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Irrationality measure

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Rational approximations to the Square root of 2.

In mathematics, an irrationality measure of a real number {\displaystyle x} is a measure of how "closely" it can be approximated by rationals.

If a function {\displaystyle f(t,\lambda )}, defined for {\displaystyle t,\lambda >0}, takes positive real values and is strictly decreasing in both variables, consider the following inequality:

{\displaystyle 0<\left|x-{\frac {p}{q}}\right|<f(q,\lambda )}

for a given real number {\displaystyle x\in \mathbb {R} } and rational numbers {\displaystyle {\frac {p}{q}}} with {\displaystyle p\in \mathbb {Z} ,q\in \mathbb {Z} ^{+}}. Define {\displaystyle R} as the set of all {\displaystyle \lambda \in \mathbb {R} ^{+}} for which only finitely many {\displaystyle {\frac {p}{q}}} exist, such that the inequality is satisfied. Then {\displaystyle \lambda (x)=\inf R} is called an irrationality measure of {\displaystyle x} with regard to {\displaystyle f.} If there is no such {\displaystyle \lambda } and the set {\displaystyle R} is empty, {\displaystyle x} is said to have infinite irrationality measure {\displaystyle \lambda (x)=\infty }.

Consequently, the inequality

{\displaystyle 0<\left|x-{\frac {p}{q}}\right|<f(q,\lambda (x)+\varepsilon )}

has at most only finitely many solutions {\displaystyle {\frac {p}{q}}} for all {\displaystyle \varepsilon >0}.[1]

Irrationality exponent

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The irrationality exponent or Liouville–Roth irrationality measure is given by setting {\displaystyle f(q,\mu )=q^{-\mu }},[1] a definition adapting the one of Liouville numbers — the irrationality exponent {\displaystyle \mu (x)} is defined for real numbers {\displaystyle x} to be the supremum of the set of {\displaystyle \mu } such that {\displaystyle 0<\left|x-{\frac {p}{q}}\right|<{\frac {1}{q^{\mu }}}} is satisfied by an infinite number of coprime integer pairs {\displaystyle (p,q)} with {\displaystyle q>0}.[2][3]: 246 

For any value {\displaystyle n<\mu (x)}, the infinite set of all rationals {\displaystyle p/q} satisfying the above inequality yields good approximations of {\displaystyle x}. Conversely, if {\displaystyle n>\mu (x)}, then there are at most finitely many coprime {\displaystyle (p,q)} with {\displaystyle q>0} that satisfy the inequality.

For example, whenever a rational approximation {\displaystyle {\frac {p}{q}}\approx x} with {\displaystyle p,q\in \mathbb {N} } yields {\displaystyle n+1} exact decimal digits, then

{\displaystyle {\frac {1}{10^{n}}}\geq \left|x-{\frac {p}{q}}\right|\geq {\frac {1}{q^{\mu (x)+\varepsilon }}}}

for any {\displaystyle \varepsilon >0}, except for at most a finite number of "lucky" pairs {\displaystyle (p,q)}.

A number {\displaystyle x\in \mathbb {R} } with irrationality exponent {\displaystyle \mu (x)\leq 2} is called a diophantine number,[4] while numbers with {\displaystyle \mu (x)=\infty } are called Liouville numbers.

Corollaries

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Rational numbers have irrationality exponent 1, while (as a consequence of Dirichlet's approximation theorem) every irrational number has irrationality exponent at least 2.

On the other hand, an application of Borel-Cantelli lemma shows that almost all numbers, including all algebraic irrational numbers, have an irrationality exponent exactly equal to 2.[3]: 246 

It is {\displaystyle \mu (x)=\mu (rx+s)} for real numbers {\displaystyle x} and rational numbers {\displaystyle r\neq 0} and {\displaystyle s}. If for some {\displaystyle x} we have {\displaystyle \mu (x)\leq \mu }, then it follows {\displaystyle \mu (x^{1/2})\leq 2\mu }.[5]: 368 

For a real number {\displaystyle x} given by its simple continued fraction expansion {\displaystyle x=[a_{0};a_{1},a_{2},...]} with convergents {\displaystyle p_{i}/q_{i}} it holds:[1]

{\displaystyle \mu (x)=1+\limsup _{n\to \infty }{\frac {\ln q_{n+1}}{\ln q_{n}}}=2+\limsup _{n\to \infty }{\frac {\ln a_{n+1}}{\ln q_{n}}}.}

