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Superfluidity

Fluid which flows without losing kinetic energy

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Through Fluid, Viscosity and Isotope

Superfluidity often co-occurs with Bose–Einstein condensation (BEC), but neither phenomenon is directly related to the other; not all Bose–Einstein condensates can be regarded as superfluids, and not all superfluids are Bose–Einstein condensates. Even when superfluidity and condensation co-occur, their magnitudes are not linked: at low temperature, liquid helium has a large superfluid fraction but a low condensate fraction; while a weakly interacting BEC, with almost unity condensate fraction, can display a vanishing superfluid fraction.

Superfluids have some potential practical uses, such as dissolving substances in a quantum solvent.

Superfluidity of liquid helium

Superfluidity was discovered in helium-4 by Pyotr Kapitsa and independently by John F. Allen and Don Misener in 1937. Onnes possibly observed the superfluid phase transition on August 2 1911, the same day that he observed superconductivity in mercury. It has since been described through phenomenology and microscopic theories. Only Kapitza received the Nobel Prize for this discovery. The accepted macroscopic theory of superfluidity in helium-4 was developed by Lev Landau in 1941. [L. D. Landau, J. Phys. USSR 5, 71 (1941), "The Theory Of Superfluidity In Helium II".] Landau received the Nobel Prize for this work in 1962.

In liquid helium-4, the superfluidity occurs at far higher temperatures than it does in helium-3. Each atom of helium-4 is a boson particle, by virtue of its integer spin. A helium-3 atom is a fermion particle; it can form bosons only by pairing with another particle like itself, which occurs at much lower temperatures. The discovery of superfluidity in helium-3 was the basis for the award of the 1996 Nobel Prize in Physics. This process is similar to the electron pairing in superconductivity.

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