In number theory, specifically in Diophantine approximation theory, the Markov constant \( {\displaystyle M(\alpha )} \) of an irrational number \( \alpha \) is the factor for which Dirichlet's approximation theorem can be improved for \( \alpha \) .
History and motivation
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Certain numbers can be approximated well by certain rationals; specifically, the convergents of the continued fraction are the best approximations by rational numbers having denominators less than a certain bound. For example, the approximation \( {\displaystyle \pi \approx {\frac {22}{7}}} \)is the best rational approximation among rational numbers with denominator up to 56.[1] Also, some numbers can be approximated more readily than others. Dirichlet proved in 1840[2] that the least readily approximable numbers are the rational numbers, in the sense that for every irrational number there exists infinitely many rational numbers approximating it to a certain degree of accuracy that only finitely many such rational approximations exist for rational numbers[further explanation needed]. Specifically, he proved that for any number \( \alpha \) there are infinitely many pairs of relatively prime numbers ( (p,q) such that \( {\displaystyle \left|\alpha -{\frac {p}{q}}\right|<{\frac {1}{q^{2}}}} \) if and only if \( \alpha \) is irrational.
51 years later, Hurwitz further improved Dirichlet's approximation theorem by a factor of √5,[3] improving the right-hand side from \( {\displaystyle 1/q^{2}} \) to \( {\displaystyle 1/{\sqrt {5}}q^{2}} \) for irrational numbers:
\( \left|\alpha - \frac{p}{q}\right| < \frac{1}{\sqrt{5}q^2}. \)
The above result is best possible since the golden ratio \( \phi \) is irrational but if we replace √5 by any larger number in the above expression then we will only be able to find finitely many rational numbers that satisfy the inequality for \( {\displaystyle \alpha =\phi }. \)
Furthermore, he showed that among the irrational numbers, the least readily approximable numbers are those of the form \( {\displaystyle {\frac {a\phi +b}{c\phi +d}}} \) where \( \phi \) is the golden ratio, \( {\displaystyle a,b,c,d\in \mathbb {Z} } \) and \( {\displaystyle ad-bc=\pm 1} \).[4] (These numbers are said to be equivalent to \( \phi \) .) If we omit these numbers, just as we omitted the rational numbers in Dirichlet's theorem, then we can increase the number √5 to 2√2. Again this new bound is best possible in the new setting, but this time the number √2, and numbers equivalent to it, limits the bound.[4] If we don't allow those numbers then we can again increase the number on the right hand side of the inequality from 2√2 to √221/5,[4] for which the numbers equivalent to \( {\displaystyle {\frac {1+{\sqrt {221}}}{10}}}\) limits the bound. The numbers generated show how well these numbers can be approximated, this can be seen as a property of the real numbers.
However, instead of considering Hurwitz's theorem (and the extensions mentioned above) as a property of the real numbers except certain special numbers, we can consider it as a property of each excluded number. Thus, the theorem can be interpreted as "numbers equivalent to \( \phi \) , \( {\displaystyle {\frac {1+{\sqrt {221}}}{10}}} \)are among the least readily approximable irrational numbers." This leads us to consider how accurately each number can be approximated by rationals - specifically, by how much can the factor in Dirichlet's approximation theorem be increased to from 1 for that specific number.