If we have {\displaystyle \limsup _{n\to \infty }{\tfrac {1}{n}}{\ln |q_{n}|}\leq \sigma } and {\displaystyle \lim _{n\to \infty }{\tfrac {1}{n}}{\ln |q_{n}x-p_{n}|}=-\tau } for some positive real numbers {\displaystyle \sigma ,\tau }, then we can establish an upper bound for the irrationality exponent of {\displaystyle x} by:[6][7]

{\displaystyle \mu (x)\leq 1+{\frac {\sigma }{\tau }}}

Known bounds

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For most transcendental numbers, the exact value of their irrationality exponent is not known.[5] Below is a table of known upper and lower bounds.

Number {\displaystyle x} Irrationality exponent {\displaystyle \mu (x)} Notes
Lower bound Upper bound
Rational number {\displaystyle p/q} with {\displaystyle p\in \mathbb {Z} ,q\in \mathbb {Z} ^{+}} 1 Every rational number {\displaystyle p/q} has an irrationality exponent of exactly 1.
Irrational algebraic number {\displaystyle \alpha } 2 By Roth's theorem the irrationality exponent of any irrational algebraic number is exactly 2. Examples include square roots and the golden ratio {\displaystyle \varphi }.
{\displaystyle e^{2/k},k\in \mathbb {Z} ^{+}} 2 If the elements {\displaystyle a_{n}} of the simple continued fraction expansion of an irrational number {\displaystyle x} are bounded above {\displaystyle a_{n}<P(n)} by an arbitrary polynomial {\displaystyle P}, then its irrationality exponent is {\displaystyle \mu (x)=2}.

Examples include numbers whose continued fractions behave predictably such as

{\displaystyle e=[2;1,2,1,1,4,1,1,6,1,...]} and {\displaystyle I_{0}(2)/I_{1}(2)=[1;2,3,4,5,6,7,8,9,10,...]}.

{\displaystyle \tan(1/k),k\in \mathbb {Z} ^{+}} 2
{\displaystyle \tanh(1/k),k\in \mathbb {Z} ^{+}} 2
{\displaystyle S(b)} with {\displaystyle b\geq 2} 2 {\displaystyle S(b):=\sum _{k=0}^{\infty }b^{-2^{k}}}with {\displaystyle b\in \mathbb {Z} }, has continued fraction terms which do not exceed a fixed constant.[8][9]
{\displaystyle T(b)} with {\displaystyle b\geq 2}[10] 2 {\displaystyle T(b):=\sum _{k=0}^{\infty }t_{k}b^{-k}} where {\displaystyle t_{k}} is the Thue–Morse sequence and {\displaystyle b\in \mathbb {Z} }. See Prouhet-Thue-Morse constant.
{\displaystyle \ln(2)}[11][12] 2 3.57455... There are other numbers of the form {\displaystyle \ln(a/b)} for which bounds on their irrationality exponents are known.[13][14][15]
{\displaystyle \ln(3)}[11][16] 2 5.11620...
{\displaystyle 5\ln(3/2)}[17] 2 3.43506... There are many other numbers of the form {\displaystyle {\sqrt {2k+1}}\ln \left({\frac {{\sqrt {2k+1}}+1}{{\sqrt {2k+1}}-1}}\right)} for which bounds on their irrationality exponents are known.[17] This is the case for {\displaystyle k=12}.
{\displaystyle \pi /{\sqrt {3}}}[18][19] 2 4.60105... There are many other numbers of the form {\displaystyle {\sqrt {2k-1}}\arctan \left({\frac {\sqrt {2k-1}}{k-1}}\right)} for which bounds on their irrationality exponents are known.[18] This is the case for {\displaystyle k=2}.
{\displaystyle \pi }[11][20] 2 7.10320... It has been proven that if the Flint Hills series {\displaystyle \displaystyle \sum _{n=1}^{\infty }{\frac {\csc ^{2}n}{n^{3}}}} (where n is in radians) converges, then {\displaystyle \pi }'s irrationality exponent is at most {\displaystyle 5/2}[21][22] and that if it diverges, the irrationality exponent is at least {\displaystyle 5/2}.[23]
{\displaystyle \pi ^{2}}[11][24] 2 5.09541... {\displaystyle \pi ^{2}} and {\displaystyle \zeta (2)} are linearly dependent over {\displaystyle \mathbb {Q} }. {\displaystyle \left(\zeta (2)={\frac {\pi ^{2}}{6}}\right)}, also see the Basel problem.
{\displaystyle \arctan(1/2)}[25] 2 9.27204... There are many other numbers of the form {\displaystyle \arctan(1/k)} for which bounds on their irrationality exponents are known.[26][27]
{\displaystyle \arctan(1/3)}[28] 2 5.94202...
Apéry's constant {\displaystyle \zeta (3)}[11] 2 5.51389...
{\displaystyle \Gamma (1/4)}[29] 2 10330
Cahen's constant {\displaystyle C}[30] 3
Champernowne constants {\displaystyle C_{b}} in base {\displaystyle b\geq 2}[31] {\displaystyle b} Examples include {\displaystyle C_{10}=0.1234567891011...=[0;8,9,1,149083,1,...]}
Liouville numbers {\displaystyle L} {\displaystyle \infty } The Liouville numbers are precisely those numbers having infinite irrationality exponent.[3]: 248 

