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Proca action

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Title: Proca action  
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Subject: Quantum field theory, Anomaly (physics), Crossing (physics), Effective field theory, Faddeev–Popov ghost
Collection: Quantum Field Theory
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Proca action

In physics, specifically field theory and particle physics, the Proca action describes a massive spin-1 field of mass m in Minkowski spacetime. The corresponding equation is a relativistic wave equation called the Proca equation.[1] The Proca action and equation are named after Romanian physicist Alexandru Proca.

This article uses the (+−−−) metric signature and tensor index notation in the language of 4-vectors.


  • Lagrangian density 1
  • Equation 2
  • Gauge fixing 3
  • See also 4
  • References 5
  • Further reading 6

Lagrangian density

The field involved is the 4-potential Aμ = (φ/c, A), where φ is the electric potential and A is the magnetic potential. The Lagrangian density is given by:

\mathcal{L}=-\frac{1}{16\pi}(\partial^\mu A^\nu-\partial^\nu A^\mu)(\partial_\mu A_\nu-\partial_\nu A_\mu)+\frac{m^2 c^2}{8\pi \hbar^2}A^\nu A_\nu.

where c is the speed of light, ħ is the reduced Planck constant, and ∂μ is the 4-gradient.


The Euler–Lagrange equation of motion for this case, also called the Proca equation, is:

\partial_\mu(\partial^\mu A^\nu - \partial^\nu A^\mu)+\left(\frac{mc}{\hbar}\right)^2 A^\nu=0

which is equivalent to the conjunction of[2]

\left[\partial_\mu \partial^\mu+ \left(\frac{mc}{\hbar}\right)^2\right]A^\nu=0

with (in the massive case)

\partial_\mu A^\mu=0 \!

which may be called a generalized Lorenz gauge condition. The field A^\nu transforms like a four-vector, but consists in contrary to electromagnetism generally of four complex valued functions.[3]

When m = 0, the equations reduce to Maxwell's equations without charge or current. The Proca equation is closely related to the Klein–Gordon equation, because it is second order in space and time.

In the more familiar vector calculus notation, the equations are:

\Box \phi - \frac{\partial }{\partial t} \left(\frac{1}{c^2}\frac{\partial \phi}{\partial t} + \nabla\cdot\mathbf{A}\right) =-\left(\frac{mc}{\hbar}\right)^2\phi \!
\Box \mathbf{A} + \nabla \left(\frac{1}{c^2}\frac{\partial \phi}{\partial t} + \nabla\cdot\mathbf{A}\right) =-\left(\frac{mc}{\hbar}\right)^2\mathbf{A}\!

and \Box is the D'Alembert operator.

Gauge fixing

The Proca action is the gauge-fixed version of the Stueckelberg action via the Higgs mechanism. Quantizing the Proca action requires the use of second class constraints.

They are not invariant under the electromagnetic gauge transformations

A^\mu \rightarrow A^\mu - \partial^\mu f

where f is an arbitrary function, except for when m = 0.

See also


  1. ^ Particle Physics (2nd Edition), B.R. Martin, G. Shaw, Manchester Physics, John Wiley & Sons, 2008, ISBN 978-0-470-03294-7
  2. ^ McGraw Hill Encyclopaedia of Physics (2nd Edition), C.B. Parker, 1994, ISBN 0-07-051400-3
  3. ^ W. Greiner, "Relativistic quantum mechanics", Springer, p. 359, ISBN 3-540-67457-8

Further reading

  • Supersymmetry P. Labelle, Demystified, McGraw–Hill (USA), 2010, ISBN 978-0-07-163641-4
  • Quantum Field Theory, D. McMahon, Mc Graw Hill (USA), 2008, ISBN 978-0-07-154382-8
  • Quantum Mechanics Demystified, D. McMahon, Mc Graw Hill (USA), 2006, ISBN(10-) 0-07-145546 9
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