Complex analysis

Complex analysis, traditionally known as the theory of functions of a complex variable, is the branch of mathematical analysis that investigates functions of complex numbers. It is useful in many branches of mathematics, including algebraic geometry, number theory, analytic combinatorics, applied mathematics; as well as in physics, including hydrodynamics and thermodynamics and also in engineering fields such as nuclear, aerospace, mechanical and electrical engineering.

Complex analysis is particularly concerned with analytic functions of complex variables (or, more generally, meromorphic functions). Because the separate real and imaginary parts of any analytic function must satisfy Laplace's equation, complex analysis is widely applicable to two-dimensional problems in physics.

History

Complex analysis is one of the classical branches in mathematics, with roots in the 19th century and just prior. Important mathematicians associated with complex analysis include Euler, Gauss, Riemann, Cauchy, Weierstrass, and many more in the 20th century. Complex analysis, in particular the theory of conformal mappings, has many physical applications and is also used throughout analytic number theory. In modern times, it has become very popular through a new boost from complex dynamics and the pictures of fractals produced by iterating holomorphic functions. Another important application of complex analysis is in string theory which studies conformal invariants in quantum field theory.

Complex functions

A complex function is one in which the independent variable and the dependent variable are both complex numbers. More precisely, a complex function is a function whose domain and range are subsets of the complex plane.

For any complex function, both the independent variable and the dependent variable may be separated into real and imaginary parts:

z

=

x + iy

and

w

=

f (z)

=

u (x, y) + iv (x, y)

where

x, y \in ℝ

and

u (x, y), v (x, y)

are real-valued functions.

In other words, the components of the function $f (z)$ ,

u

=

u (x, y)

and

v

=

v (x, y)

can be interpreted as real-valued functions of the two real variables, $x$ and $y$ .

The basic concepts of complex analysis are often introduced by extending the elementary real functions (e.g., exponential functions, logarithmic functions, and trigonometric functions) into the complex domain.

Holomorphic functions

Holomorphic functions are complex functions, defined on an open subset of the complex plane, that are differentiable. In the context of complex analysis, the derivative of $f$ at $z_{0}$ is defined to be

$f'(z_{0})=\lim _{z\to z_{0}}{\frac {f(z)-f(z_{0})}{z-z_{0}}},z\in \mathbb {C}$ .

Although superficially similar in form to the derivative of a real function, the behavior of complex derivatives and differentiable functions is significantly different. In particular, for this limit to exist, the value of the difference quotient must approach the same complex number, regardless of the manner in which we approach $z_{0}$ in the complex plane. Consequently, complex differentiability has much stronger consequences than usual (real) differentiability. For instance, holomorphic functions are infinitely differentiable, whereas most real differentiable functions are not. For this reason, holomorphic functions are also referred to as analytic functions. Most elementary functions, including the exponential function, the trigonometric functions, and all polynomial functions, extended appropriately to complex arguments as functions $\mathbb {C} \to \mathbb {C}$ , are holomorphic over the entire complex plane, making them entire functions, while rational functions $p/q$ , where p and q are polynomials, are holomorphic on domains that exclude points where q is zero. Such functions that are holomorphic everywhere except a set of isolated points are known as meromorphic functions. On the other hand, the functions $z\mapsto \Re (z)$ , $z\mapsto |z|$ , and $z\mapsto {\bar {z}}$ are not holomorphic anywhere on the complex plane, as can be shown by their failure to satisfy the Cauchy-Riemann conditions (see below).

An important property the characterizes holomorphic functions is the relationship between the partial derivatives of their real and imaginary components, known as the Cauchy-Riemann conditions. If $f:\mathbb {C} \to \mathbb {C}$ , defined by $f(z)=f(x+iy)=u(x,y)+iv(x,y)$ , where $x,y,u(x,y),v(x,y)\in \mathbb {R}$ , is holomorphic on a region $\Omega$ , then $(\partial f/\partial {\bar {z}})(z_{0})=0$ must hold for all $z_{0}\in \Omega$ . Here, the differential operator $\partial /\partial {\bar {z}}$ is defined as $(1/2)(\partial /\partial x+i\partial /\partial y)$ . In terms of the real and imaginary parts of the function, u and v, this is equivalent to the pair of equations $u_{x}=v_{y}$ and $u_{y}=-v_{x}$ , where the subscripts indicate partial differentiation. However, it is important to note that functions satisfying the Cauchy-Riemann conditions are not necessarily holomorphic, unless additional continuity conditions are met (see Looman-Menchoff Theorem for a discussion).