Irrationality base

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The irrationality base or Sondow irrationality measure is obtained by setting {\displaystyle f(q,\beta )=\beta ^{-q}}.[1][6] It is a weaker irrationality measure, being able to distinguish how well different Liouville numbers can be approximated, but yielding {\displaystyle \beta (x)=1} for all other real numbers:

Let {\displaystyle x} be an irrational number. If there exist real numbers {\displaystyle \beta \geq 1} with the property that for any {\displaystyle \varepsilon >0}, there is a positive integer {\displaystyle q(\varepsilon )} such that

{\displaystyle \left|x-{\frac {p}{q}}\right|>{\frac {1}{(\beta +\varepsilon )^{q}}}}

for all integers {\displaystyle p,q} with {\displaystyle q\geq q(\varepsilon )} then the least such {\displaystyle \beta } is called the irrationality base of {\displaystyle x} and is represented as {\displaystyle \beta (x)}.

If no such {\displaystyle \beta } exists, then {\displaystyle \beta (x)=\infty } and {\displaystyle x} is called a super Liouville number.

If a real number {\displaystyle x} is given by its simple continued fraction expansion {\displaystyle x=[a_{0};a_{1},a_{2},...]} with convergents {\displaystyle p_{i}/q_{i}} then it holds:

{\displaystyle \beta (x)=\limsup _{n\to \infty }{\frac {\ln q_{n+1}}{q_{n}}}=\limsup _{n\to \infty }{\frac {\ln a_{n+1}}{q_{n}}}}.[1]

Examples

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Any real number {\displaystyle x} with finite irrationality exponent {\displaystyle \mu (x)<\infty } has irrationality base {\displaystyle \beta (x)=1}, while any number with irrationality base {\displaystyle \beta (x)>1} has irrationality exponent {\displaystyle \mu (x)=\infty } and is a Liouville number.

The number {\displaystyle L=[1;2,2^{2},2^{2^{2}},...]} has irrationality exponent {\displaystyle \mu (L)=\infty } and irrationality base {\displaystyle \beta (L)=1}.

The numbers {\displaystyle \tau _{a}=\sum _{n=0}^{\infty }{\frac {1}{^{n}a}}=1+{\frac {1}{a}}+{\frac {1}{a^{a}}}+{\frac {1}{a^{a^{a}}}}+{\frac {1}{a^{a^{a^{a}}}}}+...} ({\displaystyle {^{n}a}} represents tetration, {\displaystyle a=2,3,4...}) have irrationality base {\displaystyle \beta (\tau _{a})=a}.

The number {\displaystyle S=1+{\frac {1}{2^{1}}}+{\frac {1}{4^{2^{1}}}}+{\frac {1}{8^{4^{2^{1}}}}}+{\frac {1}{16^{8^{4^{2^{1}}}}}}+{\frac {1}{32^{16^{8^{4^{2^{1}}}}}}}+\ldots } has irrationality base {\displaystyle \beta (S)=\infty }, hence it is a super Liouville number.

