Let 
 be a permutation of 
 elements, and let 
 be the number of permutation
 cycles of length 
 in this permutation. Picking
 
 at random, it turns out that
| 
(1)
 | |||
| 
(2)
 | |||
| 
(3)
 | |||
| 
(4)
 | |||
| 
(5)
 | |||
| 
(6)
 | 
(Shepp and Lloyd 1966, Wilf 1990), where  is a harmonic number
 and 
 is a generalized harmonic number.
In addition,
| 
(7)
 | 
(Shepp and Lloyd 1966, Wilf 1990). Goncharov (1942) showed that
| 
(8)
 | 
which is a Poisson distribution, and
| 
(9)
 | 
which is a normal distribution,  is the Euler-Mascheroni
 constant, and 
 is the normal
 distribution function.
Let
| 
(10)
 | 
i.e., the length of the longest cycle in . Golomb (1964) computed an approximation (with a sizable
 error) to the constant defined as
| 
(11)
 | |||
| 
(12)
 | 
(OEIS A084945) and which is known as the Golomb constant or Golomb-Dickman constant.
Knuth (1997) asked for the constants  and 
 such that
| 
(13)
 | 
and Gourdon (1996) showed that
| 
(14)
 | 
where
| 
(15)
 | 
 can be expressed in terms of the function 
 defined by 
 for 
 and
| 
(16)
 | 
for ,
 by
| 
(17)
 | 
Shepp and Lloyd (1966) derived
| 
(18)
 | |||
| 
(19)
 | |||
| 
(20)
 | 
where 
 is the logarithmic integral.
Surprisingly, there is a connection between  and prime
 factorization (Knuth and Pardo 1976, Knuth 1997, pp. 367-368, 395, and 611).
 Dickman (1930) investigated the probability 
 that the greatest
 prime factor 
 of a random integer between 1
 and 
 satisfies 
 for 
.
 He found that
| 
(21)
 | 
where 
 is now known as the Dickman function. Dickman
 then found the average value of 
 such that 
, obtaining
| 
(22)
 | |||
| 
(23)
 | |||
| 
(24)
 | |||
| 
(25)
 | |||
| 
(26)
 | 
which is identical to .
 
         
	    
	
    

