Quantum field theory

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In physics, specifically field theory and particle physics, the Proca action describes a massive spin1 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 4vectors.
Contents

Lagrangian density 1

Equation 2

Gauge fixing 3

See also 4

References 5

Further reading 6
Lagrangian density
The field involved is the 4potential A^{μ} = (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 4gradient.
Equation
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 fourvector, 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 gaugefixed 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
References

^ Particle Physics (2nd Edition), B.R. Martin, G. Shaw, Manchester Physics, John Wiley & Sons, 2008, ISBN 9780470032947

^ McGraw Hill Encyclopaedia of Physics (2nd Edition), C.B. Parker, 1994, ISBN 0070514003

^ W. Greiner, "Relativistic quantum mechanics", Springer, p. 359, ISBN 3540674578
Further reading

Supersymmetry P. Labelle, Demystified, McGraw–Hill (USA), 2010, ISBN 9780071636414

Quantum Field Theory, D. McMahon, Mc Graw Hill (USA), 2008, ISBN 9780071543828

Quantum Mechanics Demystified, D. McMahon, Mc Graw Hill (USA), 2006, ISBN(10) 007145546 9
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