Although it is not known whether or not {\displaystyle e^{\pi }} is a Liouville number,[32]: 20  it is known that {\displaystyle \beta (e^{\pi })=1}.[5]: 371 

Other irrationality measures

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Markov constant

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Setting {\displaystyle f(q,M)=(Mq^{2})^{-1}} gives a stronger irrationality measure: the Markov constant {\displaystyle M(x)}. For an irrational number {\displaystyle x\in \mathbb {R} \setminus \mathbb {Q} } it is the factor by which Dirichlet's approximation theorem can be improved for {\displaystyle x}. Namely if {\displaystyle c<M(x)} is a positive real number, then the inequality

{\displaystyle 0<\left|x-{\frac {p}{q}}\right|<{\frac {1}{cq^{2}}}}

has infinitely many solutions {\displaystyle {\frac {p}{q}}\in \mathbb {Q} }. If {\displaystyle c>M(x)} there are at most finitely many solutions.

Dirichlet's approximation theorem implies {\displaystyle M(x)\geq 1} and Hurwitz's theorem gives {\displaystyle M(x)\geq {\sqrt {5}}} both for irrational {\displaystyle x}.[33]

This is in fact the best general lower bound since the golden ratio gives {\displaystyle M(\varphi )={\sqrt {5}}}. It is also {\displaystyle M({\sqrt {2}})=2{\sqrt {2}}}.

Given {\displaystyle x=[a_{0};a_{1},a_{2},...]} by its simple continued fraction expansion, one may obtain:[34]

{\displaystyle M(x)=\limsup _{n\to \infty }{([a_{n+1};a_{n+2},a_{n+3},...]+[0;a_{n},a_{n-1},...,a_{2},a_{1}])}.}

Bounds for the Markov constant of {\displaystyle x=[a_{0};a_{1},a_{2},...]} can also be given by {\displaystyle {\sqrt {p^{2}+4}}\leq M(x)<p+2} with {\displaystyle p=\limsup _{n\to \infty }a_{n}}.[35] This implies that {\displaystyle M(x)=\infty } if and only if {\displaystyle (a_{k})} is not bounded and in particular {\displaystyle M(x)<\infty } if {\displaystyle x} is a quadratic irrational number. A further consequence is {\displaystyle M(e)=\infty }.

Any number with {\displaystyle \mu (x)>2} or {\displaystyle \beta (x)>1} has an unbounded simple continued fraction and hence {\displaystyle M(x)=\infty }.

For rational numbers {\displaystyle r} it may be defined {\displaystyle M(r)=0}.

Other results

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The values {\displaystyle M(e)=\infty } and {\displaystyle \mu (e)=2} imply that the inequality {\displaystyle 0<\left|e-{\frac {p}{q}}\right|<{\frac {1}{cq^{2}}}} has for all {\displaystyle c\in \mathbb {R} ^{+}} infinitely many solutions {\displaystyle {\frac {p}{q}}\in \mathbb {Q} } while the inequality {\displaystyle 0<\left|e-{\frac {p}{q}}\right|<{\frac {1}{q^{2+\varepsilon }}}} has for all {\displaystyle \varepsilon \in \mathbb {R} ^{+}} only at most finitely many solutions {\displaystyle {\frac {p}{q}}\in \mathbb {Q} } . This gives rise to the question what the best upper bound is. The answer is given by:[36]

{\displaystyle 0<\left|e-{\frac {p}{q}}\right|<{\frac {c\ln \ln q}{q^{2}\ln q}}}

which is satisfied by infinitely many {\displaystyle {\frac {p}{q}}\in \mathbb {Q} } for {\displaystyle c>{\tfrac {1}{2}}} but not for {\displaystyle c<{\tfrac {1}{2}}}.

This makes the number {\displaystyle e} alongside the rationals and quadratic irrationals an exception to the fact that for almost all real numbers {\displaystyle x\in \mathbb {R} } the inequality below has infinitely many solutions {\displaystyle {\frac {p}{q}}\in \mathbb {Q} }:[5] (see Khinchin's theorem)

{\displaystyle 0<\left|x-{\frac {p}{q}}\right|<{\frac {1}{q^{2}\ln q}}}

Mahler's generalization

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Kurt Mahler extended the concept of an irrationality measure and defined a so-called transcendence measure, drawing on the idea of a Liouville number and partitioning the transcendental numbers into three distinct classes.[3]

Mahler's irrationality measure

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Instead of taking for a given real number {\displaystyle x} the difference {\displaystyle |x-p/q|} with {\displaystyle p/q\in \mathbb {Q} }, one may instead focus on term {\displaystyle |qx-p|=|L(x)|} with {\displaystyle p,q\in \mathbb {Z} } and {\displaystyle L\in \mathbb {Z} [x]} with {\displaystyle \deg L=1}. Consider the following inequality:

{\displaystyle 0<|qx-p|\leq \max(|p|,|q|)^{-\omega }} with {\displaystyle p,q\in \mathbb {Z} } and {\displaystyle \omega \in \mathbb {R} _{0}^{+}}.

