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Superfluidity is the characteristic property of a with zero which therefore flows without any loss of . When stirred, a superfluid forms that continue to rotate indefinitely. Superfluidity occurs in two of (helium-3 and helium-4) when they are liquefied by cooling to temperatures. It is also a property of various other exotic states of matter theorized to exist in , high-energy physics, and theories of . The theory of superfluidity was developed by Soviet theoretical physicists and Isaak Khalatnikov.

Superfluidity often co-occurs with Bose–Einstein condensation, 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 .


Superfluidity of liquid helium
Superfluidity was discovered in helium-4 by and independently by John F. Allen and in 1937. Onnes possibly observed the superfluid on August 2 1911, the same day that he observed superconductivity in mercury. It has since been described through phenomenology and microscopic theories.

In liquid helium-4, the superfluidity occurs at far higher temperatures than it does in helium-3. Each atom of helium-4 is a particle, by virtue of its . A helium-3 atom is a 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 in superconductivity.


Cold atomic gases
Superfluidity in an ultracold was experimentally proven by Wolfgang Ketterle and his team who observed in lithium-6 at a temperature of 50 nK at MIT in April 2005. Such vortices had previously been observed in an ultracold using rubidium-87 in 2000, and more recently in two-dimensional gases. As early as 1999, created such a condensate using atoms for the purpose of slowing light, and later stopping it completely. Her team subsequently used this system of compressed light to generate the superfluid analogue of shock waves and tornadoes:


Superfluids in astrophysics
The idea that superfluidity exists inside was first proposed by . By analogy with electrons inside forming because of electron–lattice interaction, it is expected that in a neutron star at sufficiently high density and low temperature can also form Cooper pairs because of the long-range attractive nuclear force and lead to superfluidity and superconductivity.
(2025). 9783540423409


In high-energy physics and quantum gravity
Superfluid vacuum theory (SVT) is an approach in theoretical physics and quantum mechanics where the physical is viewed as superfluid.

The ultimate goal of the approach is to develop scientific models that unify quantum mechanics (describing three of the four known fundamental interactions) with . This makes SVT a candidate for the theory of and an extension of the .

It is hoped that development of such a theory would unify into a single consistent model of all fundamental interactions, and to describe all known interactions and elementary particles as different manifestations of the same entity, superfluid vacuum.

On the macro-scale a larger similar phenomenon has been suggested as happening in the of . The rapidity of change in flight patterns mimics the phase change leading to superfluidity in some liquid states.

Light behaves like a superfluid in various applications such as Poisson's Spot. As the liquid helium shown above, light will travel along the surface of an obstacle before continuing along its trajectory. Since light is not affected by local gravity its "level" becomes its own trajectory and velocity. Another example is how a beam of light travels through the hole of an aperture and along its backside before diffraction.


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