The Casimir effect is an attractive force between two uncharged conducting plates due to quantum vacuum fluctuations.At a distance of 10 nanometers, two mirror plates are compressed with a pressure of one atmosphere, even though there is an absolute vacuum around them. This is the Casimir effect: quantum fluctuations give rise to a real force in the void. The vacuum constantly boils with pairs of particles and antiparticles that exist for instants. In the gap between the plates, only those fluctuations fit whose wavelength is a multiple of the distance—like standing waves on a string. Outside, however, the spectrum is unrestricted. As a result, the 'population' of particles is larger outside, and it presses on the plates, pushing them together. The force quickly weakens with increasing gap—inversely proportional to the fourth power.
The idea came to Casimir during discussions with Bohr about the properties of colloidal solutions. Together with Dirk Polder, he derived a formula for the force between two perfectly conducting plates. Later, Evgeny Lifshitz generalized the theory to real materials, taking into account finite conductivity and roughness. The first confident measurement was made by Steve Lamoreaux in 1997 using torsion balances; it was followed by experiments with an atomic force microscope that confirmed the dependence on distance and surface properties.
Quantization of the electromagnetic field in the presence of boundaries leads to a renormalization of the zero-point energy. The mode density between the plates is lower than in the outer space, and the integrated pressure difference yields an attractive force. In the formula, the force is inversely proportional to the fourth power of the distance. For real metals at small distances, retardation starts to play a role, and the force transitions to the van der Waals force. At higher temperatures, thermal fluctuations enhance the effect.
The effect causes tiny parts in microchips to stick together without any lubricant.
If the plates were perfectly smooth and infinite, the Casimir force at microscopic distances could reach tens of atmospheres.






















