Pfaffian

Pfaffian

In mathematics, the determinant of a skew-symmetric matrix can always be written as the square of a polynomial in the matrix entries. This polynomial is called the Pfaffian of the matrix. The Pfaffian is nonvanishing only for 2"n" × 2"n" skew-symmetric matrices, in which case it is a polynomial of degree "n".

Examples

:mbox{Pf}egin{bmatrix} 0 & a \ -a & 0 end{bmatrix}=a.

:mbox{Pf}egin{bmatrix} 0 & a & b & c \ -a & 0 & d & e \ -b & -d & 0& f \-c & -e & -f & 0 end{bmatrix}=af-be+dc.

:mbox{Pf}egin{bmatrix}egin{matrix}0 & lambda_1\ -lambda_1 & 0end{matrix} & 0 & cdots & 0 \0 & egin{matrix}0 & lambda_2\ -lambda_2 & 0end{matrix} & & 0 \vdots & & ddots & vdots \0 & 0 & cdots & egin{matrix}0 & lambda_n\ -lambda_n & 0end{matrix}end{bmatrix} = lambda_1lambda_2cdotslambda_n.

Formal definition

Let "A" = {"a""i,j"} be a 2"n"×2"n" skew-symmetric matrix. The Pfaffian of "A" is defined by the equation

:mathrm{Pf}(A) = frac{1}{2^n n!}sum_{sigmain S_{2nmathrm{sgn}(sigma)prod_{i=1}^{n}a_{sigma(2i-1),sigma(2i)}

where "S"2"n" is the symmetric group and sgn(σ) is the signature of σ.

One can make use of the skew-symmetry of "A" to avoid summing over all possible permutations. Let Π be the set of all partitions of {1, 2, …, 2"n"} into pairs without regard to order. There are (2"n" − 1)!! such partitions. An element α ∈ Π, can be written as

:alpha={(i_1,j_1),(i_2,j_2),cdots,(i_n,j_n)}

with "i""k" < "j""k" and i_1 < i_2 < cdots < i_n. Let

:pi=egin{bmatrix} 1 & 2 & 3 & 4 & cdots & 2n \ i_1 & j_1 & i_2 & j_2 & cdots & j_{n} end{bmatrix}

be a corresponding permutation. This depends only on the partition α and not on the particular choice of π. Given a partition α as above define

: A_alpha =operatorname{sgn}(pi)a_{i_1,j_1}a_{i_2,j_2}cdots a_{i_n,j_n}.

The Pfaffian of "A" is then given by

:operatorname{Pf}(A)=sum_{alphainPi} A_alpha.

The Pfaffian of a "n"&times;"n" skew-symmetric matrix for "n" odd is defined to be zero, as the determinant of an odd skew-symmetric matrix is zero, since for a skew-symmetric matrix, det,A = det,A^T = det,-A = (-1)^n det,A, and for "n" odd, this implies det,A = 0.

Recursive definition

By convention, the Pfaffian of the 0×0 matrix is equal to one. The Pfaffian of a skew-symmetric 2"n"×2"n" matrix "A" with "n">0 can be computed recursively as

:mbox{Pf}(A)=sum_{i=2}^{2n}(-1)^{i}a_{1i}mbox{Pf}(A_{hat{1}hat{i),

where A_{hat{1}hat{i denotes the matrix "A" with both the first and "i"-th rows and columns removed.

Alternative definition

One can associate to any skew-symmetric 2"n"×2"n" matrix "A" ={"a""ij"} a bivector

:omega=sum_{i

where {"e"1, "e"2, …, "e"2"n"} is the standard basis of R2n. The Pfaffian is then defined by the equation

:frac{1}{n!}omega^n = mbox{Pf}(A);e^1wedge e^2wedgecdotswedge e^{2n},here ω"n" denotes the wedge product of "n" copies of ω with itself.