Definition
Mathematically, the Markov constant of irrational \( \alpha \) is defined as \( {\displaystyle M(\alpha )=\sup\{\lambda \in \mathbb {R} |\left\vert \alpha -{\frac {p}{q}}\right\vert <{\frac {1}{\lambda q^{2}}}{\text{ has infinitely many solutions for }}p,q\in \mathbb {N} \}} \).[5] If the set does not have an upper bound we define \( {\displaystyle M(\alpha )=\infty }. \)
Alternatively, it can be defined as \( {\displaystyle \limsup _{k\to \infty }{\frac {1}{k^{2}\left\vert \alpha -{\frac {f(k)}{k}}\right\vert }}} \) where f(k) is defined as the closest integer to \( {\displaystyle \alpha k}. \)
Properties and results
Hurwitz's theorem implies that \( {\displaystyle M(\alpha )\geq {\sqrt {5}} \) } for all \( \alpha \in \mathbb{R} . \)
If \( {\displaystyle \alpha =[a_{0};a_{1},a_{2},...]} \) is its continued fraction expansion then \( {\displaystyle M(\alpha )=\limsup _{k\to \infty }{([a_{k};a_{k+1},a_{k+2},...]+[0;a_{k-1},a_{k-2},...,a_{1},a_{0}])}} \) .[5]
From the above, if \( {\displaystyle p=\limsup _{k\to \infty }{a_{k}}} \) then \( {\displaystyle p<M(\alpha )<p+2} \) . This implies that \( {\displaystyle M(\alpha )=\infty } \) if and only if \( (a_{k}) \) is not bounded. In particular, \( {\displaystyle M(\alpha )<\infty } \) if \( \alpha \) is a quadratic irrationality. In fact, the lower bound for \( {\displaystyle M(\alpha )} \) can be strengthened to \( {\displaystyle M(\alpha )\geq {\sqrt {p^{2}+4}}} \), the tightest possible.[6]
The values of \( \alpha \) for which \( {\displaystyle M(\alpha )<3} \)are families of quadratic irrationalities having the same period (but at different offsets), and the values of \( {\displaystyle M(\alpha )} \) for these \( \alpha \) are limited to Lagrange numbers. There are uncountably many numbers for which \( {\displaystyle M(\alpha )=3} \), no two of which have the same ending; for instance, for each number \( {\displaystyle \alpha =[\underbrace {1;1,...,1} _{r_{1}},2,2,\underbrace {1;1,...,1} _{r_{2}},2,2,\underbrace {1;1,...,1} _{r_{3}},2,2,...]} \) where \( {\displaystyle r_{1}<r_{2}<r_{3}<\cdots } \) , \( {\displaystyle M(\alpha )=3} \) .[5]
If \( {\displaystyle \beta ={\frac {p\alpha +q}{r\alpha +s}}} \) where \( {\displaystyle p,q,r,s\in \mathbb {Z} } \) then \( {\displaystyle M(\beta )\geq {\frac {M(\alpha )}{\left\vert ps-rq\right\vert }}} \).[7] In particular if \( {\displaystyle \left\vert ps-rq\right\vert =1} \) them \( {\displaystyle M(\beta )=M(\alpha )} \).[8]
The set \( {\displaystyle L=\{M(\alpha )|\alpha \in \mathbb {R} -\mathbb {Q} \}} \) forms the Lagrange spectrum. It contains the interval \( {\displaystyle [F,\infty ]} \) where F is Freiman's constant.[8] Hence, if \( {\displaystyle m>F\approx 4.52783} \) then there exists irrational \( \alpha \) whose Markov constant is m {\displaystyle m} m.
Numbers having a Markov constant less than 3
Burger et al. (2002)[9] provides a formula for which the quadratic irrationality \( {\displaystyle \alpha _{n}} \) whose Markov constant is the nth Lagrange number:
\( {\displaystyle \alpha _{n}={\frac {2u-3m_{n}+{\sqrt {9m_{n}^{2}-4}}}{2m_{n}}}} \) where \( m_{n} \) is the nth Markov number, and u is the smallest positive integer such that \( {\displaystyle m_{n}\mid u^{2}+1}. \)
Nicholls (1978)[10] provides a geometric proof of this (based on circles tangent to each other), providing a method that these numbers can be systematically found.
Examples
A demonstration that √10/2 has Markov constant √10, as stated in the example below. This plot graphs y(k) = 1/k2|α-f(αk)/k| against log(k) (the natural log of k) where f(x) is the nearest integer to x. The dots at the top corresponding to an x-axis value of 0.7, 2.5, 4.3 and 6.1 (k=2,12,74,456) are the points for which the limit superior of √10 is approached.
