Special function defined by an integral
"Li(x)" redirects here. For the polylogarithm denoted by Li
s (
z ), see
Polylogarithm .
Plot of the logarithmic integral function li(z) in the complex plane from -2-2i to 2+2i with colors created with Mathematica 13.1 function ComplexPlot3D
In mathematics , the logarithmic integral function or integral logarithm li(x ) is a special function . It is relevant in problems of physics and has number theoretic significance. In particular, according to the prime number theorem , it is a very good approximation to the prime-counting function , which is defined as the number of prime numbers less than or equal to a given value
x
{\displaystyle x}
.
Logarithmic integral function plot
Integral representation [ edit ]
The logarithmic integral has an integral representation defined for all positive real numbers x ≠ 1 by the definite integral
li
(
x
)
=
∫
0
x
d
t
ln
t
.
{\displaystyle \operatorname {li} (x)=\int _{0}^{x}{\frac {dt}{\ln t}}.}
Here, ln denotes the natural logarithm . The function 1/(ln t ) has a singularity at t = 1 , and the integral for x > 1 is interpreted as a Cauchy principal value ,
li
(
x
)
=
lim
ε
→
0
+
(
∫
0
1
−
ε
d
t
ln
t
+
∫
1
+
ε
x
d
t
ln
t
)
.
{\displaystyle \operatorname {li} (x)=\lim _{\varepsilon \to 0+}\left(\int _{0}^{1-\varepsilon }{\frac {dt}{\ln t}}+\int _{1+\varepsilon }^{x}{\frac {dt}{\ln t}}\right).}
Offset logarithmic integral [ edit ]
The offset logarithmic integral or Eulerian logarithmic integral is defined as
Li
(
x
)
=
∫
2
x
d
t
ln
t
=
li
(
x
)
−
li
(
2
)
.
{\displaystyle \operatorname {Li} (x)=\int _{2}^{x}{\frac {dt}{\ln t}}=\operatorname {li} (x)-\operatorname {li} (2).}
As such, the integral representation has the advantage of avoiding the singularity in the domain of integration.
Equivalently,
li
(
x
)
=
∫
0
x
d
t
ln
t
=
Li
(
x
)
+
li
(
2
)
.
{\displaystyle \operatorname {li} (x)=\int _{0}^{x}{\frac {dt}{\ln t}}=\operatorname {Li} (x)+\operatorname {li} (2).}
The function li(x ) has a single positive zero; it occurs at x ≈ 1.45136 92348 83381 05028 39684 85892 02744 94930... OEIS : A070769 ; this number is known as the Ramanujan–Soldner constant .
li
(
Li
−
1
(
0
)
)
=
li
(
2
)
{\displaystyle {\text{li}}({\text{Li}}^{-1}(0))={\text{li}}(2)}
≈ 1.045163 780117 492784 844588 889194 613136 522615 578151... OEIS : A069284
This is
−
(
Γ
(
0
,
−
ln
2
)
+
i
π
)
{\displaystyle -(\Gamma \left(0,-\ln 2\right)+i\,\pi )}
where
Γ
(
a
,
x
)
{\displaystyle \Gamma \left(a,x\right)}
is the incomplete gamma function . It must be understood as the Cauchy principal value of the function.
Series representation [ edit ]
The function li(x ) is related to the exponential integral Ei(x ) via the equation
li
(
x
)
=
Ei
(
ln
x
)
,
{\displaystyle {\hbox{li}}(x)={\hbox{Ei}}(\ln x),\,\!}
which is valid for x > 0. This identity provides a series representation of li(x ) as
li
(
e
u
)
=
Ei
(
u
)
=
γ
+
ln
|
u
|
+
∑
n
=
1
∞
u
n
n
⋅
n
!
for
u
≠
0
,
{\displaystyle \operatorname {li} (e^{u})={\hbox{Ei}}(u)=\gamma +\ln |u|+\sum _{n=1}^{\infty }{u^{n} \over n\cdot n!}\quad {\text{ for }}u\neq 0\;,}
where γ ≈ 0.57721 56649 01532 ... OEIS : A001620 is the Euler–Mascheroni constant . A more rapidly convergent series by Ramanujan [ 1] is
li
(
x
)
=
γ
+
ln
|
ln
x
|
+
x
∑
n
=
1
∞
(
(
−
1
)
n
−
1
(
ln
x
)
n
n
!
2
n
−
1
∑
k
=
0
⌊
(
n
−
1
)
/
2
⌋
1
2
k
+
1
)
.
