Birch and Swinnerton-Dyer conjecture: Difference between revisions

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In [[number theory]], [[Aleksandr Yakovlevich Khinchin]] proved that for [[almost all]] real numbers ''x'', coefficients ''a''<sub>''i''</sub> of the [[continued fraction]] expansion of ''x'' have a finite [[geometric mean]] that is independent of the value of ''x'' and is known as '''Khinchin's constant'''.
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That is, for
 
:<math>x = a_0+\cfrac{1}{a_1+\cfrac{1}{a_2+\cfrac{1}{a_3+\cfrac{1}{\ddots}}}}\;</math>
 
it is [[almost all|almost always]] true that
 
:<math>\lim_{n \rightarrow \infty } \left( \prod_{i=1}^n a_i \right) ^{1/n} =
K_0</math>
where <math>\prod</math> is [[Multiplication#Capital_Pi_notation|sequence multiplication]] <math>( a_1 * a_2 * ... a_n )</math> and <math>K_0</math> is Khinchin's constant
:<math>K_0 =
\prod_{r=1}^\infty {\left( 1+{1\over r(r+2)}\right)}^{\log_2 r}  \approx 2.6854520010\dots</math> {{OEIS|id=A002210}}.
 
Among the numbers ''x'' whose continued fraction expansions do ''not'' have this property are [[rational number]]s, solutions of [[quadratic equation]]s with rational coefficients (including the [[golden ratio]] &Phi;), and the [[e (mathematical constant)|base of the natural logarithm]] ''e''.
 
Khinchin is sometimes spelled Khintchine (the French transliteration of Russian Хи́нчин) in older mathematical literature.
 
==Sketch of proof==
The proof presented here was arranged by {{harvtxt|Ryll-Nardzewski|1951}} and is much simpler than Khinchin's original proof which did not use [[ergodic theory]].
 
Since the first coefficient ''a''<sub>0</sub> of the continued fraction of ''x'' plays no role in Khinchin's theorem and since the [[rational numbers]] have [[Lebesgue measure]] zero, we are reduced to the study of irrational numbers in the [[unit interval]], i.e., those in <math>\scriptstyle I=[0,1]\setminus\mathbb{Q}</math>. These numbers are in [[bijection]] with infinite [[continued fraction]]s of the form [0;&nbsp;''a''<sub>1</sub>,&nbsp;''a''<sub>2</sub>,&nbsp;...], which we simply write [''a''<sub>1</sub>,&nbsp;''a''<sub>2</sub>,&nbsp;...], where ''a''<sub>1</sub>, ''a''<sub>2</sub>,&nbsp;... are [[positive integer]]s. Define a transformation ''T'':''I''&nbsp;&rarr;&nbsp;''I'' by
 
:<math>T([a_1,a_2,\dots])=[a_2,a_3,\dots].\,</math>
 
The transformation ''T'' is called the [[Gauss–Kuzmin–Wirsing operator]]. For every [[Borel set|Borel subset]] ''E'' of ''I'', we also define the [[Gauss–Kuzmin distribution|Gauss&ndash;Kuzmin measure]] of ''E''
 
:<math>\mu(E)=\frac{1}{\log 2}\int_E\frac{dx}{1+x}.</math>
 
Then ''&mu;'' is a [[probability measure]] on the [[Sigma-algebra|''&sigma;''-algebra]] of Borel subsets of ''I''. The measure ''&mu;'' is [[Equivalence (measure theory)|equivalent]] to the Lebesgue measure on ''I'', but it has the additional property that the transformation ''T'' [[measure-preserving transformation|preserves]] the measure ''&mu;''. Moreover, it can be proved that ''T'' is an [[ergodic transformation]] of the [[measurable space]] ''I'' endowed with the probability measure ''&mu;'' (this is the hard part of the proof). The [[ergodic theorem]] then says that for any ''&mu;''-[[integrable function]] ''f'' on ''I'', the average value of <math>f \left( T^k x \right)</math> is the same for almost all <math>x</math>:
 
:<math>\lim_{n\to\infty} \frac 1n\sum_{k=0}^{n-1}(f\circ T^k)(x)=\int_I f d\mu\quad\text{for }\mu\text{-almost all }x\in I.</math>
 
Applying this to the function defined by ''f''([''a''<sub>1</sub>,&nbsp;''a''<sub>2</sub>,&nbsp;...]) = log(''a''<sub>1</sub>), we obtain that
 
:<math>\lim_{n\to\infty}\frac 1n\sum_{k=1}^{n}\log(a_k)=\int_I f \, d\mu = \sum_{r=1}^\infty\log(r)\frac{\log\bigl(1+\frac{1}{r(r+2)}\bigr)}{\log 2}</math>
 
for almost all [''a''<sub>1</sub>,&nbsp;''a''<sub>2</sub>,&nbsp;...] in ''I'' as ''n''&nbsp;&rarr;&nbsp;&infin;.
 
