Buchstab function

From HandWiki
Graph of the Buchstab function ω(u) from u = 1 to u = 4.

The Buchstab function (or Buchstab's function) is the unique continuous function [math]\displaystyle{ \omega: \R_{\ge 1}\rightarrow \R_{\gt 0} }[/math] defined by the delay differential equation

[math]\displaystyle{ \omega(u)=\frac 1 u, \qquad\qquad\qquad 1\le u\le 2, }[/math]
[math]\displaystyle{ {\frac{d}{du}} (u\omega(u))=\omega(u-1), \qquad u\ge 2. }[/math]

In the second equation, the derivative at u = 2 should be taken as u approaches 2 from the right. It is named after Alexander Buchstab, who wrote about it in 1937.

Asymptotics

The Buchstab function approaches [math]\displaystyle{ e^{-\gamma} \approx 0.561 }[/math] rapidly as [math]\displaystyle{ u\to\infty, }[/math] where [math]\displaystyle{ \gamma }[/math] is the Euler–Mascheroni constant. In fact,

[math]\displaystyle{ |\omega(u)-e^{-\gamma}|\le \frac{\rho(u-1)}{u}, \qquad u\ge 1, }[/math]

where ρ is the Dickman function.[1] Also, [math]\displaystyle{ \omega(u)-e^{-\gamma} }[/math] oscillates in a regular way, alternating between extrema and zeroes; the extrema alternate between positive maxima and negative minima. The interval between consecutive extrema approaches 1 as u approaches infinity, as does the interval between consecutive zeroes.[2]

Applications

The Buchstab function is used to count rough numbers. If Φ(xy) is the number of positive integers less than or equal to x with no prime factor less than y, then for any fixed u > 1,

[math]\displaystyle{ \Phi(x,x^{1/u}) \sim \omega(u)\frac{x}{\log x^{1/u}}, \qquad x\to\infty. }[/math]

Notes

  1. (5.13), Jurkat and Richert 1965. In this paper the argument of ρ has been shifted by 1 from the usual definition.
  2. p. 131, Cheer and Goldston 1990.

References