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Eric Kvaalen (talk | contribs) The 3D graph doesn't correstpond to the real function between 0 and 1. The series should not take the absolute value of u in the meromorphic case. |
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{{Use American English|date = January 2019}}▼
{{Short description|Special function defined by an integral}}
{{Redirect|Li(x)|the polylogarithm denoted by Li<sub>''s''</sub>(''z'')|Polylogarithm}}
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 theory|number theoretic]] significance. In particular, according to the [[Siegel-Walfisz theorem]] it is a very good [[approximation]] to the [[prime-counting function]], which is defined as the number of [[prime numbers]] less than a given value <math>x</math>. [[Image:Logarithmic integral function.svg|thumb|right|300px|Logarithmic integral function plot]]▼
▲{{Use American English|date = January 2019}}
[[File: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.svg|alt=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|thumb|Plot of the absolute value of the logarithmic integral function li(z) in the complex plane from -2-2i to 2+2i with colors showing the argument (the angle around the complex plane)]]
▲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 theory|number theoretic]] significance. In particular, according to the [[
== Integral representation ==
The logarithmic integral has an integral representation defined for all positive [[real number]]s {{mvar|x}} ≠ 1 by the [[integral|definite integral]]
: <math> \operatorname{li}(x) =
Here, {{math|ln}} denotes the [[natural logarithm]]. The function {{math|1/
: <math> \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)
However, the logarithmic integral can also be taken to be a [[meromorphic]] complex-valued function in the complex ___domain. In this case it is multi-valued with branch points at 0 and 1, and the values between 0 and 1 defined by the above integral are not compatible with the values beyond 1. The complex function is shown in the figure above. The values on the real axis beyond 1 are the same as defined above, but the values between 0 and 1 are offset by iπ so that the absolute value at 0 is π rather than zero. The complex function is also defined (but multi-valued) for numbers with negative real part, but on the negative real axis the values are not real.
▲Here, {{math|ln}} denotes the [[natural logarithm]]. The function {{math|1/ln(''t'')}} has a [[mathematical singularity|singularity]] at {{mvar|t}} = 1, and the integral for {{mvar|x}} > 1 has to be interpreted as a ''[[Cauchy principal value]]'',
▲:<math> \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)~.</math>
== Offset logarithmic integral ==
The '''offset logarithmic integral''' or '''Eulerian logarithmic integral''' is defined as
: <math> \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.▼
▲:<math> \operatorname{Li}(x) = \operatorname{li}(x) - \operatorname{li}(2) \, </math>
Equivalently,
: <math> \operatorname{
▲:<math> \operatorname{Li}(x) = \int_2^x \frac{dt}{\ln t} \, </math>
▲As such, the integral representation has the advantage of avoiding the singularity in the ___domain of integration.
== Special values ==
The function li(''x'') has a single positive zero; it occurs at ''x'' ≈ 1.45136 92348 83381 05028 39684 85892 02744 94930... {{OEIS2C|A070769}}; this number is known as the [[Ramanujan–Soldner constant]].
This is <math>-(\Gamma
== Series representation ==
The function li(''x'') is related to the ''[[exponential integral]]'' Ei(''x'') via the equation
▲:<math>\hbox{li}(x)=\hbox{Ei}(\ln x) , \,\!</math>
which is valid for ''x'' > 0. This identity provides a series representation of li(''x'') as
: <math> \operatorname{li}(e^u) = \hbox{Ei}(u) =
\gamma + \ln |u| + \sum_{n=1}^\infty {u^{n}\over n \cdot n!}
\quad \text{ for } u \ne 0 \
where ''γ'' ≈ 0.57721 56649 01532 ... {{OEIS2C|id=A001620}} is the [[Euler–Mascheroni constant]].
:<math>▼
\gamma + \ln u + \sum_{n=1}^\infty {u^{n}\over n \cdot n!}
\quad \text{ for } u \ne 0 \, , </math>
(without taking the absolute value of u).