Markov constant of a number
Since \( {\displaystyle {\frac {\sqrt {10}}{2}}=[1;{\overline {1,1,2}}]}, \)
\( {\displaystyle {\begin{aligned}M\left({\frac {\sqrt {10}}{2}}\right)&=\max([1;{\overline {2,1,1}}]+[0;{\overline {1,2,1}}],[1;{\overline {1,2,1}}]+[0;{\overline {2,1,1}}],[2;{\overline {1,1,2}}]+[0;{\overline {1,1,2}}])\\&=\max \left({\frac {2{\sqrt {10}}}{3}},{\frac {2{\sqrt {10}}}{3}},{\sqrt {10}}\right)\\&={\sqrt {10}}.\end{aligned}}} \)
As \( {\displaystyle e=[2;1,2,1,1,4,1,1,6,1,\ldots ,1,2n,1,\ldots ],M(e)=\infty } \) because the continued fraction representation of e is unbounded.
Numbers α n {\displaystyle \alpha _{n}} \alpha_n having Markov constant less than 3
Consider n=6; Then \( {\displaystyle m_{n}=34} \). By trial and error it can be found that \( {\displaystyle u=13} \). Then
\( {\displaystyle {\begin{aligned}\alpha _{6}&={\frac {2u-3m_{6}+{\sqrt {9m_{6}^{2}-4}}}{2m_{6}}}\\[6pt]&={\frac {-76+{\sqrt {10400}}}{68}}\\[6pt]&={\frac {-19+5{\sqrt {26}}}{17}}\\[6pt]&=[0;{\overline {2,1,1,1,1,1,1,2}}].\end{aligned}}} \)
See also
Lagrange number
Continued fraction
Lagrange spectrum
References
Fernando, Suren L. (27 July 2001). "A063673 (Denominators of sequence {3/1, 13/4, 16/5, 19/6, 22/7, 179/57, 201/64, 223/71, 245/78, 267/85, 289/92, 311/99, 333/106, ... } of approximations to Pi with increasing denominators, where each approximation is an improvement on its predecessors.)". The On-Line Encyclopedia of Integer Sequences. Retrieved 2 December 2019.
Koro (22 March 2013). "Dirichlet's approximation theorem". Planet Math. Retrieved 21 November 2019.
Hurwitz, A. (1891). "Ueber die angenäherte Darstellung der Irrationalzahlen durch rationale Brüche (On the approximate representation of irrational numbers by rational fractions)". Mathematische Annalen (in German). 39 (2): 279–284. doi:10.1007/BF01206656. JFM 23.0222.02. contains the actual proof in German.
Weisstein, Eric W. (25 November 2019). "Hurwitz's Irrational Number Theorem". Wolfram Mathworld. Retrieved 2 December 2019.
LeVeque, William (1977). Fundamentals of Number Theory. Addison-Wesley Publishing Company, Inc. pp. 251–254. ISBN 0-201-04287-8.
Hancl, Jaroslav (January 2016). "Second basic theorem of Hurwitz". Lithuanian Mathematical Journal. 56: 72–76. doi:10.1007/s10986-016-9305-4.
Pelantová, Edita; Starosta, Štěpán; Znojil, Miloslav (2016). "Markov constant and quantum instabilities". Journal of Physics A: Mathematical and Theoretical. 49 (15): 155201. arXiv:1510.02407. Bibcode:2016JPhA...49o5201P. doi:10.1088/1751-8113/49/15/155201.
Hazewinkel, Michiel (1990). Encyclopaedia of Mathematics. Springer Science & Business Media. p. 106. ISBN 9781556080050.
Burger, Edward B.; Folsom, Amanda; Pekker, Alexander; Roengpitya, Rungporn; Snyder, Julia (2002). "On a quantitative refinement of the Lagrange spectrum". Acta Arithmetica. 102 (1): 59–60. Bibcode:2002AcAri.102...55B. doi:10.4064/aa102-1-5.
Nicholls, Peter (1978). "Diophantine Approximation via the Modular Group". Journal of the London Mathematical Society. Second Series. 17: 11–17.
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