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In linear algebra, the permanent of a square matrix is a function of the matrix similar to the
determinant In mathematics, the determinant is a Scalar (mathematics), scalar-valued function (mathematics), function of the entries of a square matrix. The determinant of a matrix is commonly denoted , , or . Its value characterizes some properties of the ...
. The permanent, as well as the determinant, is a polynomial in the entries of the matrix. Both are special cases of a more general function of a matrix called the immanant.


Definition

The permanent of an matrix is defined as \operatorname(A)=\sum_\prod_^n a_. The sum here extends over all elements σ of the
symmetric group In abstract algebra, the symmetric group defined over any set is the group whose elements are all the bijections from the set to itself, and whose group operation is the composition of functions. In particular, the finite symmetric grou ...
''S''''n''; i.e. over all permutations of the numbers 1, 2, ..., ''n''. For example, \operatorname\begina&b \\ c&d\end=ad+bc, and \operatorname\begina&b&c \\ d&e&f \\ g&h&i \end=aei + bfg + cdh + ceg + bdi + afh. The definition of the permanent of ''A'' differs from that of the
determinant In mathematics, the determinant is a Scalar (mathematics), scalar-valued function (mathematics), function of the entries of a square matrix. The determinant of a matrix is commonly denoted , , or . Its value characterizes some properties of the ...
of ''A'' in that the signatures of the permutations are not taken into account. The permanent of a matrix A is denoted per ''A'', perm ''A'', or Per ''A'', sometimes with parentheses around the argument. Minc uses Per(''A'') for the permanent of rectangular matrices, and per(''A'') when ''A'' is a square matrix. Muir and Metzler use the notation \overset\quad \overset. The word, ''permanent'', originated with Cauchy in 1812 as “fonctions symétriques permanentes” for a related type of function, and was used by Muir and Metzler in the modern, more specific, sense.


Properties

If one views the permanent as a map that takes ''n'' vectors as arguments, then it is a multilinear map and it is symmetric (meaning that any order of the vectors results in the same permanent). Furthermore, given a square matrix A = \left(a_\right) of order ''n'': * perm(''A'') is invariant under arbitrary permutations of the rows and/or columns of ''A''. This property may be written symbolically as perm(''A'') = perm(''PAQ'') for any appropriately sized
permutation matrices In mathematics, particularly in Matrix (mathematics), matrix theory, a permutation matrix is a square binary matrix that has exactly one entry of 1 in each row and each column with all other entries 0. An permutation matrix can represent a permu ...
''P'' and ''Q'', * multiplying any single row or column of ''A'' by a scalar ''s'' changes perm(''A'') to ''s''⋅perm(''A''), * perm(''A'') is invariant under transposition, that is, perm(''A'') = perm(''A''T). * If A = \left(a_\right) and B=\left(b_\right) are square matrices of order ''n'' then, \operatorname\left(A + B\right) = \sum_ \operatorname \left(a_\right)_ \operatorname \left(b_\right)_, where ''s'' and ''t'' are subsets of the same size of and \bar, \bar are their respective complements in that set. * If A is a triangular matrix, i.e. a_=0, whenever i>j or, alternatively, whenever i, then its permanent (and determinant as well) equals the product of the diagonal entries: \operatorname\left(A\right) = a_ a_ \cdots a_ = \prod_^n a_.


