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{{for|the generalization of hypergeometric series |MacRobert E function}}
In [[mathematics]], ''E-functions'' are a type of [[power series]] that satisfy particular systems of linear differential equations.
In [[mathematics]], '''E-functions''' are a type of [[power series]] that satisfy particular arithmetic conditions on the coefficients. They are of interest in [[transcendental number theory]], and are closely related to [[G-function (power series)|G-function]]s.


==Definition==
==Definition==


A power series with coefficients in the field of algebraic numbers
A function ''f''(''x'') is called of '''type ''E''''', or an '''''E''-function'''<ref>Carl Ludwig Siegel, ''Transcendental Numbers'', p.33, Princeton University Press, 1949.</ref>, if the power series


:<math>f(x)=\sum_{n=0}^{\infty} c_{n}\frac{x^{n}}{n!}</math>
:<math>f(x)=\sum_{n=0}^\infty c_n \frac{x^n}{n!} \in \overline{\mathbb{Q}}[\![x]\!]</math>


satisfies the following three conditions:
is called an '''{{math|1=''E''}}-function'''<ref>Carl Ludwig Siegel, ''Transcendental Numbers'', p.33, Princeton University Press, 1949.</ref> if it satisfies the following three conditions:


* All the coefficients ''c<sub>n</sub>'' belong to the same [[algebraic number field]], ''K'', which has [[Degree of a field extension|finite degree]] over the rational numbers;
* It is a solution of a non-zero linear differential equation with polynomial coefficients (this implies that all the coefficients {{math|1=''c<sub>n</sub>''}} belong to the same [[algebraic number field]], {{math|1=''K''}}, which has [[Degree of a field extension|finite degree]] over the rational numbers);
* For all <math> \varepsilon>0</math>,&nbsp;&nbsp;&nbsp;<math>\overline{\left|c_n\right|}=O\left(n^{n\varepsilon}\right),</math>
* For all &epsilon;&nbsp;&gt;&nbsp;0,
: where the left hand side represents the maximum of the absolute values of all the [[Conjugate element (field theory)|algebraic conjugates]] of {{math|1=''c<sub>n</sub>''}};
:<math>\overline{\left|c_{n}\right|}=O\left(n^{n\varepsilon}\right)</math>,
* For all <math> \varepsilon>0</math> there is a sequence of natural numbers {{math|1=''q''<sub>0</sub>, ''q''<sub>1</sub>, ''q''<sub>2</sub>,...}} such that {{math|1=''q<sub>n</sub>c<sub>k</sub>''}} is an [[algebraic integer]] in {{math|1=''K''}} for {{math|1=''k'' = 0, 1, 2,..., ''n''}}, and {{math|1=''n'' = 0, 1, 2,...}} and for which <math>q_n=O\left(n^{n\varepsilon}\right). </math>
where the left hand side represents the maximum of the absolute values of all the [[Conjugate element (field theory)|algebraic conjugates]] of ''c<sub>n</sub>'';
* For all &epsilon;&nbsp;&gt;&nbsp;0 there is a sequence of natural numbers ''q''<sub>0</sub>, ''q''<sub>1</sub>, ''q''<sub>2</sub>,&hellip; such that ''q<sub>n</sub>c<sub>k''</sub> is an [[algebraic integer]] in ''K'' for ''k''=0, 1, 2,&hellip;, ''n'', and ''n'' = 0, 1, 2,&hellip; and for which
:<math>q_{n}=O\left(n^{n\varepsilon}\right)</math>.


The second condition implies that ''f'' is an [[entire function]] of ''x''.
The second condition implies that {{math|1=''f''}} is an [[entire function]] of {{math|1=''x''}}.