Taking the [[exponential function|exponential]] on both sides, we obtain to the left the [[geometric mean]] of the first ''n'' coefficients of the continued fraction, and to the right Khinchin's constant.
 
==Series expressions==
Khinchin's constant may be expressed as a [[rational zeta series]] in the form
 
:<math>\log K_0 = \frac{1}{\log 2} \sum_{n=1}^\infty
\frac {\zeta (2n)-1}{n} \sum_{k=1}^{2n-1} \frac{(-1)^{k+1}}{k}
</math>
or, by peeling off terms in the series,
:<math>\log K_0 = \frac{1}{\log 2} \left[
\sum_{k=3}^N \log \left(\frac{k-1}{k} \right) \log \left(\frac{k+1}{k} \right)
+ \sum_{n=1}^\infty
\frac {\zeta (2n,N)}{n} \sum_{k=1}^{2n-1} \frac{(-1)^{k+1}}{k}
\right]
</math>
 
where ''N'' is an integer, held fixed, and &zeta;(''s'',&nbsp;''n'') is the [[Hurwitz zeta function]]. Both series are strongly convergent, as &zeta;(''n'')&nbsp;&minus;&nbsp;1 approaches zero quickly for large ''n''.  An expansion may also be given in terms of the [[dilogarithm]]:
 
:<math>\log K_0 = \log 2 + \frac{1}{\log 2} \left[
\mbox{Li}_2 \left( \frac{-1}{2} \right) +
\frac{1}{2}\sum_{k=2}^\infty (-1)^k \mbox{Li}_2 \left( \frac{4}{k^2} \right)
\right].
</math>
 
==Hölder means==
The Khinchin constant can be viewed as the first in a series of the [[Hölder mean]]s of the terms of continued fractions.  Given an arbitrary series {''a''<sub>''n''</sub>}, the Hölder mean of order ''p'' of the series is given by
 
:<math>K_p=\lim_{n\to\infty} \left[\frac{1}{n}
\sum_{k=1}^n a_k^p \right]^{1/p}.</math>
 
When the {''a''<sub>''n''</sub>} are the terms of a continued fraction expansion, the constants are given by
 
:<math>K_p=\left[\sum_{k=1}^\infty -k^p
\log_2\left( 1-\frac{1}{(k+1)^2} \right)
\right]^{1/p}.</math>
 
This is obtained by taking the ''p''-th mean in conjunction with the [[Gauss–Kuzmin distribution]].  The value for ''K''<sub>0</sub> may be shown to be obtained in the limit of ''p''&nbsp;&rarr;&nbsp;0.
 
==Harmonic mean==
By means of the above expressions, the [[harmonic mean]] of the terms of a continued fraction may be obtained as well.  The value obtained is
 
:<math>K_{-1}=1.74540566240\dots</math> {{OEIS|A087491}}.
 
==Open problems==
* Among the numbers whose geometric mean of the coefficients ''a''<sub>''i''</sub> in the continued fraction expansion apparently (based on numerical evidence) tends to Khinchin's constant are [[pi|{{pi}}]], the [[Euler–Mascheroni constant]] &gamma;, and Khinchin's constant itself.  However, none of these limits has been rigorously established, even though it is known that [[almost all]] real numbers have this property.
* It is not known if Khinchin's constant is a rational, [[Algebraic numbers|algebraic]] [[Irrational numbers|irrational]] or [[Transcendental numbers|transcendental]] number.<ref>{{MathWorld|urlname=KhinchinsConstant|title=Khinchin's constant}}</ref>
 
==See also==
* [[Lévy's constant]]
 
==References==
* {{cite journal|author=David H. Bailey, Jonathan M. Borwein, Richard E. Crandall
|url=http://www.reed.edu/~crandall/papers/95-036-Bailey-Borwein-Crandall.pdf
|title=On the Khinchine constant
|journal=
|year=1995
|volume=
|pages=
}}
 
* {{cite journal|author=Jonathan M. Borwein, David M. Bradley, Richard E. Crandall
|url=http://www.maths.ex.ac.uk/~mwatkins/zeta/borwein1.pdf
|title=Computational Strategies for the Riemann Zeta Function
|journal=J. Comp. App. Math.
|year=2000
|volume=121
|pages=p.11
}}
 
* {{cite book|author=Aleksandr Ya. Khinchin|title=Continued Fractions|publisher=Dover Publications|location=New York|year=1997}}
 
* {{citation|last=Ryll-Nardzewski|first=Czesław|title=On the ergodic theorems II (Ergodic theory of continued fractions)|journal=Studia Mathematica|volume=12|year=1951|pages=74&ndash;79}}
 
<references/>
 
==External links==
* [http://pi.lacim.uqam.ca/piDATA/khintchine.txt 110,000 digits of Khinchin's constant]
* [http://mpmath.googlecode.com/svn/data/khinchin.txt 10,000 digits of Khinchin's constant]
 
[[Category:Continued fractions]]
[[Category:Mathematical constants]]

Latest revision as of 18:45, 24 November 2014

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