Relation to determinants

Laplace's expansion by minors for computing the determinant along a row, column or diagonal extends to the permanent by ignoring all signs. For every i, \mathbb(B)=\sum_^n B_ M_, where B_ is the entry of the ''i''th row and the ''j''th column of ''B'', and M_ is the permanent of the submatrix obtained by removing the ''i''th row and the ''j''th column of ''B''. For example, expanding along the first column, \begin \operatorname \left ( \begin 1 & 1 & 1 & 1\\2 & 1 & 0 & 0\\3 & 0 & 1 & 0\\4 & 0 & 0 & 1 \end \right ) = & 1 \cdot \operatorname \left( \begin 1&0&0\\ 0&1&0\\ 0&0&1 \end\right) + 2\cdot \operatorname \left(\begin1&1&1\\0&1&0\\0&0&1\end\right) \\ & + \ 3\cdot \operatorname \left(\begin1&1&1\\1&0&0\\0&0&1\end\right) + 4 \cdot \operatorname \left(\begin1&1&1\\1&0&0\\0&1&0\end\right) \\ = & 1(1) + 2(1) + 3(1) + 4(1) = 10, \end while expanding along the last row gives, \begin \operatorname \left ( \begin 1 & 1 & 1 & 1\\2 & 1 & 0 & 0\\3 & 0 & 1 & 0\\4 & 0 & 0 & 1 \end \right ) = & 4 \cdot \operatorname \left(\begin1&1&1\\1&0&0\\0&1&0\end\right) + 0\cdot \operatorname \left(\begin1&1&1\\2&0&0\\3&1&0\end\right) \\ & + \ 0\cdot \operatorname \left(\begin1&1&1\\2&1&0\\3&0&0\end\right) + 1 \cdot \operatorname \left( \begin 1&1&1\\ 2&1&0\\ 3&0&1\end\right) \\ = & 4(1) + 0 + 0 + 1(6) = 10. \end On the other hand, the basic multiplicative property of determinants is not valid for permanents. A simple example shows that this is so. \begin 4 &= \operatorname \left ( \begin 1 & 1 \\ 1 & 1 \end \right )\operatorname \left ( \begin 1 & 1 \\ 1 & 1 \end \right ) \\ &\neq \operatorname\left ( \left ( \begin 1 & 1 \\ 1 & 1 \end \right ) \left ( \begin 1 & 1 \\ 1 & 1 \end \right ) \right ) = \operatorname \left ( \begin 2 & 2 \\ 2 & 2 \end \right )= 8. \end Unlike the determinant, the permanent has no easy geometrical interpretation; it is mainly used in
combinatorics Combinatorics is an area of mathematics primarily concerned with counting, both as a means and as an end to obtaining results, and certain properties of finite structures. It is closely related to many other areas of mathematics and has many ...
, in treating boson Green's functions in
quantum field theory In theoretical physics, quantum field theory (QFT) is a theoretical framework that combines Field theory (physics), field theory and the principle of relativity with ideas behind quantum mechanics. QFT is used in particle physics to construct phy ...
, and in determining state probabilities of boson sampling systems. However, it has two graph-theoretic interpretations: as the sum of weights of cycle covers of a directed graph, and as the sum of weights of perfect matchings in a bipartite graph.


Applications


Symmetric tensors

The permanent arises naturally in the study of the symmetric tensor power of Hilbert spaces. In particular, for a Hilbert space H, let \vee^k H denote the kth symmetric tensor power of H, which is the space of symmetric tensors. Note in particular that \vee^k H is spanned by the symmetric products of elements in H. For x_1,x_2,\dots,x_k \in H, we define the symmetric product of these elements by x_1 \vee x_2 \vee \cdots \vee x_k = (k!)^ \sum_ x_ \otimes x_ \otimes \cdots \otimes x_ If we consider \vee^k H (as a subspace of \otimes^kH, the ''k''th tensor power of H) and define the inner product on \vee^kH accordingly, we find that for x_j,y_j \in H \langle x_1 \vee x_2 \vee \cdots \vee x_k, y_1 \vee y_2 \vee \cdots \vee y_k \rangle = \operatorname\left langle x_i,y_j \rangle\right^k Applying the Cauchy–Schwarz inequality, we find that \operatorname \left langle x_i,x_j \rangle\right^k \geq 0, and that \left, \operatorname \left langle x_i,y_j \rangle\right^k \^2 \leq \operatorname \left langle x_i,x_j \rangle\right^k \cdot \operatorname \left langle y_i,y_j \rangle\right^k


Cycle covers

Any square matrix A = (a_)_^n can be viewed as the adjacency matrix of a weighted directed graph on vertex set V=\, with a_ representing the weight of the arc from vertex ''i'' to vertex ''j''. A cycle cover of a weighted directed graph is a collection of vertex-disjoint directed cycles in the digraph that covers all vertices in the graph. Thus, each vertex ''i'' in the digraph has a unique "successor" \sigma(i) in the cycle cover, and so \sigma represents a permutation on ''V''. Conversely, any permutation \sigma on ''V'' corresponds to a cycle cover with arcs from each vertex ''i'' to vertex \sigma(i). If the weight of a cycle-cover is defined to be the product of the weights of the arcs in each cycle, then \operatorname(\sigma) = \prod_^n a_, implying that \operatorname(A)=\sum_\sigma \operatorname(\sigma). Thus the permanent of ''A'' is equal to the sum of the weights of all cycle-covers of the digraph.


Perfect matchings

A square matrix A = (a_) can also be viewed as the adjacency matrix of a bipartite graph which has vertices x_1, x_2, \dots, x_n on one side and y_1, y_2, \dots, y_n on the other side, with a_ representing the weight of the edge from vertex x_i to vertex y_j. If the weight of a perfect matching \sigma that matches x_i to y_ is defined to be the product of the weights of the edges in the matching, then \operatorname(\sigma) = \prod_^n a_. Thus the permanent of ''A'' is equal to the sum of the weights of all perfect matchings of the graph.


