Complex Scalar Field and Probability Field

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SUMMARY

The discussion centers on the relationship between the Lagrangian for a free complex scalar field and the conserved current for probability, specifically highlighting the equation ∂ρ/∂t = ∇·j. The conserved current is defined as jα = -i(ψ*αψ - ψ∂αψ*), derived from the Lagrangian ℒ = ∂αψ*αψ. The author suggests that this Lagrangian may represent a free field of probability, drawing parallels to historical interpretations in relativistic quantum mechanics.

PREREQUISITES
  • Understanding of Lagrangian mechanics
  • Familiarity with complex scalar fields
  • Knowledge of conserved currents in quantum field theory
  • Basic concepts of probability density and current
NEXT STEPS
  • Research the implications of the Lagrangian ℒ = ∂αψ*αψ in quantum field theory
  • Explore the historical context of the complex scalar field in relativistic quantum mechanics
  • Investigate the relationship between phase invariance and probability interpretation in quantum mechanics
  • Study the transition from the Schrödinger field to the Klein-Gordon field
USEFUL FOR

The discussion is beneficial for theoretical physicists, quantum field theorists, and students of advanced quantum mechanics interested in the foundational aspects of complex scalar fields and their interpretations.

jfy4
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Hi,

I was looking at the lagrangian and conserved currents for the free complex scalar field and it looks like it has a striking similarity to the conserved current for probability:
[tex] \frac{\partial \rho}{\partial t}=\nabla\cdot \vec{j}[/tex]
where [itex]j_i =-i(\psi^{\ast}\partial_i \psi - \psi\partial_i \psi^{\ast})[/itex] and [itex]\rho[/itex] is the probability density. Then with the action
[tex] \mathcal{L}=\partial_\alpha \psi^{\ast}\partial^\alpha \psi[/tex]
the conserved current is
[tex] j^{\alpha}=-i(\psi^\ast \partial^\alpha \psi - \psi \partial^\alpha \psi^\ast )[/tex]
Then I had the thought that with the conservation of probability current, the above lagrangian appears to be a lagrangian for a free field of...probability. Now I'm aware that the complex scalar field is used to describe various spin-0 particles, but has anyone heard of any other possible thoughts on this lagrangian, maybe back when it was first put forward, or when anyone was just looking at relativistic quantum mechanics about 100 years ago?
 
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There's no coincidence. The so-called Schroedinger field described by a complex wavefunction in a Galilei invariant space-time goes into the complex free KG field. But when the probability interpretation of the current derived from phase invariance fails, a new interpretation is necessary, the electric charge one.

This is classic stuff described in a gazillion of books.
 
Good to know, thanks.
 

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