Quantum Field Theory – Understanding the Dynamic Casimir Effect

casimir-effectquantum-field-theory

A few years ago, when i studied the casimir effect interpretation as the filtering out of vacuum modes with appropiate boundary conditions, i had the following dilemma; supposedly the derivation of the force between the walls was entirely equivalent to just calculating Van der Waals forces. This, as it was argued, compelled us to not take too seriously the idea of a negative energy density of the space between the walls.

However, i was left wondering what would happen if one would take the interpretation based on vacuum modes a bit further, and we could somehow switch on and off the permitivity $\epsilon$ of the conductor; what sort of long range radiation we would expect to see?
A possible experimental implementation would be if the layers where superconductive, and then a magnetic field would be switched on just to break the superconductive phase.

We probably need to use the Dirac-Heisenberg-Wigner formalism for these sort of dynamic quantum systems, but what would be intuitively expected to be detected?

Best Answer

A friend recently brought to my attention that this experiment was actually performed 6 months after i posted the question in this site:

http://blogs.nature.com/news/2011/11/light_coaxed_from_nothingness.html

http://www.chalmers.se/en/news/pages/chalmers-scientists-create-light-from-vacuum.aspx

Christopher Wilson from Chalmers (and his team) used the same mechanism that i've proposed in here: using a superconducting magnet to oscillate the mirror surface.

I'm glad to see that the idea really works!

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