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Dirac operator

In mathematics and quantum mechanics, a Dirac operator is a differential operator that is a formal square root, or half-iterate, of a second order operator such as a Laplacian. The original case which concerned Dirac was to factorise formally an operator for Minkowski space, to get a form of quantum theory compatible with special relativity; to get the relevant Laplacian as a product of first order operators he introduced spinors.

In general, let D be a first-order differential operator acting on a vector bundle V over a Riemannian manifold M.

If

D^2=\triangle,

\triangle being the Laplacian of V, D is called a Dirac operator.

In high-energy physics, this requirement is often relaxed: only the second-order part of D2 must equal the Laplacian.

Examples

1: -i\partial_x is a Dirac operator on the tangential bundle over a line.

2: We now consider a simple bundle of importance in physics: The configuration space of a particle with spin \begin{matrix}\frac{1}{2}\end{matrix} confined to a plane, which is also the base manifold. Physicists generally think of wavefunctions \psi:\mathbb{R}^2\to\mathbb{C}^2 which they write

\begin{pmatrix}\chi(x,y) \\ \eta(x,y)\end{pmatrix}.

x and y are the usual coordinate functions on \mathbb{R}^2. χ specifies the probability amplitude for the particle to be in the spin-up state, similarly for η. The so-called spin-Dirac operator can then be written

D=-i\sigma_x\partial_x-i\sigma_y\partial_y,

where σi are the Pauli matrices. Note that the anticommutation relations for the Pauli matrices make the proof of the above defining property trivial. Those relations define the notion of a Clifford algebra.

3: The most famous Dirac operator describes the propagation of a free electron in three dimensions and is elegantly written

D=\gamma^\mu\partial_\mu

using Einstein's summation convention.

See also

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