Dickman function

The Dickman–de Bruijn function ${\displaystyle \rho (u)}$ is a continuous function that satisfies the delay differential equation

${\displaystyle u\rho '(u)+\rho (u-1)=0\,}$

with initial conditions ${\displaystyle \rho (u)=1}$ for 0 ≤ u ≤ 1.

Dickman proved that, when ${\displaystyle a}$ is fixed, we have

${\displaystyle \Psi (x,x^{1/a})\sim x\rho (a)\,}$

where ${\displaystyle \Psi (x,y)}$ is the number of y-smooth (or y-friable) integers below x.

Ramaswami later gave a rigorous proof that for fixed a, ${\displaystyle \Psi (x,x^{1/a})}$ was asymptotic to ${\displaystyle x\rho (a)}$, with the error bound

${\displaystyle \Psi (x,x^{1/a})=x\rho (a)+O(x/\log x)}$

in big O notation.[4]

The Dickman–de Bruijn used to calculate the probability that the largest and 2nd largest factor of x is less than x^a

The main purpose of the Dickman–de Bruijn function is to estimate the frequency of smooth numbers at a given size. This can be used to optimize various number-theoretical algorithms such as P-1 factoring and can be useful of its own right.

It can be shown using ${\displaystyle \log \rho }$ that[5]

${\displaystyle \Psi (x,y)=xu^{O(-u)}}$

which is related to the estimate ${\displaystyle \rho (u)\approx u^{-u}}$ below.

The Golomb–Dickman constant has an alternate definition in terms of the Dickman–de Bruijn function.

A first approximation might be ${\displaystyle \rho (u)\approx u^{-u}.\,}$ A better estimate is[6]

${\displaystyle \rho (u)\sim {\frac {1}{\xi {\sqrt {2\pi u}}}}\cdot \exp(-u\xi +\operatorname {Ei} (\xi ))}$

where Ei is the exponential integral and ξ is the positive root of

${\displaystyle e^{\xi }-1=u\xi .\,}$

A simple upper bound is ${\displaystyle \rho (x)\leq 1/x!.}$

${\displaystyle u}$	${\displaystyle \rho (u)}$
1	1
2	3.0685282×10−1
3	4.8608388×10−2
4	4.9109256×10−3
5	3.5472470×10−4
6	1.9649696×10−5
7	8.7456700×10−7
8	3.2320693×10−8
9	1.0162483×10−9
10	2.7701718×10−11

For each interval [n − 1, n] with n an integer, there is an analytic function ${\displaystyle \rho _{n}}$ such that ${\displaystyle \rho _{n}(u)=\rho (u)}$. For 0 ≤ u ≤ 1, ${\displaystyle \rho (u)=1}$. For 1 ≤ u ≤ 2, ${\displaystyle \rho (u)=1-\log u}$. For 2 ≤ u ≤ 3,

${\displaystyle \rho (u)=1-(1-\log(u-1))\log(u)+\operatorname {Li} _{2}(1-u)+{\frac {\pi ^{2}}{12}}.}$

with Li₂ the dilogarithm. Other ${\displaystyle \rho _{n}}$ can be calculated using infinite series.[7]

An alternate method is computing lower and upper bounds with the trapezoidal rule;[6] a mesh of progressively finer sizes allows for arbitrary accuracy. For high precision calculations (hundreds of digits), a recursive series expansion about the midpoints of the intervals is superior.[8]

Friedlander defines a two-dimensional analog ${\displaystyle \sigma (u,v)}$ of ${\displaystyle \rho (u)}$.[9] This function is used to estimate a function ${\displaystyle \Psi (x,y,z)}$ similar to de Bruijn's, but counting the number of y-smooth integers with at most one prime factor greater than z. Then

${\displaystyle \Psi (x,x^{1/a},x^{1/b})\sim x\sigma (b,a).\,}$

• Buchstab function, a function used similarly to estimate the number of rough numbers, whose convergence to ${\displaystyle e^{-\gamma }}$ is controlled by the Dickman function
• Golomb–Dickman constant

• Broadhurst, David (2010). "Dickman polylogarithms and their constants". arXiv:1004.0519 [math-ph].
• Soundararajan, Kannan (2012). "An asymptotic expansion related to the Dickman function". Ramanujan Journal. 29 (1–3): 25–30. arXiv:1005.3494. doi:10.1007/s11139-011-9304-3. MR 2994087.
• Weisstein, Eric W. "Dickman function". MathWorld.