Derivation from Determinant

The Pfaffian can be derived from the determinant for a skew-symmetric matrix A as follows. Using Laplace's formula we can write the determinant as

:det(A)=(-1)^{p+1}a_{p1}A_{p1} + (-1)^{p+2}a_{p2}A_{p2}+cdots+(-1)^{n+p}a_{pn}A_{pn},

where A_{pi} is the p,i minor matrix of the matrix A.We further use Laplace's formula to note that

:det(A [A_{ij}] )=|A|^n,

since this determinant is that of an n imes n matrix whose only non-zero elements are the diagonals (each with value det(A)) and [A_{ij}] is a matrix whose i,jth component is the corresponding i,j minor matrix. In this way, following a proof by Parameswaran, we can write the determinant as,

:det(A)equivDelta_n=left| egin{array}{cccc}a_{11}&a_{12}&cdots&a_{1n}\a_{21}&a_{22}&cdots&a_{2n}\vdots&&&vdots\ a_{n1}&a_{n2}&cdots&a_{nn}end{array} ight
.

The minor of left| egin{array}{cc} a_{11}&a_{12}\a_{21}&a_{22}end{array} ight| would be Delta_{n-2}. With this notation:left| egin{array}{cccc}1&0&cdots&0\ 0&1&cdots&0\ a_{31}&a_{32}&cdots&a_{3n}\ cdots&cdots&cdots&cdots\ a_{n1}&a_{n2}&cdots&a_{nn}end{array} ight
imes left| egin{array}{cccc}A_{11}&A_{21}&cdots&A_{n1}\ A_{12}&A_{22}&cdots&A_{n2}\ A_{13}&A_{23}&cdots&A_{n3}\ cdots&cdots&cdots&cdots\ A_{1n}&A_{2n}&cdots&A_{nn}end{array} ight
=left| egin{array}{cc} A_{11}&A_{21}\A_{12}&a_{22}end{array} ight|Delta_n^{n-2}.

Thus

:Delta_{n-2}Delta_n^{n-1}=left| egin{array}{cc} A_{11}&A_{21}\A_{12}&a_{22}end{array} ight|Delta_n^{n-2}.

Of course, it was only arbitrarily that we chose to remove the first two rows, and more generically we can write

:A_{rr}A_{ss}-A_{rs}A_{sr}=Delta_{rs,rs}Delta_{n}

where Delta_{rs,rs} is the determinant of the original matrix with the rows r and s, as well as the columns r and s removed.The equation above simplifies in the skew-symmetric case to

:A_{rs} = sqrt{Delta_{rs,rs}Delta_n}.

We now plug this back into the original formula for the determinant,

:Delta_n=(-1)^{p+1}a_{p1}sqrt{Delta_{p1,p1}Delta_n} + (-1)^{p+2}a_{p2}sqrt{Delta_{p2,p2}Delta_n}+cdots+(-1)^{n+p}a_{pn}sqrt{Delta_{pn,pn}Delta_n},

or with slight manipulation,

:sqrt{Delta_n}=(-1)^{p+1}left( a_{p1}sqrt{Delta_{p1,p1 - a_{p2}sqrt{Delta_{p2,p2+cdots+(-1)^{n-1}a_{pn}sqrt{Delta_{pn,pn ight),

The determinant is thus the square of the right hand side, and so we identify the right hand side as the Pfaffian.

Identities

For a 2"n" &times; 2"n" skew-symmetric matrix "A" and an arbitrary 2"n" &times; 2"n" matrix "B",

*mbox{Pf}(A)^2 = det(A)

*mbox{Pf}(BAB^T)= det(B)mbox{Pf}(A)

*mbox{Pf}(lambda A) = lambda^n mbox{Pf}(A)

*mbox{Pf}(A^T) = (-1)^nmbox{Pf}(A)

* For a block-diagonal matrix

::A_1oplus A_2=egin{bmatrix} A_1 & 0 \ 0 & A_2 end{bmatrix},

: Pf("A"1⊕"A"2) = Pf("A"1)Pf("A"2).