Define {\displaystyle R} as the set of all {\displaystyle \omega \in \mathbb {R} _{0}^{+}} for which infinitely many solutions {\displaystyle p,q\in \mathbb {Z} } exist, such that the inequality is satisfied. Then {\displaystyle \omega _{1}(x)=\sup M} is Mahler's irrationality measure. It gives {\displaystyle \omega _{1}(p/q)=0} for rational numbers, {\displaystyle \omega _{1}(\alpha )=1} for algebraic irrational numbers and in general {\displaystyle \omega _{1}(x)=\mu (x)-1}, where {\displaystyle \mu (x)} denotes the irrationality exponent.

Transcendence measure

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Mahler's irrationality measure can be generalized as follows:[2][3] Take {\displaystyle P} to be a polynomial with {\displaystyle \deg P\leq n\in \mathbb {Z} ^{+}} and integer coefficients {\displaystyle a_{i}\in \mathbb {Z} }. Then define a height function {\displaystyle H(P)=\max(|a_{0}|,|a_{1}|,...,|a_{n}|)} and consider for complex numbers {\displaystyle z} the inequality:

{\displaystyle 0<|P(z)|\leq H(P)^{-\omega }} with {\displaystyle \omega \in \mathbb {R} _{0}^{+}}.

Set {\displaystyle R} to be the set of all {\displaystyle \omega \in \mathbb {R} _{0}^{+}} for which infinitely many such polynomials exist, that keep the inequality satisfied. Further define {\displaystyle \omega _{n}(z)=\sup R} for all {\displaystyle n\in \mathbb {Z} ^{+}} with {\displaystyle \omega _{1}(z)} being the above irrationality measure, {\displaystyle \omega _{2}(z)} being a non-quadraticity measure, etc.

Then Mahler's transcendence measure is given by:

{\displaystyle \omega (z)=\limsup _{n\to \infty }\omega _{n}(z).}

The transcendental numbers can now be divided into the following three classes:

If for all {\displaystyle n\in \mathbb {Z} ^{+}} the value of {\displaystyle \omega _{n}(z)} is finite and {\displaystyle \omega (z)} is finite as well, {\displaystyle z} is called an S-number (of type {\displaystyle \omega (z)}).

If for all {\displaystyle n\in \mathbb {Z} ^{+}} the value of {\displaystyle \omega _{n}(z)} is finite but {\displaystyle \omega (z)} is infinite, {\displaystyle z} is called an T-number.

If there exists a smallest positive integer {\displaystyle N} such that for all {\displaystyle n\geq N} the {\displaystyle \omega _{n}(z)} are infinite, {\displaystyle z} is called an U-number (of degree {\displaystyle N}).

The number {\displaystyle z} is algebraic (and called an A-number) if and only if {\displaystyle \omega (z)=0}.

Almost all numbers are S-numbers. In fact, almost all real numbers give {\displaystyle \omega (x)=1} while almost all complex numbers give {\displaystyle \omega (z)={\tfrac {1}{2}}}.[37]: 86  The number e is an S-number with {\displaystyle \omega (e)=1}. The number π is either an S- or T-number.[37]: 86  The U-numbers are a set of measure 0 but still uncountable.[38] They contain the Liouville numbers which are exactly the U-numbers of degree one.

Linear independence measure

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Another generalization of Mahler's irrationality measure gives a linear independence measure.[2][13] For real numbers {\displaystyle x_{1},...,x_{n}\in \mathbb {R} } consider the inequality

{\displaystyle 0<|c_{1}x_{1}+...+c_{n}x_{n}|\leq \max(|c_{1}|,...,|c_{n}|)^{-\nu }} with {\displaystyle c_{1},...,c_{n}\in \mathbb {Z} } and {\displaystyle \nu \in \mathbb {R} _{0}^{+}}.