Permanents of (0, 1) matrices


Enumeration

The answers to many counting questions can be computed as permanents of matrices that only have 0 and 1 as entries. Let Ω(''n'',''k'') be the class of all (0, 1)-matrices of order ''n'' with each row and column sum equal to ''k''. Every matrix ''A'' in this class has perm(''A'') > 0. The incidence matrices of projective planes are in the class Ω(''n''2 + ''n'' + 1, ''n'' + 1) for ''n'' an integer > 1. The permanents corresponding to the smallest projective planes have been calculated. For ''n'' = 2, 3, and 4 the values are 24, 3852 and 18,534,400 respectively. Let ''Z'' be the incidence matrix of the projective plane with ''n'' = 2, the Fano plane. Remarkably, perm(''Z'') = 24 = , det (''Z''), , the absolute value of the determinant of ''Z''. This is a consequence of ''Z'' being a circulant matrix and the theorem: :If ''A'' is a circulant matrix in the class Ω(''n'',''k'') then if ''k'' > 3, perm(''A'') > , det (''A''), and if ''k'' = 3, perm(''A'') = , det (''A''), . Furthermore, when ''k'' = 3, by permuting rows and columns, ''A'' can be put into the form of a direct sum of ''e'' copies of the matrix ''Z'' and consequently, ''n'' = 7''e'' and perm(''A'') = 24e. Permanents can also be used to calculate the number of permutations with restricted (prohibited) positions. For the standard ''n''-set , let A = (a_) be the (0, 1)-matrix where ''a''''ij'' = 1 if ''i'' → ''j'' is allowed in a permutation and ''a''''ij'' = 0 otherwise. Then perm(''A'') is equal to the number of permutations of the ''n''-set that satisfy all the restrictions. Two well known special cases of this are the solution of the derangement problem and the ménage problem: the number of permutations of an ''n''-set with no fixed points (derangements) is given by \operatorname(J - I) = \operatorname\left (\begin 0 & 1 & 1 & \dots & 1 \\ 1 & 0 & 1 & \dots & 1 \\ 1 & 1 & 0 & \dots & 1 \\ \vdots & \vdots & \vdots & \ddots & \vdots \\ 1 & 1 & 1 & \dots & 0 \end \right) = n! \sum_^n \frac, where ''J'' is the ''n''×''n'' all 1's matrix and ''I'' is the identity matrix, and the ménage numbers are given by \begin \operatorname(J - I - I') & = \operatorname\left (\begin 0 & 0 & 1 & \dots & 1 \\ 1 & 0 & 0 & \dots & 1 \\ 1 & 1 & 0 & \dots & 1 \\ \vdots & \vdots & \vdots & \ddots & \vdots \\ 0 & 1 & 1 & \dots & 0 \end \right) \\ & = \sum_^n (-1)^k \frac (n-k)!, \end where ''I is the (0, 1)-matrix with nonzero entries in positions (''i'', ''i'' + 1) and (''n'', 1). Permanent of ''n''×''n'' all 1's matrix is a number of possible arrangements of ''n'' mutually non-attacking rooks in the positions of the board of size ''n''×''n''.


Bounds

The Bregman–Minc inequality, conjectured by H. Minc in 1963 and proved by L. M. Brégman in 1973, gives an upper bound for the permanent of an ''n'' × ''n'' (0, 1)-matrix. If ''A'' has ''r''''i'' ones in row ''i'' for each 1 ≤ ''i'' ≤ ''n'', the inequality states that \operatorname A \leq \prod_^n (r_i)!^.


Van der Waerden's conjecture

In 1926, Van der Waerden conjectured that the minimum permanent among all doubly stochastic matrices is ''n''!/''n''''n'', achieved by the matrix for which all entries are equal to 1/''n''. Proofs of this conjecture were published in 1980 by B. Gyires and in 1981 by G. P. Egorychev and D. I. Falikman; Egorychev's proof is an application of the Alexandrov–Fenchel inequality.Brualdi (2006) p.487 For this work, Egorychev and Falikman won the Fulkerson Prize in 1982.


