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Free convolution is the
free probability Free probability is a mathematical theory that studies non-commutative random variables. The "freeness" or free independence property is the analogue of the classical notion of independence, and it is connected with free products. This theory was in ...
analog of the classical notion of
convolution In mathematics (in particular, functional analysis), convolution is a operation (mathematics), mathematical operation on two function (mathematics), functions ( and ) that produces a third function (f*g) that expresses how the shape of one is ...
of probability measures. Due to the non-commutative nature of free probability theory, one has to talk separately about additive and multiplicative free convolution, which arise from addition and multiplication of free random variables (see below; in the classical case, what would be the analog of free multiplicative convolution can be reduced to additive convolution by passing to logarithms of random variables). These operations have some interpretations in terms of empirical spectral measures of
random matrices In probability theory and mathematical physics, a random matrix is a matrix-valued random variable—that is, a matrix in which some or all elements are random variables. Many important properties of physical systems can be represented mathemat ...
. The notion of free convolution was introduced by Voiculescu.


Free additive convolution

Let \mu and \nu be two probability measures on the real line, and assume that X is a random variable in a non commutative probability space with law \mu and Y is a random variable in the same non commutative probability space with law \nu. Assume finally that X and Y are freely independent. Then the free additive convolution \mu\boxplus\nu is the law of X+Y.
Random matrices In probability theory and mathematical physics, a random matrix is a matrix-valued random variable—that is, a matrix in which some or all elements are random variables. Many important properties of physical systems can be represented mathemat ...
interpretation: if A and B are some independent n by n Hermitian (resp. real symmetric) random matrices such that at least one of them is invariant, in law, under conjugation by any unitary (resp. orthogonal) matrix and such that the empirical spectral measures of A and B tend respectively to \mu and \nu as n tends to infinity, then the empirical spectral measure of A+B tends to \mu\boxplus\nu. In many cases, it is possible to compute the probability measure \mu\boxplus\nu explicitly by using complex-analytic techniques and the R-transform of the measures \mu and \nu.


Rectangular free additive convolution

The rectangular free additive convolution (with ratio c) \boxplus_c has also been defined in the non commutative probability framework by Benaych-Georges and admits the following
random matrices In probability theory and mathematical physics, a random matrix is a matrix-valued random variable—that is, a matrix in which some or all elements are random variables. Many important properties of physical systems can be represented mathemat ...
interpretation. For c\in ,1/math>, for A and B are some independent n by p complex (resp. real) random matrices such that at least one of them is invariant, in law, under multiplication on the left and on the right by any unitary (resp. orthogonal) matrix and such that the empirical singular values distribution of A and B tend respectively to \mu and \nu as n and p tend to infinity in such a way that n/p tends to c, then the empirical singular values distribution of A+B tends to \mu\boxplus_c\nu. In many cases, it is possible to compute the probability measure \mu\boxplus_c\nu explicitly by using complex-analytic techniques and the rectangular R-transform with ratio c of the measures \mu and \nu.


Free multiplicative convolution

Let \mu and \nu be two probability measures on the interval [0,+\infty), and assume that X is a random variable in a non commutative probability space with law \mu and Y is a random variable in the same non commutative probability space with law \nu. Assume finally that X and Y are freely independent. Then the free multiplicative convolution \mu\boxtimes\nu is the law of X^YX^ (or, equivalently, the law of Y^XY^.
Random matrices In probability theory and mathematical physics, a random matrix is a matrix-valued random variable—that is, a matrix in which some or all elements are random variables. Many important properties of physical systems can be represented mathemat ...
interpretation: if A and B are some independent n by n non negative Hermitian (resp. real symmetric) random matrices such that at least one of them is invariant, in law, under conjugation by any unitary (resp. orthogonal) matrix and such that the empirical spectral measures of A and B tend respectively to \mu and \nu as n tends to infinity, then the empirical spectral measure of AB tends to \mu\boxtimes\nu.Anderson, G.W.; Guionnet, A.; Zeitouni, O. (2010). An introduction to random matrices. Cambridge: Cambridge University Press. . A similar definition can be made in the case of laws \mu,\nu supported on the unit circle \, with an orthogonal or unitary
random matrices In probability theory and mathematical physics, a random matrix is a matrix-valued random variable—that is, a matrix in which some or all elements are random variables. Many important properties of physical systems can be represented mathemat ...
interpretation. Explicit computations of multiplicative free convolution can be carried out using complex-analytic techniques and the S-transform.


Applications of free convolution

* Free convolution can be used to give a proof of the free central limit theorem. * Free convolution can be used to compute the laws and spectra of sums or products of random variables which are free. Such examples include: random walk operators on free groups (Kesten measures); and asymptotic distribution of eigenvalues of sums or products of independent random matrix, random matrices. Through its applications to random matrices, free convolution has some strong connections with other works on G-estimation of Girko. The applications in
wireless communication Wireless communication (or just wireless, when the context allows) is the transfer of information between two or more points without the use of an electrical conductor, optical fiber or other continuous guided medium for the transfer. The most ...
s,
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and
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have provided a useful framework when the number of observations is of the same order as the dimensions of the system.


See also

*
Convolution In mathematics (in particular, functional analysis), convolution is a operation (mathematics), mathematical operation on two function (mathematics), functions ( and ) that produces a third function (f*g) that expresses how the shape of one is ...
*
Free probability Free probability is a mathematical theory that studies non-commutative random variables. The "freeness" or free independence property is the analogue of the classical notion of independence, and it is connected with free products. This theory was in ...
*
Random matrix In probability theory and mathematical physics, a random matrix is a matrix-valued random variable—that is, a matrix in which some or all elements are random variables. Many important properties of physical systems can be represented mathemat ...


References

{{Reflist * "Free Deconvolution for Signal Processing Applications", O. Ryan and M. Debbah, ISIT 2007, pp. 1846–1850 *James A. Mingo, Roland Speicher: /www.springer.com/us/book/9781493969418 Free Probability and Random Matrices Fields Institute Monographs, Vol. 35, Springer, New York, 2017. *D.-V. Voiculescu, N. Stammeier, M. Weber (eds.)
Free Probability and Operator Algebras
Münster Lectures in Mathematics, EMS, 2016


External links


http://www.cmapx.polytechnique.fr/~benaychhttp://folk.uio.no/oyvindry


of Roland Speicher on free probability. Signal processing Combinatorics Functional analysis Free probability theory Free algebraic structures