==Uses==
==Uses==


''E''-functions were first studied by [[Carl Ludwig Siegel|Siegel]] in 1929<ref>C.L. Siegel, ''Über einige Anwendungen diophantischer Approximationen'', Abh. Preuss. Akad. Wiss. '''1''', 1929.</ref>. He found a method to show that the values taken by certain ''E''-functions were [[algebraically independent]], one of the only results of the early twentieth century which established the algebraic independence of classes of numbers rather than just linear independence<ref>Alan Baker, ''Transcendental Number Theory'', pp.109-112, Cambridge University Press, 1975.</ref>. Since then these functions have proved somewhat useful in [[number theory]] and in particular they have application in [[Transcendental numbers|transcendence]] proofs and [[differential equations]]<ref>Serge Lang, ''Introduction to Transcendental Numbers'', pp.76-77, Addison-Wesley Publishing Company, 1966.</ref>.
{{math|1=''E''}}-functions were first studied by [[Carl Ludwig Siegel|Siegel]] in 1929.<ref>C.L. Siegel, ''Über einige Anwendungen diophantischer Approximationen'', Abh. Preuss. Akad. Wiss. '''1''', 1929.</ref> He found a method to show that the values taken by certain {{math|1=''E''}}-functions were [[algebraically independent]]. This was a result which established the algebraic independence of classes of numbers rather than just linear independence.<ref>Alan Baker, ''Transcendental Number Theory'', pp.109-112, Cambridge University Press, 1975.</ref> Since then these functions have proved somewhat useful in [[number theory]] and in particular they have application in [[Transcendental numbers|transcendence]] proofs and [[differential equations]].<ref>[[Serge Lang]], ''Introduction to Transcendental Numbers'', pp.76-77, Addison-Wesley Publishing Company, 1966.</ref>


==The Siegel-Shidlovsky theorem==
==The Siegel–Shidlovsky theorem==


Perhaps the main result connected to ''E''-functions is the Siegel-Shidlovsky theorem (known also as the Shidlovsky and Shidlovskii theorem).
Perhaps the main result connected to {{math|1=''E''}}-functions is the Siegel–Shidlovsky theorem (also known as the Siegel and Shidlovsky theorem), named after [[Carl Ludwig Siegel]] and Andrei Borisovich Shidlovsky.


Suppose that we are given ''n'' ''E''-functions, ''E''<sub>1</sub>(''x''),&hellip;,''E''<sub>''n''</sub>(''x''), that satisfy a system of homogeneous linear differential equations
Suppose that we are given {{math|1=''n''}} {{math|1=''E''}}-functions, {{math|1=''E''<sub>1</sub>(''x''),...,''E''<sub>''n''</sub>(''x'')}}, that satisfy a system of homogeneous linear differential equations
:<math>y^\prime_i=\sum_{j=1}^n f_{ij}(x)y_j\quad(1\leq i\leq n)</math>
:<math>y^\prime_i=\sum_{j=1}^n f_{ij}(x)y_j\quad(1\leq i\leq n)</math>
where the ''f<sub>ij</sub>'' are rational functions of ''x'', and the coefficients of each ''E'' and ''f'' are elements of an algebraic number field ''K''. Then the theorem states that if ''E''<sub>1</sub>(''x''),&hellip;,''E''<sub>''n''</sub>(''x'') are algebraically independent over ''K''(''x''), then for any non-zero algebraic number &alpha; that is not a pole of any of the ''f<sub>ij</sub>'' the numbers ''E''<sub>1</sub>(&alpha;),&hellip;,''E''<sub>''n''</sub>(&alpha;) are algebraically independent.
where the {{math|1=''f<sub>ij</sub>''}} are rational functions of {{math|1=''x''}}, and the coefficients of each {{math|1=''E''}} and {{math|1=''f''}} are elements of an algebraic number field {{math|1=''K''}}. Then the theorem states that if {{math|1=''E''<sub>1</sub>(''x''),...,''E''<sub>''n''</sub>(''x'')}} are algebraically independent over {{math|1=''K''(''x'')}}, then for any non-zero algebraic number {{math|1=α}} that is not a pole of any of the {{math|1=''f<sub>ij</sub>''}} the numbers {{math|1=''E''<sub>1</sub>(α),...,''E''<sub>''n''</sub>(α)}} are algebraically independent.


