Deriving the continuity equation from the Dirac equation (Relativistic Quantum)

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SUMMARY

The continuity equation, expressed as \(\frac{\partial}{\partial x^{\mu}}J^{\mu} = 0\), can be derived from the Dirac equation \(i\gamma^{\mu} \frac{\partial}{\partial x^{\mu}}\Psi - \mu\Psi = 0\) and its Hermitian adjoint. The derivation involves multiplying the Dirac equation by the Dirac conjugate \(\overline{\Psi}\) and the adjoint by \(\Psi\), leading to the expression \(i(\frac{\partial}{\partial x^{\mu}}(\gamma^{\mu}\Psi)\overline{\Psi} + \frac{\partial}{\partial x^{\mu}}(\overline{\Psi})\gamma^{\mu}\Psi) - \mu(\Psi\overline{\Psi} - \overline{\Psi}\Psi)=0\). A critical point is ensuring the correct application of the product rule and the order of multiplication, particularly with respect to the matrix dimensions involved.

PREREQUISITES
  • Understanding of the Dirac equation and its components
  • Familiarity with Dirac conjugates and their properties
  • Knowledge of matrix multiplication and dimensions
  • Basic concepts of quantum field theory
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  • Study the derivation of the continuity equation in quantum mechanics
  • Explore the properties of Dirac matrices in relativistic quantum mechanics
  • Learn about the implications of the continuity equation in quantum field theory
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Physicists, particularly those specializing in quantum mechanics and quantum field theory, as well as students seeking to understand the derivation of fundamental equations in relativistic quantum mechanics.

toam
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So I am trying to derive the continuity equation:

\frac{\partial}{\partial x^{\mu}}J^{\mu} = 0

From the Dirac equation:

i\gamma^{\mu} \frac{\partial}{\partial x^{\mu}}\Psi - \mu\Psi = 0

And its Hermitian adjoint:

i\frac{\partial}{\partial x^{\mu}}\overline{\Psi}\gamma^{\mu} - \mu\overline{\Psi} = 0

Where:

\overline{\Psi}=\Psi^{+}\gamma^{0} (Dirac conjugate)



The Attempt at a Solution


By multiplying the Dirac equation on the right by \overline{\Psi} and the adjoint on the right by \Psi I get:

i(\frac{\partial}{\partial x^{\mu}}(\gamma^{\mu}\Psi)\overline{\Psi} + \frac{\partial}{\partial x^{\mu}}(\overline{\Psi})\gamma^{\mu}\Psi) - \mu(\Psi\overline{\Psi} - \overline{\Psi}\Psi)=0

The first term is basically what I am after (except I am not 100% sure I can simply apply the product rule - what is the correct order?) which means I shoudl expect the second term to go to zero:

\Psi\overline{\Psi} - \overline{\Psi}\Psi =0

But because \gamma^{0} is a 4x4 matrix, \Psi is a 4x1 and \overline{\Psi} is a 1x4, I should also expect the second term to be multiplied by the 4x4 identity matrix (so that the subtraction makes sense). However the first term is NOT a constant multiplied by the identity so I don't see how this works.



Any help would be greatly appreciated...
 
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toam said:
By multiplying the Dirac equation on the right by \overline{\Psi} and the adjoint on the right by \Psi …

Hi toam! :smile:

Don't you have to multiply one of them on the left? :confused:
 
I tried that and got something else that didn't work. However I will try again because I was surprised that it didn't work so I may have made a mistake or missed something obvious...
 
Ok so it turned out I had multiplied the wrong function on the left. It worked out quite simply when I fixed that. The lecture notes had erroneously shown both functions multiplied on the right.

Thanks, tiny-tim.
 

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