Computation

The naïve approach, using the definition, of computing permanents is computationally infeasible even for relatively small matrices. One of the fastest known algorithms is due to H. J. Ryser. Ryser's method is based on an inclusion–exclusion formula that can be given as follows: Let A_k be obtained from ''A'' by deleting ''k'' columns, let P(A_k) be the product of the row-sums of A_k, and let \Sigma_k be the sum of the values of P(A_k) over all possible A_k. Then \operatorname(A)=\sum_^ (-1)^ \Sigma_k. It may be rewritten in terms of the matrix entries as follows: \operatorname (A) = (-1)^n \sum_ (-1)^ \prod_^n \sum_ a_. The permanent is believed to be more difficult to compute than the determinant. While the determinant can be computed in polynomial time by Gaussian elimination, Gaussian elimination cannot be used to compute the permanent. Moreover, computing the permanent of a (0,1)-matrix is #P-complete. Thus, if the permanent can be computed in polynomial time by any method, then FP =  #P, which is an even stronger statement than P = NP. When the entries of ''A'' are nonnegative, however, the permanent can be computed approximately in probabilistic polynomial time, up to an error of \varepsilon M, where M is the value of the permanent and \varepsilon > 0 is arbitrary. The permanent of a certain set of positive semidefinite matrices is NP-hard to approximate within any subexponential factor. If further conditions on the spectrum are imposed, the permanent can be approximated in probabilistic polynomial time: the best achievable error of this approximation is \varepsilon\sqrt (M is again the value of the permanent). The hardness in these instances is closely linked with difficulty of simulating boson sampling experiments.


MacMahon's master theorem

Another way to view permanents is via multivariate generating functions. Let A = (a_) be a square matrix of order ''n''. Consider the multivariate generating function: \begin F(x_1,x_2,\dots,x_n) &= \prod_^n \left ( \sum_^n a_ x_j \right ) \\ &= \left( \sum_^n a_ x_j \right ) \left ( \sum_^n a_ x_j \right ) \cdots \left ( \sum_^n a_ x_j \right). \end The coefficient of x_1 x_2 \dots x_n in F(x_1,x_2,\dots,x_n) is perm(''A''). As a generalization, for any sequence of ''n'' non-negative integers, s_1,s_2,\dots,s_n define: \operatorname^(A) as the coefficient of x_1^ x_2^ \cdots x_n^ in\left ( \sum_^n a_ x_j \right )^ \left ( \sum_^n a_ x_j \right )^ \cdots \left ( \sum_^n a_ x_j \right )^. MacMahon's master theorem relating permanents and determinants is: \operatorname^(A) = \textx_1^ x_2^ \cdots x_n^ \text \frac, where ''I'' is the order ''n'' identity matrix and ''X'' is the diagonal matrix with diagonal _1,x_2,\dots,x_n


Rectangular matrices

The permanent function can be generalized to apply to non-square matrices. Indeed, several authors make this the definition of a permanent and consider the restriction to square matrices a special case. Specifically, for an ''m'' × ''n'' matrix A = (a_) with ''m'' ≤ ''n'', define \operatorname (A) = \sum_ a_ a_ \ldots a_ where P(''n'',''m'') is the set of all ''m''-permutations of the ''n''-set . Ryser's computational result for permanents also generalizes. If ''A'' is an ''m'' × ''n'' matrix with ''m'' ≤ ''n'', let A_k be obtained from ''A'' by deleting ''k'' columns, let P(A_k) be the product of the row-sums of A_k, and let \sigma_k be the sum of the values of P(A_k) over all possible A_k. Then \operatorname(A)=\sum_^ (-1)^\binom\sigma_.


Systems of distinct representatives

The generalization of the definition of a permanent to non-square matrices allows the concept to be used in a more natural way in some applications. For instance: Let ''S''1, ''S''2, ..., ''S''''m'' be subsets (not necessarily distinct) of an ''n''-set with ''m'' ≤ ''n''. The incidence matrix of this collection of subsets is an ''m'' × ''n'' (0,1)-matrix ''A''. The number of systems of distinct representatives (SDR's) of this collection is perm(''A'').


See also

* Computing the permanent * Bapat–Beg theorem, an application of permanents in order statistics * Slater determinant, an application of permanents in
quantum mechanics Quantum mechanics is the fundamental physical Scientific theory, theory that describes the behavior of matter and of light; its unusual characteristics typically occur at and below the scale of atoms. Reprinted, Addison-Wesley, 1989, It is ...
* Hafnian


Notes


References

* * * * * *


Further reading

* Contains a proof of the Van der Waerden conjecture. *


External links

* *{{PlanetMath , urlname=VanDerWaerdensPermanentConjecture , title=Van der Waerden's permanent conjecture Algebra Linear algebra Matrix theory Permutations