==Examples==
==Examples==


# Any polynomial with algebraic coefficients is a simple example of an ''E''-function.
# Any polynomial with algebraic coefficients is a simple example of an {{math|1=''E''}}-function.
# The [[exponential function]] is an ''E''-function, in its case ''c<sub>n</sub>''=1 for all of the ''n''.
# The [[exponential function]] is an {{math|1=''E''}}-function, in its case {{math|1=''c<sub>n</sub>''&nbsp;=&nbsp;1}} for all of the {{math|1=''n''}}.
# If &lambda; is an algebraic number then the [[Bessel function]] ''J''<sub>&lambda;</sub> is an ''E''-function.
# If {{math|1=λ}} is an algebraic number then the [[Bessel function]] {{math|1=''J''<sub>λ</sub>}} is an {{math|1=''E''}}-function.
# The sum or product of two ''E''-functions is an ''E''-function. In particular ''E''-functions form a [[Ring (mathematics)|ring]].
# The sum or product of two {{math|1=''E''}}-functions is an {{math|1=''E''}}-function. In particular {{math|1=''E''}}-functions form a [[Ring (mathematics)|ring]].
# If ''a'' is an algebraic number and ''f''(''x'') is an ''E''-function then ''f''(''ax'') will be an ''E''-function.
# If {{math|1=''a''}} is an algebraic number and {{math|1=''f''(''x'')}} is an {{math|1=''E''}}-function then {{math|1=''f''(''ax'')}} will be an {{math|1=''E''}}-function.
# If ''f''(''x'') is an ''E''-function then the derivative and integral of ''f'' are also ''E''-functions.
# If {{math|1=''f''(''x'')}} is an {{math|1=''E''}}-function then the derivative and integral of {{math|1=''f''}} are also {{math|1=''E''}}-functions.


==References==
==References==
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* {{mathworld|title=E-Function|urlname=E-Function}}
* {{mathworld|title=E-Function|urlname=E-Function}}


[[Category:Number theory]]
[[Category:Transcendental numbers]]
[[Category:Algebraic number theory]]
[[Category:Analytic functions]]
[[Category:Analytic number theory]]

Latest revision as of 21:37, 16 September 2024

In mathematics, E-functions are a type of power series that satisfy particular arithmetic conditions on the coefficients. They are of interest in transcendental number theory, and are closely related to G-functions.

Definition

[edit]

A power series with coefficients in the field of algebraic numbers

is called an E-function[1] if it satisfies the following three conditions:

  • It is a solution of a non-zero linear differential equation with polynomial coefficients (this implies that all the coefficients cn belong to the same algebraic number field, K, which has finite degree over the rational numbers);
  • For all ,   
where the left hand side represents the maximum of the absolute values of all the algebraic conjugates of cn;
  • For all there is a sequence of natural numbers q0, q1, q2,... such that qnck is an algebraic integer in K for k = 0, 1, 2,..., n, and n = 0, 1, 2,... and for which

The second condition implies that f is an entire function of x.

Uses

[edit]

E-functions were first studied by Siegel in 1929.[2] He found a method to show that the values taken by certain E-functions were algebraically independent. This was a result which established the algebraic independence of classes of numbers rather than just linear independence.[3] Since then these functions have proved somewhat useful in number theory and in particular they have application in transcendence proofs and differential equations.[4]

The Siegel–Shidlovsky theorem

[edit]

Perhaps the main result connected to E-functions is the Siegel–Shidlovsky theorem (also known as the Siegel and Shidlovsky theorem), named after Carl Ludwig Siegel and Andrei Borisovich Shidlovsky.

Suppose that we are given n E-functions, E1(x),...,En(x), that satisfy a system of homogeneous linear differential equations

where the fij are rational functions of x, and the coefficients of each E and f are elements of an algebraic number field K. Then the theorem states that if E1(x),...,En(x) are algebraically independent over K(x), then for any non-zero algebraic number α that is not a pole of any of the fij the numbers E1(α),...,En(α) are algebraically independent.

Examples

[edit]
  1. Any polynomial with algebraic coefficients is a simple example of an E-function.
  2. The exponential function is an E-function, in its case cn = 1 for all of the n.
  3. If λ is an algebraic number then the Bessel function Jλ is an E-function.
  4. The sum or product of two E-functions is an E-function. In particular E-functions form a ring.
  5. If a is an algebraic number and f(x) is an E-function then f(ax) will be an E-function.
  6. If f(x) is an E-function then the derivative and integral of f are also E-functions.

References

[edit]
  1. ^ Carl Ludwig Siegel, Transcendental Numbers, p.33, Princeton University Press, 1949.
  2. ^ C.L. Siegel, Über einige Anwendungen diophantischer Approximationen, Abh. Preuss. Akad. Wiss. 1, 1929.
  3. ^ Alan Baker, Transcendental Number Theory, pp.109-112, Cambridge University Press, 1975.
  4. ^ Serge Lang, Introduction to Transcendental Numbers, pp.76-77, Addison-Wesley Publishing Company, 1966.
  • Weisstein, Eric W. "E-Function". MathWorld.