Nonlinear vacuum permittivity?

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Discussion Overview

The discussion revolves around the concept of nonlinear vacuum permittivity and its implications in the presence of strong electric fields, particularly in relation to the creation of electron-positron pairs from the vacuum. Participants explore theoretical aspects, historical context, and related phenomena in quantum electrodynamics (QED).

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants suggest that vacuum permittivity may not be constant under strong electric fields, potentially leading to the creation of electron-positron pairs.
  • One participant mentions "vacuum sparking" as a phenomenon where high field energy density can excite electron/positron degrees of freedom.
  • Another participant refers to vacuum polarization in QED, noting that as the electric field increases, the vacuum can polarize, affecting its permittivity and leading to radiative corrections.
  • Historical references are made to Heisenberg and Euler's work on the topic, indicating that this is a recognized area of study in theoretical physics.
  • Participants discuss vacuum birefringence, which is predicted by QED as a change in refractive index under strong electric fields, and its relevance to current research.
  • One participant describes the instability of constant electric fields in the context of nonlinear QED equations, suggesting a decay into electron-positron pairs that could weaken the original field.

Areas of Agreement / Disagreement

Participants express various viewpoints on the nature of vacuum permittivity and its behavior under strong fields, with no consensus reached on the implications or interpretations of these phenomena.

Contextual Notes

The discussion includes references to specific phenomena and theoretical frameworks, but lacks detailed mathematical derivations or empirical evidence to support the claims made. The implications of nonlinear effects in vacuum permittivity remain an area of active inquiry.

Pythagorean
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I've been told recently that the vacuum permittivity, given a sufficiently strong electric field, is not a constant, as it can cause positron-electron pair to split out of the vacuum.

1) is this true?
2) if so, where do such pairs as the positron-electron come from in a vacuum?

I did try to research this myself, but I wasn't able to find it. If there's a name for the phenomena, it would be helpful in searching.
 
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There is a phenomenon called "vacuum sparking", where the field energy density becomes high enough to excite electron/positron degrees of freedom. I confess I haven't thought about it in terms of permittivity.
 
Pythagorean said:
I've been told recently that the vacuum permittivity, given a sufficiently strong electric field, is not a constant, as it can cause positron-electron pair to split out of the vacuum.

1) is this true?
2) if so, where do such pairs as the positron-electron come from in a vacuum?

I did try to research this myself, but I wasn't able to find it. If there's a name for the phenomena, it would be helpful in searching.


True;
In QED its usually referred to as vacuum polarization (of the virtual particle pairs).

In materials non-linear permittivity is well known...in the vacuum it is not as commonly appreciated.
As the field gets high enough or as one gets close enough to a charge source the vacuum begins to polarize (in effect changing the 'permittivity'), and necessitating what is called "radiative corrections" . If the field is high enough (say from colliding two high Z nucleii) then a "critical vacuum" can be reached whereby the energy of the field gets up to 2 mc^2 and the virtual particle-antiparticle pair becomes real.

..
Creator
 
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I think there is a paper by Uehling (Phys Rev, 1935) on the vacuum polarization renormalization of Coulomb charge at short distances. See
http://prola.aps.org/abstract/PR/v48/i1/p55_1
Sorry, this is pay per view.
Also look up Uehling integral in Google.
Bob S
 
..

Furthermore, to add to my previous post,...
...Because the vacuum acts as a polarizable medium QED predicts vacuum birefringence, (refractive index change in othogonal directions), at sufficiently high electric fields. Detection of vacuum birefringement in the vacinity of highly intense laser fields is currently an active area of research.
see :http://www.slac.stanford.edu/xorg/ilcac/talks/heinzl.pdf

Magnetic vacuum birefringence is also a possibility at high magnetic field strength, and is actively being sought with sensitive ellipsometry.
see for ex,: http://www.spectro.jussieu.fr/QED2005/Talks/Chen.pdf

Creator
 
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The problem is easy to understand: as soon as the QED equations are non linear, the Lagrangian is not really quadratic function of E. There is no the principle of superposition of fileds: there is a reaction to an external field E. There is some sort of instability of any constant field E. The state decays into E plus electron-positron couples that weaken the original filed. Kind of tunnelling.
 
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