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)
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(2)
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(3)
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(4)
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(5)
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(6)
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(Shepp and Lloyd 1966, Wilf 1990), where is a harmonic number
and
is a generalized harmonic number.
In addition,
(7)
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(Shepp and Lloyd 1966, Wilf 1990). Goncharov (1942) showed that
(8)
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which is a Poisson distribution, and
(9)
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which is a normal distribution, is the Euler-Mascheroni
constant, and
is the normal
distribution function.
Let
(10)
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i.e., the length of the longest cycle in . Golomb (1964) computed an approximation (with a sizable
error) to the constant defined as
(11)
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(12)
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(OEIS A084945) and which is known as the Golomb constant or Golomb-Dickman constant.
Knuth (1997) asked for the constants and
such that
(13)
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and Gourdon (1996) showed that
(14)
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where
(15)
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can be expressed in terms of the function
defined by
for
and
(16)
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for ,
by
(17)
|
Shepp and Lloyd (1966) derived
(18)
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(19)
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(20)
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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)
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where
is now known as the Dickman function. Dickman
then found the average value of
such that
, obtaining
(22)
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(23)
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(24)
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(25)
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(26)
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which is identical to .