Fermion condensate

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A fermion condensate (also Fermi condensate ) is a superfluid aggregate state in a system of fermions . The effect is based - analogous to the Bose-Einstein condensate of bosons - on the superposition of the wave functions of the fermions involved, whereupon these assume a uniform quantum state .

generation

Fermions do not line up ( Pauli principle ), so it's only by a degeneration in the spin - quantum number possible. This is achieved in that two fermions each (with spin ½) combine to form a boson (spin 1), which in turn condense to form a Bose-Einstein condensate.

One possibility for this is that molecules of two fermions form and behave as bosons. Bose-Einstein condensates of such molecules were first produced almost simultaneously in 2003 by the working groups led by Rudolf Grimm at the University of Innsbruck and Deborah Jin at the American National Institute of Standards and Technology .

In contrast to the formation of molecules from two fermions, it is also conceivable that the two fermions interact over greater distances, as occurs, for example, in the analogous case of electrons ( Cooper pairs ) in superconductors . First steps in this direction were taken in 2004 with an ultracold gas made of potassium atoms in the research group of Deborah Jin. A similar effect is also for the superfluidity of helium - isotope 3 responsible He.

All of these phenomena are only possible at extremely low temperatures.

See also

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