Dirac operator: Difference between revisions
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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 [[spinor]]s. |
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[[vector bundle]] <math>V</math> over a [[Riemannian manifold]] <math>M</math>. |
[[vector bundle]] <math>V</math> over a [[Riemannian manifold]] <math>M</math>. |
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:<math>D^2=\triangle,</math> |
:<math>D^2=\triangle,</math> |
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<math>\triangle</math> being the |
<math>\triangle</math> being the Laplacian of <math>V</math>, <math>D</math> is |
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called a '''Dirac operator'''. |
called a '''Dirac operator'''. |
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3: The most famous Dirac operator describes the propagation of a free electron in |
3: The most famous Dirac operator describes the propagation of a free electron in |
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three dimensions and is elegantly written <math>D=\gamma^\mu\partial_\mu</math> |
three dimensions and is elegantly written |
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:<math>D=\gamma^\mu\partial_\mu</math> |
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using Einstein's summation convention. |
using [[Einstein's summation convention]]. |
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==See also== |
==See also== |
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[[Clifford algebra]], [[Connection (mathematics)|Connection]], [[Dolbeault operator]], [[manifold]], |
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*[[Clifford algebra]] |
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[[Riemannian geometry]], [[Heat kernel]]. |
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*[connection (mathematics)|Connection]] |
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*[[Dolbeault operator]] |
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*[[Heat kernel]]. |
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[[Category:Differential operators]] |
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[[Category:Quantum mechanics]] |
Revision as of 15:08, 18 October 2004
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 be a first-order differential operator acting on a vector bundle over a Riemannian manifold .
If
being the Laplacian of , is called a Dirac operator.
In high-energy physics, this requirement is often relaxed: only the second-order part of must equal the Laplacian.
Examples
1: 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 confined to a plane, which is also the base manifold. Physicists generally think of wavefunctions which they write
and are the usual coordinate functions on . specifies the probability amplitude for the particle to be in the spin-up state, similarly for . The so-called spin-Dirac operator can then be written
where 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
using Einstein's summation convention.
See also
- Clifford algebra
- [connection (mathematics)|Connection]]
- Dolbeault operator
- Heat kernel.