Define {\displaystyle R} as the set of all {\displaystyle \nu \in \mathbb {R} _{0}^{+}} for which infinitely many solutions {\displaystyle c_{1},...c_{n}\in \mathbb {Z} } exist, such that the inequality is satisfied. Then {\displaystyle \nu (x_{1},...,x_{n})=\sup R} is the linear independence measure.

If the {\displaystyle x_{1},...,x_{n}} are linearly dependent over {\displaystyle \mathbb {\mathbb {Q} } } then {\displaystyle \nu (x_{1},...,x_{n})=0}.

If {\displaystyle 1,x_{1},...,x_{n}} are linearly independent algebraic numbers over {\displaystyle \mathbb {\mathbb {Q} } } then {\displaystyle \nu (1,x_{1},...,x_{n})\leq n}.[32]

It is further {\displaystyle \nu (1,x)=\omega _{1}(x)=\mu (x)-1}.

Other generalizations

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Koksma’s generalization

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Jurjen Koksma in 1939 proposed another generalization, similar to that of Mahler, based on approximations of complex numbers by algebraic numbers.[3][37]

For a given complex number {\displaystyle z} consider algebraic numbers {\displaystyle \alpha } of degree at most {\displaystyle n}. Define a height function {\displaystyle H(\alpha )=H(P)}, where {\displaystyle P} is the characteristic polynomial of {\displaystyle \alpha } and consider the inequality:

{\displaystyle 0<|z-\alpha |\leq H(\alpha )^{-\omega ^{*}-1}} with {\displaystyle \omega ^{*}\in \mathbb {R} _{0}^{+}}.

Set {\displaystyle R} to be the set of all {\displaystyle \omega ^{*}\in \mathbb {R} _{0}^{+}} for which infinitely many such algebraic numbers {\displaystyle \alpha } exist, that keep the inequality satisfied. Further define {\displaystyle \omega _{n}^{*}(z)=\sup R} for all {\displaystyle n\in \mathbb {Z} ^{+}} with {\displaystyle \omega _{1}^{*}(z)} being an irrationality measure, {\displaystyle \omega _{2}^{*}(z)} being a non-quadraticity measure,[17] etc.

Then Koksma's transcendence measure is given by:

{\displaystyle \omega ^{*}(z)=\limsup _{n\to \infty }\omega _{n}^{*}(z)}.

The complex numbers can now once again be partitioned into four classes A*, S*, T* and U*. However it turns out that these classes are equivalent to the ones given by Mahler in the sense that they produce exactly the same partition.[37]: 87 

Simultaneous approximation of real numbers

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Given a real number {\displaystyle x\in \mathbb {R} }, an irrationality measure of {\displaystyle x} quantifies how well it can be approximated by rational numbers {\displaystyle {\frac {p}{q}}} with denominator {\displaystyle q\in \mathbb {Z} ^{+}}. If {\displaystyle x=\alpha } is taken to be an algebraic number that is also irrational one may obtain that the inequality

{\displaystyle 0<\left|\alpha -{\frac {p}{q}}\right|<{\frac {1}{q^{\mu }}}}

has only at most finitely many solutions {\displaystyle {\frac {p}{q}}\in \mathbb {Q} } for {\displaystyle \mu >2}. This is known as Roth's theorem.

This can be generalized: Given a set of real numbers {\displaystyle x_{1},...,x_{n}\in \mathbb {R} } one can quantify how well they can be approximated simultaneously by rational numbers {\displaystyle {\frac {p_{1}}{q}},...,{\frac {p_{n}}{q}}} with the same denominator {\displaystyle q\in \mathbb {Z} ^{+}}. If the {\displaystyle x_{i}=\alpha _{i}} are taken to be algebraic numbers, such that {\displaystyle 1,\alpha _{1},...,\alpha _{n}} are linearly independent over the rational numbers {\displaystyle \mathbb {Q} } it follows that the inequalities

{\displaystyle 0<\left|\alpha _{i}-{\frac {p_{i}}{q}}\right|<{\frac {1}{q^{\mu }}},\forall i\in \{1,...,n\}}

have only at most finitely many solutions {\displaystyle \left({\frac {p_{1}}{q}},...,{\frac {p_{n}}{q}}\right)\in \mathbb {Q} ^{n}} for {\displaystyle \mu >1+{\frac {1}{n}}}. This result is due to Wolfgang M. Schmidt.[39][40]

See also

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References

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Irrationality measure
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