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Superfluidity

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Superfluidity
NameSuperfluidity
CaptionThe creep effect in superfluid helium-4, demonstrating flow against gravity.
PhenomenaZero viscosity, quantized vortices, fountain effect, second sound
DiscoveredPyotr Kapitsa, John F. Allen, Don Misener (1937)
RelatedSuperconductivity, Bose–Einstein condensate, Quantum hydrodynamics

Superfluidity. It is a state of matter characterized by the complete absence of viscosity, allowing flow without energy dissipation. This macroscopic quantum phenomenon was first observed in liquid helium-4 below the lambda point. The behavior defies classical fluid dynamics, exhibiting remarkable effects like frictionless motion and quantized circulation.

Discovery and history

The phenomenon was discovered in 1937 by a team led by Soviet physicist Pyotr Kapitsa at the Institute for Physical Problems in Moscow, alongside the independent work of John F. Allen and Don Misener at the University of Cambridge. Their experiments on liquid helium-4 revealed its ability to flow through extremely narrow capillaries without resistance. This followed earlier observations of anomalous heat capacity by Willem Hendrik Keesom and the identification of the lambda point by his daughter Anna Petronella Keesom. Theoretical groundwork was laid by Fritz London, who suggested a connection to Bose–Einstein statistics, a concept later expanded by Lev Landau in his two-fluid model. The discovery of superfluidity in the fermionic isotope helium-3 by the team of David Lee, Douglas D. Osheroff, and Robert C. Richardson at Cornell University in the 1970s, for which they received the Nobel Prize in Physics, marked a major extension of the field.

Fundamental properties

A superfluid exhibits several defining characteristics absent in normal fluids. It possesses zero viscosity, enabling perpetual flow in a closed loop. This leads to the creep effect, where a film of superfluid can move over container walls. It supports non-classical wave propagation known as second sound, which is a temperature wave. The circulation of a superfluid is quantized, meaning its angular momentum can only take discrete values set by Planck's constant. This quantization gives rise to stable topological defects called quantized vortices. The fluid also displays an extremely high thermal conductivity, making it an effective conductor of heat. The fountain effect, demonstrated by Jack Allen and Harry Jones, occurs when heat applied to a superfluid generates a mechanical pressure gradient.

Theoretical explanation

The primary theoretical framework for superfluidity in helium-4 is provided by the two-fluid model developed by Lev Landau and later refined by László Tisza. This model treats the liquid as an interpenetrating mixture of a normal viscous component and an inviscid superfluid component. At a microscopic level, superfluidity in bosonic systems like helium-4 is explained by the formation of a macroscopic wave function, analogous to a Bose–Einstein condensate, as proposed by Fritz London. For fermionic systems like helium-3, the explanation requires the formation of Cooper pairs via an attractive interaction, analogous to the BCS theory of superconductivity developed by John Bardeen, Leon Cooper, and John Robert Schrieffer. The mathematical description of superfluid dynamics often employs the Gross–Pitaevskii equation.

Experimental observations

Key experiments have vividly demonstrated its unique properties. The classic Hess–Fairbank experiment at Yale University directly measured the momentum of inertia, showing it was less than that of a classical fluid, confirming irrotational flow. Observations of quantized vortices were made by William Vinen using a vibrating wire technique. The Andronikashvili experiment, devised by Élevter Andronikashvili, used a stack of rotating disks to separate the normal and superfluid components, validating the two-fluid model. The fountain effect is readily observed in apparatus like the Rollin film setup. In ultracold atomic gases, the creation of Bose–Einstein condensates by teams led by Eric Cornell, Carl Wieman, and Wolfgang Ketterle allowed direct visualization of superfluid behaviors, including vortex lattices, using techniques like time-of-flight imaging.

While practical applications are often constrained by the cryogenic temperatures required, superfluidity is a cornerstone of low-temperature physics. It is essential for high-precision devices like SQUID magnetometers and in providing ultra-stable environments for experiments in metrology. The study of quantized vortices and quantum turbulence informs research in astrophysics, particularly regarding the interior dynamics of neutron stars. The phenomenon is intimately related to superconductivity, with the flow of charge carriers in a superconductor being analogous to the frictionless flow of a superfluid. Research into non-equilibrium states and the Kibble–Zurek mechanism connects superfluidity to concepts in cosmology and phase transitions. The field continues to expand with studies of polaritons in semiconductor microcavities and supersolidity. Category:Condensed matter physics Category:Quantum mechanics Category:States of matter Category:Low-temperature physics