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Most recent edit on 2008-02-13 23:24:42 by CharlesFrancis

Additions:
where p satisfies the mass shell condition and u is a Dirac spinor» having the form, for r = 1, 2, and for a two-spinor ζ normalised so that Dirac-29

Deletions:
where p satisfies the mass shell condition and u is a Dirac spinor» having the form, for r = 1, 2, and for a two-spinor ζ normalised so that Dirac-29



Edited on 2008-01-08 03:40:48 by CharlesFrancis

Additions:
Dirac-28
Dirac-32
Dirac-33
Dirac-35
Dirac-37
Dirac-38
Dirac-39

Deletions:
Dirac-28
Proof:
Dirac-32
Dirac-33
Dirac-35
Dirac-37
Dirac-38
Dirac-39




Oldest known version of this page was edited on 2008-01-08 03:16:45 by CharlesFrancis []
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Solution of the Dirac Equation

The positive energy solutions to the Dirac equation are
Dirac-28
where p satisfies the mass shell condition and u is a Dirac spinor» having the form, for r = 1, 2, and for a two-spinor ζ normalised so that Dirac-29
Dirac-30
Proof:
Proof: Observe that
Dirac-31
So,
Dirac-32
Dirac-33
Dirac-34
Hence,
Dirac-35
Dirac-36
Dirac-37
Dirac-38
Dirac-39

Then, differentiation of the solution of the Dirac equation gives,
Dirac-40
Dirac-41
Dirac-42
as required.

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Normalisation of Dirac Spinors

The Pauli spin matrices are Hermition, so (as above)
Dirac-44
Then
Dirac-45
Dirac-46
Dirac-47

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