Klein-Gordon Equation & Continuity Equation

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Discussion Overview

The discussion focuses on the Klein-Gordon equation and its relationship to the continuity equation, particularly regarding the interpretation of probability density and current in quantum mechanics. Participants explore the implications of these equations, including the conditions under which probability density can be negative.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant presents the Klein-Gordon equation and continuity equation, expressing uncertainty about the normalization of the probability density and current.
  • Another participant questions whether the probability current 'j' must equal zero for conservation of probability, suggesting that 'j' may vary across the surface.
  • A different participant argues that a superposition of two plane waves with different positive energies can lead to a negative probability density, implying that the density is not always a valid probability measure.
  • Another participant notes that the dependence of the probability density on both the wave function and its time derivative can lead to negative values, suggesting that it may be more accurately described as charge density rather than probability density.
  • The original poster seeks clarification on the validity of using negative energy plane wave solutions to demonstrate that probability density can be negative.

Areas of Agreement / Disagreement

Participants express differing views on the interpretation of probability density and current, with some suggesting that negative values are possible under certain conditions. There is no consensus on whether the probability density can be considered a valid measure in all cases.

Contextual Notes

The discussion highlights limitations in the interpretation of the Klein-Gordon equation, particularly regarding the assumptions made about the wave function and its derivatives. The implications of negative probability density and the conditions under which it arises remain unresolved.

Sekonda
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Hello,

My question is on the Klein-Gordon equation and it's relation to the continuity equation, so for a Klein-Gordon equation & continuity equation of the following form, I have attained the following probability density and probability current relations (although not normalised correctly? If that's the correct term):

[tex]-\frac{\partial^2 }{\partial t^2}\psi +\bigtriangledown ^2\psi-m^2\psi=0 \: ,\: \frac{\partial }{\partial t}\rho +\mathbf{\bigtriangledown } \cdot \mathbf{j}=0[/tex]

[tex]\rho=i(\psi^{*}\dot{\psi}-\psi\dot{\psi^{*}})\,,\; \mathbf{j} =i(\psi\bigtriangledown \psi^{*}-\psi^{*}\bigtriangledown\psi)[/tex]

We then impose conservation of probability by making the time derivative of the probability equal to zero, and the following manipulation of this derivative is shown below:

[tex]\frac{\partial P}{\partial t}=\int_{V}\frac{\partial \rho}{\partial t}\, d^3x=-\int_{V}\bigtriangledown\cdot \mathbf{j}\, d^3x=-\oint_{S}\mathbf{j}\cdot d\mathbf{s}=0[/tex]

This above equation makes use of the divergence theorem in the last pair. This is true if j=0, but does j in general need to be equal to zero? I thought 'j' would vary around the surface and so the integration of all 'j' at each part on the surface would equal zero but not necessarily all 'j' =0.

To be honest I'm quite unsure at what 'j' represents in terms of probability!

Can anyone explain this?

Thanks,
SK
 
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Also I want to show that the probability density is not always positive but can be negative, so I tried substituting a plane wave solution of the form:

[tex]\psi\sim e^{-iEt+i\mathbf{p\cdot x}}[/tex]

into my probability density equation in the post above, but this gave me a positive answer - though if I use the negative energy plane wave solutions I will attain negative probability density (negative energy plane wave solutions attained by switching the signs in the exponent above), is this the correct way of showing this?

The -ve energies correspond to the -ve probabilities?
 
Sekonda, if you take a SUPERPOSITION of two plane waves with different positive energies, you will obtain that rho is not positive at some points. This implies that rho is NOT a probability density.

For some details, see also
http://arxiv.org/abs/0804.4564
 
there is a problem with single particle representation of klein-gordon eqn.you can see that ρ depends on both ψ and ∂ψ/∂t,and klein-gordon eqn itself is a second order differential eqn which requires both ψ and ∂ψ/∂t to be specified at say t=0.so they can take arbitrary value and hence can make ρ negative.it is here identified as charge density rather than probability density.
 
Thanks guys,

I think that link is a bit too complex for me but I think I understand how to go about the superposition of waves, I'll try it. Though is my negative energy plane-wave not also a simple and fair enough way of showing that the probability density can be negative - but this only occurs for negative energy solutions.

Cheers,
SK
 

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