Entire function
In complex analysis, an entire function, also called an integral function, is a complexvalued function that is holomorphic over the whole complex plane. Typical examples of entire functions are polynomials and the exponential function, and any sums, products and compositions of these, such as the trigonometric functions sine and cosine and their hyperbolic counterparts sinh and cosh, as well as derivatives and integrals of entire functions such as the error function. If an entire function f(z) has a root at w, then f(z)/(z−w) is an entire function. On the other hand, neither the natural logarithm nor the square root is an entire function, nor can they be continued analytically to an entire function.
A transcendental entire function is an entire function that is not a polynomial.
Properties
Every entire function f(z) can be represented as a power series
that converges everywhere in the complex plane, hence uniformly on compact sets. The radius of convergence is infinite, which implies that
or
Any power series satisfying this criterion will represent an entire function.
If (and only if) the coefficients of the power series are all real then the function (obviously) takes real values for real arguments, and the value of the function at the complex conjugate of z will be the complex conjugate of the value at z. Such functions are sometimes called selfconjugate (the conjugate function, , being given by ^{}
If the real part of an entire function is known in a neighborhood of a point then both the real and imaginary parts are known for the whole complex plane, up to an imaginary constant. For instance, if the real part is known in a neighborhood of zero, then we can find the coefficients for n > 0 from the following derivatives with respect to a real variable r:
(Likewise, if the imaginary part is known in a neighborhood then the function is determined up to a real constant.) In fact, if the real part is known just on an arc of a circle, then the function is determined up to an imaginary constant. (For instance, if it the real part is known on part of the unit circle, then it is known on the whole unit circle by analytic extension, and then the coefficients of the infinite series are determined from the coefficients of the Fourier series for the real part on the unit circle.) Note however that an entire function is not determined by its real part on all curves. In particular, if the real part is given on any curve in the complex plane where the real part of some other entire function is zero, then any multiple of that function can be added to the function we are trying to determine. For example, if the curve where the real part is known is the real line, then we can add i times any selfconjugate function. If the curve forms a loop, then the only functions whose real part is zero on the curve are those that are everywhere equal to some imaginary number.
The Weierstrass factorization theorem asserts that any entire function can be represented by a product involving its zeroes (or "roots").
The entire functions on the complex plane form an integral domain (in fact a Prüfer domain). They also form a commutative unital associative algebra over the complex numbers.
Liouville's theorem states that any bounded entire function must be constant. Liouville's theorem may be used to elegantly prove the fundamental theorem of algebra.
As a consequence of Liouville's theorem, any function that is entire on the whole Riemann sphere (complex plane and the point at infinity) is constant. Thus any nonconstant entire function must have a singularity at the complex point at infinity, either a pole for a polynomial or an essential singularity for a transcendental entire function. Specifically, by the Casorati–Weierstrass theorem, for any transcendental entire function f and any complex w there is a sequence (z_{m})_{m∈N} with and .
Picard's little theorem is a much stronger result: any nonconstant entire function takes on every complex number as value, possibly with a single exception. When an exception exists, it is called a lacunary value of the function. The possibility of a lacunary value is illustrated by the exponential function, which never takes on the value 0. One can take a logarithm of an entire function that never hits 0, and this will also be an entire function (according to the Weierstrass factorization theorem). The logarithm hits every complex number except possibly one number, which implies that the first function will hit any value other than 0 an infinite number of times. Similarly, a nonconstant, entire function that does not hit a particular value will hit every other value an infinite number of times.
Liouville's theorem is a special case of the following statement:
Theorem: Assume M, R are positive constants and that n is a nonnegative integer. An entire function f satisfying the inequality for all z with , is necessarily a polynomial, of degree at most n.^{} Similarly, an entire function f satisfying the inequality for all z with , is necessarily a polynomial, of degree at least n.
Growth
Entire functions may grow as fast as any increasing function: for any increasing function g : [0,+∞) → [0,+∞) there exists an entire function f(z) such that f(x) > g( x ) for all real x. Such a function f may be easily found of the form:
for a constant c and a strictly increasing sequence of positive integers n_{k}. Any such sequence defines an entire function f(z), and if the powers are chosen appropriately we may satisfy the inequality f(x) > g( x ) for all real x. (For instance, it certainly holds if one chooses c:=g(2) and, for any integer k ≥ 1, although this gives powers that may be about twice as high as needed.)
