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Carsten Timm: Theory of superconductivity

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Superconductivity with rather high T c has also been found in fullerites, i.e., compounds containing fullerene<br />

anions. The record T c in this class is at present T c = 38 K for b.c.c. Cs 3 C 60 under pressure. Superconductivity<br />

in fullerites was originally thought to be driven by phonons with strong molecular vibration character but there<br />

is recent evidence that it might be unconventional (not phonon-driven).<br />

2.2 Superfluid helium<br />

In 1937 P. Kapiza and independently Allen and Misener discovered that helium shows a transition at T c = 2.17 K<br />

under ambient pressure, below which it flows through narrow capilaries without resistance. The analogy to<br />

<strong>superconductivity</strong> is obvious but here it was the viscosity instead <strong>of</strong> the resistivity that dropped to zero. The<br />

phenomenon was called superfluidity. It was also observed that due to the vanishing viscosity an open container<br />

<strong>of</strong> helium would empty itself through a flow in the microscopically thin wetting layer.<br />

He<br />

On the other hand, while part <strong>of</strong> the liquid flows with vanishing viscosity, another part does not. This was shown<br />

using torsion pendulums <strong>of</strong> plates submerged in helium. For T > 0 a temperature-dependent normal component<br />

oscillates with the plates.<br />

He<br />

Natural atmospheric helium consists <strong>of</strong> 99.9999 % He-4 and only 0.0001 % He-3, the only other stable isotope.<br />

The oberserved properties are thus essentially indistinguishable from those <strong>of</strong> pure He-4. He-4 atoms are bosons<br />

since they consist <strong>of</strong> an even number (six) <strong>of</strong> fermions. For weakly interacting bosons, A. Einstein predicted in<br />

1925 that a phase transition to a condensed phase should occur (Bose-Einstein condensation). The observation<br />

<strong>of</strong> superfluidity in He-4 was thus not a suprise—in contrast to the discovery <strong>of</strong> <strong>superconductivity</strong>—but in many<br />

details the properties <strong>of</strong> He-4 were found to be different from the predicted Bose-Einstein condensate. The reason<br />

for this is that the interactions between helium atoms are actually quite strong. For completeness, we sketch the<br />

temperature-pressure phase diagram <strong>of</strong> He-4:<br />

9

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