Holomorphic functions exhibit some remarkable features. For instance, Picard's theorem asserts that the range of an entire function can only take three possible forms: $\mathbb {C}$ , $\mathbb {C} \setminus \{z_{0}\}$ , or $\{z_{0}\}$ for some $z_{0}\in \mathbb {C}$ . In other words, if two distinct complex numbers $z$ and $w$ are not in the range of entire function $f$ , then $f$ is a constant function. Moreover, given a holomorphic function $f$ defined on a open set $U$ , the analytical extension of $f$ to a larger open set $V\supset U$ is unique. Thus, the value of a holomorphic function over a relatively small region in fact determines the value of the function everywhere to which it can be extended.

See also: analytic function, coherent sheaf and vector bundles.

Major results

One of the central tools in complex analysis is the line integral. The line integral around a closed path of a function that is holomorphic everywhere inside the area bounded by the closed path is always zero, which is what the Cauchy integral theorem states. The values of such a holomorphic function inside a disk can be computed by a path integral on the disk's boundary, as shown in (Cauchy's integral formula). Path integrals in the complex plane are often used to determine complicated real integrals, and here the theory of residues among others is applicable (see methods of contour integration). A "pole" (or isolated singularity) of a function is a point where the function's value becomes unbounded, or "blows up". If a function has such a pole, then one can compute the function's residue there, which can be used to compute path integrals involving the function; this is the content of the powerful residue theorem. The remarkable behavior of holomorphic functions near essential singularities is described by Picard's Theorem. Functions that have only poles but no essential singularities are called meromorphic. Laurent series are the complex-valued equivalent to Taylor series, but can be used to study the behavior of functions near singularities through infinite sums of more well understood functions, such as polynomials.

A bounded function that is holomorphic in the entire complex plane must be constant; this is Liouville's theorem. It can be used to provide a natural and short proof for the fundamental theorem of algebra which states that the field of complex numbers is algebraically closed.

If a function is holomorphic throughout a connected domain then its values are fully determined by its values on any smaller subdomain. The function on the larger domain is said to be analytically continued from its values on the smaller domain. This allows the extension of the definition of functions, such as the Riemann zeta function, which are initially defined in terms of infinite sums that converge only on limited domains to almost the entire complex plane. Sometimes, as in the case of the natural logarithm, it is impossible to analytically continue a holomorphic function to a non-simply connected domain in the complex plane but it is possible to extend it to a holomorphic function on a closely related surface known as a Riemann surface.

All this refers to complex analysis in one variable. There is also a very rich theory of complex analysis in more than one complex dimension in which the analytic properties such as power series expansion carry over whereas most of the geometric properties of holomorphic functions in one complex dimension (such as conformality) do not carry over. The Riemann mapping theorem about the conformal relationship of certain domains in the complex plane, which may be the most important result in the one-dimensional theory, fails dramatically in higher dimensions.

References

Ahlfors, L., Complex Analysis, 3 ed. (McGraw-Hill, 1979).
Stephen D. Fisher, Complex Variables, 2 ed. (Dover, 1999).
Carathéodory, C., Theory of Functions of a Complex Variable (Chelsea, New York). [2 volumes.]
Henrici, P., Applied and Computational Complex Analysis (Wiley). [Three volumes: 1974, 1977, 1986.]
Kreyszig, E., Advanced Engineering Mathematics, 10 ed., Ch.13-18 (Wiley, 2011).
Markushevich, A.I.,Theory of Functions of a Complex Variable (Prentice-Hall, 1965). [Three volumes.]
Marsden & Hoffman, Basic Complex Analysis. 3 ed. (Freeman, 1999).
Needham, T., Visual Complex Analysis (Oxford, 1997).
Rudin, W., Real and Complex Analysis, 3 ed. (McGraw-Hill, 1986).
Scheidemann, V., Introduction to complex analysis in several variables (Birkhauser, 2005)
Shaw, W.T., Complex Analysis with Mathematica (Cambridge, 2006).
Spiegel, Murray R. Theory and Problems of Complex Variables - with an introduction to Conformal Mapping and its applications (McGraw-Hill, 1964).
Stein & Shakarchi, Complex Analysis (Princeton, 2003).

External links