The Physics Hypertextbook™
© 1998-2008 by Glenn Elert -- A Work in Progress
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Pyotr Kapitsa, Soviet Union
Helium I vs. helium II. Helium II is a different phase than helium I
Helium liquefies under normal pressures at 4.2 K. From 4.2 K to 2.17 K it behaves like many other liquids, although it has an exceptionally low
surface tension and is extremely transparent. Below 2.2 K it behaves quite differently.
The mechanisms for this phase transition, and the details of the superfluidity in 4He and 3He, are very different. 4He has an even number of constituent particles (protons, electrons, and neutrons), which makes it a boson, meaning it is governed by Bose-Einstein statistics. At low temperatures, all the bosons in a sample will want to occupy the same quantum-mechanical ground state, forming a Bose-Einstein condensate. This condensate is responsible for the superfluid behavior of 4He below Tλ = 2.17 K.
In contrast, 3He is a fermion, since it has one less neutron than 4He. Fermions obey the Pauli exclusion principle, which says that in a sample of many identical fermions, no two can occupy the same quantum-mechanical state. Bose-Einstein condensation is ruled out for 3He, so another mechanism is needed to explain its superfluid behavior. That mechanism is provided by the Bardeen-Cooper-Schrieffer (BCS) theory.
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