Order and type
The order (at infinity) of an entire function f(z) is defined using the limit superior as:
where B_{r} is the disk of radius r and denotes the supremum norm of f(z) on B_{r}. The order is a nonnegative real number or infinity (except if f(z)=0 for all z). The order of f(z) is the infimum of all m such that f(z) = O(exp(z^{m})) as z → ∞. (A function like shows that this does not mean f(z) = O(exp(z^{m})) if f(z) is of order m.)
If 0<ρ<∞, one can also define the type:
If the order is 1 and the type is σ, the function is said to be "of exponential type σ". If it is of order less than 1 it is said to be of exponential type 0.
If
then the order and type can be found by the formulas
If we denote the n^{th} derivative of a function f() by f^{(n)}(), then we may restate these formulas in terms of the derivatives at any arbitrary point z_{0}:
The type may be infinite, as in the case of the reciprocal gamma function, or zero (see example below under #Order 1).
Examples
Here are some examples of functions of various orders:
Order ρ
For arbitrary positive numbers ρ and σ one can construct an example of an entire function of order ρ and type σ using:
Order 0
 Polynomials (other than 0)
Order 1/4
Order 1/3
Order 1/2
 with a ≠ 0 (for which the type is given by σ = a)
Order 1
 exp(az) with a ≠ 0 (σ = a)
 sin(z)
 cosh(z)
 the Bessel function J_{0}(z)
 the reciprocal gamma function 1/Γ(z) (σ is infinite)
Order 3/2
 Airy function Ai(z)
Order 2
 exp(−az^{2}) with a ≠ 0 (σ = a)
Order infinity
 exp(−e^{z})
Genus of an entire function
Entire functions of finite order have Hadamard's canonical representation:
where z_{k} are the nonzero roots of f, P a polynomial (whose degree we shall call q), and p is the smallest nonnegative integer such that the series
converges. The nonnegative integer g = max{p, q} is called the genus of the entire function f.
If the order ρ is not an integer, then g = [ρ] is the integer part of ρ. If the order is a positive integer, then there are two possibilities: g = ρ1 or g = ρ.
For example, sin, cos and exp are entire functions of genus 1.
Other examples
According to J. E. Littlewood, the Weierstrass sigma function is a 'typical' entire function. This statement can be made precise in the theory of random entire functions: the asymptotic behaviour of almost all entire functions is similar to that of the sigma function. Other examples include the Fresnel integrals, the Jacobi theta function, and the reciprocal Gamma function. The exponential function and the error function are special cases of the MittagLeffler function. According to the fundamental theorem of Paley and Wiener, Fourier transforms of functions with bounded support are entire functions or order 1 and finite type.
Other examples are solutions of linear differential equations with polynomial coefficients. If the coefficient at the highest derivative is constant, then all solutions of such equations are entire functions. For example, the exponential function, sine, cosine, Airy functions and Parabolic cylinder functions arise in this way. The class of entire functions is closed with respect to compositions. This makes it possible to study dynamics of entire functions.
An entire function of the square root of a complex number is entire if the original function is even, for example .
If a sequence of polynomials all of whose roots are real converges in a neighborhood of the origin to a limit which is not identically equal to zero, then this limit is an entire function. Such entire functions form the Laguerre–Pólya class, which can also be characterized in terms of the Hadamard product, namely, f belongs to this class if and only if in the Hadamard representation all z_{n} are real, p ≤ 1, and P(z) = a + bz + cz^{2}, where b and c are real, and c ≤ 0. For example, the sequence of polynomials converges, as n increases, to exp(−(z−d)^{2}). The polynomials have all real roots, and converge to cos(z). Interestingly, the polynomials also converge to cos(z), showing the buildup of the Hadamard product for cosine.
See also
 Jensen's formula
 Carlson's theorem
 Exponential type
 Paley–Wiener theorem
Notes
References
 Ralph P. Boas (1954). Entire Functions. Academic Press. OCLC 847696.
 B. Ya. Levin (1980). Distribution of zeros of entire functions. Amer. Math. Soc.
 B. Ya. Levin (1996). Lectures on entire functions. Amer. Math. Soc.