*For an arbitrary "n" &times; "n" matrix "M":::mbox{Pf}egin{bmatrix} 0 & M \ -M^T & 0 end{bmatrix} = (-1)^{n(n-1)/2}det M.

Applications

*The Pfaffian is an invariant polynomial of a skew-symmetric matrix (note that it is not invariant under a general change of basis but rather under a proper orthogonal transformation). As such, it is important in the theory of characteristic classes. In particular, it can be used to define the Euler class of a Riemannian manifold which is used in the generalized Gauss-Bonnet theorem.

*The number of perfect matchings in a planar graph turns out to be the absolute value of a Pfaffian, hence is polynomial time computable. This is surprising given that for a general graph, the problem is very difficult (so called #P-complete). This result is used to calculate the partition function of Ising models of spin glasses in physics, respectively of Markov random fields in machine learning (Globerson and Jaakkola, 2007), where the underlying graph is planar. Recently it is also used to derive efficient algorithms for some otherwise seemingly intractable problems, including the efficient simulation of certain types of restricted quantum computation.

*The calculation of the number of possible ways to tile a standard chessboard or 8-by-8 checkerboard with 32 dominoes is a simple example of a problem which may be solved through the use of the Pfaffian technique. There are 12,988,816 possible ways to tile a chessboard in this manner. Specifically, 12988816 is the number of possible ways to cover an 8-by-8 square with 32 1-by-2 rectangles. 12988816 is a square number: 12988816 = 36042). Note that 12988816 can be written in the form: 2x1802^2+2x1802^2, where all the numbers have a digital root of 2.

:More generally, the number of ways to cover a 2n -by- 2n square with 2n^2 dominoes (as calculated independently by Temperley and M.E. Fisher and Kasteleyn in 1961) is given by

: prod_{j=1}^N prod_{k=1}^N left ( 4cos^2 frac{pi j}{2n + 1} + 4cos^2 frac{pi k}{2n + 1} ight ).

:This technique can be applied in many mathematics-related subjects, for example, in the classical, 2-dimensional computation of the dimer-dimer correlator function in quantum mechanics.

History

The term "Pfaffian" was introduced by Arthur Cayley, who used the term in 1852: "The permutants of this class (from their connection with the researches of Pfaff on differential equations) I shall term "Pfaffians"." The term honors German mathematician Johann Friedrich Pfaff.

ee also

*Dimer
*Polyomino
*Statistical mechanics

References

*"The statistics of dimers on a lattice, Part I", "Physica", vol.27, 1961, pp.1209-25, P.W. Kasteleyn.
* .
*.
*"The Games and Puzzles Journal", No.14, 1996, pp.204-5, Robin J. Chapman, University of Exeter
*"Domino Tilings and Products of Fibonacci and Pell numbers", "Journal of Integer Sequences", Vol.5, 2002, Article 02.1.2, James A. Sellers, The Pennsylvania State University
* "The Penguin Dictionary of Curious and Interesting Numbers", revised ed., 1997, ISBN 0-14-026149-4, David Wells, p.182.
* "A Treatise on the Theory of Determinants", 1882, Macmillan and Co., Thomas Muir, [http://books.google.com/books?id=pk4DAAAAQAAJ&dq=thomas+muir+treatise+on+the+theory+of+determinant&psp=1 "Online"]
* "Skew-Symmetric Determinants", "The American Mathematical Monthly", vol. 61, no.2., 1954, p.116, S. Parameswaran [http://www.jstor.org/stable/2307800 "JSTOR link"]

External links

* [http://planetmath.org/encyclopedia/Pfafian.html Pfaffian at PlanetMath.org]
* T. Jones, [http://www.physics.drexel.edu/~tim/open/pfaff/pfaff.pdf "The Pfaffian and the Wedge Product" (a demonstration of the proof of the Pfaffian/determinant relationship)]
* R. Kenyon and A. Okounkov, [http://www.ams.org/notices/200503/what-is.pdf "What is ... a dimer?"]
*


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