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What is the Casimir Effect ?
The Casimir effect is a small attractive force which acts
between two close parallel uncharged conducting plates. It
is due to quantum vacuum fluctuations of the electromagnetic
field.
The effect was predicted by the Dutch physicist Hendrick
Casimir in 1948. According to the quantum theory, the vacuum
contains virtual particles which are in a continuous state
of fluctuation (see physics FAQ article on
virtual particles ). Casimir realised that between
two plates, only those virtual photons whose wavelengths fit
a whole number of times into the gap should be counted when
calculating the vacuum energy. The energy density decreases
as the plates are moved closer which amplies there is a
small force drawing them together.
The attractive Casimir force between two plates of area
separated by a distance can be calculated to be,
pi2 h- c
F = ----------- A
240 a4
W here h- is Planck's constant over two pi and c is the
speed of light.
The tiny force was measured in 1996 by Steven Lamoreaux. His
results were in agreement with the theory to within the
experimental uncertainty of 5%.
Particles other than the photon also contribute a small
effect but only the photon force is measurable. All Bosons
such as photons produce an attractive Casimir force while
Fermions make a repulsive contribution. If electromagnetism
was supersymmetric there would be fermionic photinos whose
contribution would exactly cancel that of the photons and
there would be no Casimir effect. The fact that the Casimir
effect exists shows that if supersymmetry exists in nature
it must be a broken symmetry.
According to the theory the total zero point energy in the
vacuum is infinite when summed over all the possible photon
modes. The Casimir effect comes from a difference of
energies in which the infinities cancel. The energy of the
vacuum is a puzzle in theories of quantum gravity since it
should act gravitationally and produce a large cosmological
constant which would cause space-time to curl up. The
solution to the inconsistency is expected to be found in a
theory of quantum gravity.
References
H.B.G. Casimir, Proc. Kon. Ned. Akad. Wetensch. B51, 793
(1948)
S. Lamoreaux, Phys Rev Lett, 78, p5 (1996)
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