A more rapidly convergent series by [[Srinivasa Ramanujan|Ramanujan]] <ref>{{MathWorld | urlname=LogarithmicIntegral | title=Logarithmic Integral}}</ref> is
▲: <math>
\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).
</math>
<!-- cribbed from Mathworld, which cites
Berndt, B. C. Ramanujan's Notebooks, Part IV. New York: Springer-Verlag, pp. 126–131, 1994.
-->
Again, for the meromorphic complex function the term <math>\ln|\ln u|</math> must be replaced by <math>\ln\ln u.</math>
== Asymptotic expansion ==
The asymptotic behavior both for
▲:<math> \operatorname{li}(x) = O \left( {x\over \ln x} \right) \; . </math>
where <math>O</math> is the [[big O notation]]. The full [[asymptotic expansion]] is
: <math> \operatorname{li}(x) \sim \frac{x}{\ln x} \sum_{k=0}^\infty \frac{k!}{(\ln x)^k} </math>▼
▲:<math> \operatorname{li}(x) \sim \frac{x}{\ln x} \sum_{k=0}^\infty \frac{k!}{(\ln x)^k} </math>
or
: <math> \frac{\operatorname{li}(x)}{x/\ln x} \sim 1 + \frac{1}{\ln x} + \frac{2}{(\ln x)^2} + \frac{6}{(\ln x)^3} + \cdots. </math>▼
▲:<math> \frac{\operatorname{li}(x)}{x/\ln x} \sim 1 + \frac{1}{\ln x} + \frac{2}{(\ln x)^2} + \frac{6}{(\ln x)^3} + \cdots. </math>
This gives the following more accurate asymptotic behaviour:
: <math> \operatorname{li}(x) - \frac{x
▲:<math> \operatorname{li}(x) - {x\over \ln x} = O \left( {x\over \ln^2 x} \right) \; . </math>
▲Note that, as an asymptotic expansion, this series is [[divergent series|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:
: <math> 1+\frac{1}{\ln x} < \operatorname{li}(x)
== Number theoretic significance ==▼
▲:<math> 1+\frac{1}{\ln x} < \operatorname{li}(x) \frac{\ln x}{x} < 1+\frac{1}{\ln x}+\frac{3}{(\ln x)^2} </math>
▲For all <math>\ln x \ge 11</math>.
▲==Number theoretic significance==
The logarithmic integral is important in [[number theory]], appearing in estimates of the number of [[prime number]]s less than a given value. For example, the [[prime number theorem]] states that:
where <math>\pi(x)</math> denotes the number of primes smaller than or equal to <math>x</math>. ▼
Assuming the [[Riemann
▲:<math>\pi(x)\sim\operatorname{Li}(x)</math>
: <math>|\operatorname{li}(x)-\pi(x)| = O(\sqrt{x}\log x)</math>
In fact, the [[Riemann hypothesis]] is equivalent to the statement that:
▲where <math>\pi(x)</math> denotes the number of primes smaller than or equal to <math>x</math>.
: <math>|\operatorname{li}(x)-\pi(x)| = O(x^{1/2+a})</math> for any <math>a>0</math>.
For small <math>x</math>, <math>\operatorname{li}(x)>\pi(x)</math> but the difference changes sign an infinite number of times as <math>x</math> increases, and the [[Skewes's number|first time that this happens]] is somewhere between 10<sup>19</sup> and {{val|1.4|e=316}}.
▲Assuming Riemann's hypothesis, we get the even stronger:<ref>Abramowitz and Stegun, p. 230, 5.1.20</ref>
▲:<math>\operatorname{Li}(x)-\pi(x) = O(\sqrt{x}\log x)</math>
== See also ==
* [[Jørgen Pedersen Gram]]
* [[Skewes' number]]
* [[List of integrals of logarithmic functions]]
== References ==
{{reflist}}
* {{AS ref|5|228}}
* {{dlmf|id=6|title=Exponential, Logarithmic, Sine, and Cosine Integrals|first=N. M. |last=Temme}}
{{Nonelementary Integral}}
{{Authority control}}
[[Category:Special hypergeometric functions]]
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