Dirac adjoint

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In quantum field theory, the Dirac adjoint \bar\psi of a Dirac spinor \ \psi is defined to be the dual spinor \ \psi^{\dagger} \gamma^0, where \ \gamma^0 is the time-like gamma matrix. Possibly to avoid confusion with the usual Hermitian adjoint \psi^\dagger, some textbooks do not give a name to the Dirac adjoint, simply calling it "psi-bar".

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[edit] Motivation

The Dirac adjoint is motivated by the need to form well-behaved, measurable quantities out of Dirac spinors. For example, \psi^\dagger\psi is not a Lorentz scalar, and \psi^\dagger\gamma^\mu\psi is not even Hermitian. One source of trouble is that if λ is the spinor representation of a Lorentz transformation, so that

\psi\to\lambda\psi,

then

\psi^\dagger\to\psi^\dagger\lambda^\dagger.

Since the Lorentz group of special relativity is not compact, λ will not be unitary, so \lambda^\dagger\neq\lambda^{-1}. Using \bar\psi fixes this problem, in that it transforms as

\bar\psi\to\bar\psi\lambda^{-1}.

[edit] Usage

Using the Dirac adjoint, the probability density for a spin-1/2 particle field can be written as

\rho = \bar\psi \psi

and the current can be written as

j^\mu = \bar\psi\gamma^\mu\psi.

[edit] See also

[edit] References

  • B. Bransden and C. Joachain (2000). Quantum Mechanics, 2e, Pearson. ISBN 0-582-35691-1.
  • M. Peskin and D. Schroeder (1995). An Introduction to Quantum Field Theory, Westview Press. ISBN 0-201-50397-2.
  • A. Zee (2003). Quantum Field Theory in a Nutshell, Princeton University Press. ISBN 0-691-01019-6.
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