{\displaystyle \operatorname {li} (x)=\gamma +\ln |\ln x|+{\sqrt {x}}\sum _{n=1}^{\infty }\left({\frac {(-1)^{n-1}(\ln x)^{n}}{n!\,2^{n-1}}}\sum _{k=0}^{\lfloor (n-1)/2\rfloor }{\frac {1}{2k+1}}\right).}
Asymptotic expansion [ edit ]
The asymptotic behavior for x → ∞ is
li
(
x
)
=
O
(
x
ln
x
)
.
{\displaystyle \operatorname {li} (x)=O\left({\frac {x}{\ln x}}\right).}
where
O
{\displaystyle O}
is the big O notation . The full asymptotic expansion is
li
(
x
)
∼
x
ln
x
∑
k
=
0
∞
k
!
(
ln
x
)
k
{\displaystyle \operatorname {li} (x)\sim {\frac {x}{\ln x}}\sum _{k=0}^{\infty }{\frac {k!}{(\ln x)^{k}}}}
or
li
(
x
)
x
/
ln
x
∼
1
+
1
ln
x
+
2
(
ln
x
)
2
+
6
(
ln
x
)
3
+
⋯
.
{\displaystyle {\frac {\operatorname {li} (x)}{x/\ln x}}\sim 1+{\frac {1}{\ln x}}+{\frac {2}{(\ln x)^{2}}}+{\frac {6}{(\ln x)^{3}}}+\cdots .}
This gives the following more accurate asymptotic behaviour:
li
(
x
)
−
x
ln
x
=
O
(
x
(
ln
x
)
2
)
.
{\displaystyle \operatorname {li} (x)-{\frac {x}{\ln x}}=O\left({\frac {x}{(\ln x)^{2}}}\right).}
As an asymptotic expansion, this series is not convergent : it is a reasonable approximation only if the series is truncated at a finite number of terms, and only large values of x are employed. This expansion follows directly from the asymptotic expansion for the exponential integral .
This implies e.g. that we can bracket li as:
1
+
1
ln
x
<
li
(
x
)
ln
x
x
<
1
+
1
ln
x
+
3
(
ln
x
)
2
{\displaystyle 1+{\frac {1}{\ln x}}<\operatorname {li} (x){\frac {\ln x}{x}}<1+{\frac {1}{\ln x}}+{\frac {3}{(\ln x)^{2}}}}
for all
ln
x
≥
11
{\displaystyle \ln x\geq 11}
.
Number theoretic significance [ edit ]
The logarithmic integral is important in number theory , appearing in estimates of the number of prime numbers less than a given value. For example, the prime number theorem states that:
π
(
x
)
∼
li
(
x
)
{\displaystyle \pi (x)\sim \operatorname {li} (x)}
where
π
(
x
)
{\displaystyle \pi (x)}
denotes the number of primes smaller than or equal to
x
{\displaystyle x}
.
Assuming the Riemann hypothesis , we get the even stronger:[ 2]
|
li
(
x
)
−
π
(
x
)
|
=
O
(
x
log
x
)
{\displaystyle |\operatorname {li} (x)-\pi (x)|=O({\sqrt {x}}\log x)}
In fact, the Riemann hypothesis is equivalent to the statement that:
|
li
(
x
)
−
π
(
x
)
|
=
O
(
x
1
/
2
+
a
)
{\displaystyle |\operatorname {li} (x)-\pi (x)|=O(x^{1/2+a})}
for any
a
>
0
{\displaystyle a>0}
.
For small
x
{\displaystyle x}
,
li
(
x
)
>
π
(
x
)
{\displaystyle \operatorname {li} (x)>\pi (x)}
but the difference changes sign an infinite number of times as
x
{\displaystyle x}
increases, and the first time this happens is somewhere between 1019 and 1.4×10316 .
Abramowitz, Milton ; Stegun, Irene Ann , eds. (1983) [June 1964]. "Chapter 5" . Handbook of Mathematical Functions with Formulas, Graphs, and Mathematical Tables . Applied Mathematics Series. Vol. 55 (Ninth reprint with additional corrections of tenth original printing with corrections (December 1972); first ed.). Washington D.C.; New York: United States Department of Commerce, National Bureau of Standards; Dover Publications. p. 228. ISBN 978-0-486-61272-0 . LCCN 64-60036 . MR 0167642 . LCCN 65-12253 .
Temme, N. M. (2010), "Exponential, Logarithmic, Sine, and Cosine Integrals" , in Olver, Frank W. J. ; Lozier, Daniel M.; Boisvert, Ronald F.; Clark, Charles W. (eds.), NIST Handbook of Mathematical Functions , Cambridge University Press, ISBN 978-0-521-19225-5 , MR 2723248 .