T)=∣{ρ=Ξ²+iΞ³:L(ρ,Ο‡)=0,Ξ²β‰₯Οƒ,βˆ£Ξ³βˆ£β‰€T}∣N(\sigma, T) = |\{\rho = \beta + i\gamma : L(\rho, \chi) = 0, \beta \geq \sigma, |\gamma| \leq T\}|. Ingham's bound: N(Οƒ,T)β‰ͺT3(1βˆ’Οƒ)/(2βˆ’Οƒ)+Ξ΅N(\sigma, T) \ll T^{3(1-\sigma)/(2-\sigma)+\varepsilon}. The density hypothesis asserts N(Οƒ,T)β‰ͺT2(1βˆ’Οƒ)+Ξ΅N(\sigma, T) \ll T^{2(1-\sigma)+\varepsilon}. Zero-density estimates substitute for RH in many applications: they show that zeros near Οƒ=1\sigma = 1 are rare enough that their collective contribution is manageable.

RemarkExplicit Formula and Error Terms

The explicit formula ψ(x)=xβˆ’βˆ‘Οxρρ+O(log⁑2x)\psi(x) = x - \sum_\rho \frac{x^\rho}{\rho} + O(\log^2 x) shows that the error in the PNT is controlled by the sum over zeros. The zero-free region Οƒ>1βˆ’c/log⁑t\sigma > 1 - c/\log t implies each zero contributes ∣xρ/Οβˆ£β‰€x1βˆ’c/log⁑T/∣ρ∣|x^\rho/\rho| \leq x^{1-c/\log T}/|\rho|. Summing over zeros with βˆ£Ξ³βˆ£β‰€T|\gamma| \leq T and optimizing TT gives ∣ψ(x)βˆ’x∣β‰ͺxexp⁑(βˆ’clog⁑x)|\psi(x) - x| \ll x\exp(-c\sqrt{\log x}), the de la Vallee-Poussin error term.