nLab
Pfaffian

Contents

Idea

The Pfaffian of a skew-symmetric matrix is a square root of its determinant.

Definition

Let A=(A i,j) be a skew-symmetric (2n×2n)-matrix with entries in some field (or ring) k.

Definition

The Pfaffian Pf(A)k is the element

12 nn! σS 2nsgn(σ) i=1 nA σ(2i1),σ(2i),\frac{1}{2^n n!} \sum_{\sigma \in S_{2n}} sgn(\sigma) \prod_{i = 1}^n A_{\sigma(2i -1), \sigma(2i)} \,,

where

Properties

In terms of Berezinian integrals

Proposition

Let Λ 2n be the Grassmann algebra on 2n generators {θ i}, which we think of as a vector θ

Then the Pfaffian Pf(A) is the Berezinian integral

Pf(A)=exp(θ,Aθ)dθ 1dθ 2dθ 2n.Pf(A) = \int \exp( \langle \vec \theta, A \cdot \vec \theta \rangle ) d \theta_1 d \theta_2 \cdots d \theta_{2n} \,.
Remark

Compare this to the Berezinian integral representation of the determinant, which is

det(A)exp(θ,Aψ)dθ 1dθ 2dθ 2ndψ 1dψ 2dψ 2n.det(A) \propto \int \exp( \langle \vec \theta, A \cdot \vec \psi \rangle ) d \theta_1 d \theta_2 \cdots d \theta_{2n} d \psi_1 d \psi_2 \cdots d \psi_{2n} \,.

Pfaffian state

Pfaffians appear in the expression of certain multiparticle wave functions. Most notable is the pfaffian state of N spinless electrons

Ψ Pf(z 1,,z N)=pfaff(1z kz l) i<j(z iz j) qexp(14z 2)\Psi_{Pf}(z_1,\ldots,z_N) = pfaff\left(\frac{1}{z_k-z_l}\right)\prod_{i\lt j}(z_i-z_j)^q exp(-\frac{1}{4}\sum |z|^2)

where pfaff(M kl) denotes the Pfaffian of the matrix whose labels are k,l and q=1/ν is the filling fraction, which is an even integer. For Pfaffian state see

  • Gregory Moore, N. Read, Nonabelions in the fractional quantum hall effect, Nucl. Phys. 360B(1991)362 pdf