Superfluid states in Fermi–Dirac systems 173
Temperature (mK)
Pressure
(b
ar
)
Normal liquid
0
0
10
20
30
40
123
Superfluiduperflui
B-phaseB-phase
Solid
A
Fig. 15.2Thephasediagram of^3 Heatmillikelvin temperatures, andin zero appliedmagneticfield.The
A-andB-phases aredifferent superfluidphases.
3 .Inthe A-phase, these vectors correspondtoaspin(S)direction andan orbital
(L)direction, sharedbyallpairsin a particular region ofthefluid. Hence the
A-phase has many similarities with liquid crystals, which also order with a highly
anisotropic vector orderingparameter. (Themagnitudeoftheorder parameter
gives the strength of the ordering; the direction of the vectorgives the direction
of alignment of the liquid crystal molecules.)
- In the B-phase, theS=1,L= 1 pairs collect togetherin a muchmore uniform
way, and the anisotropyis practicallynon-existent (although it can have secondary
manifestations). Many experimental properties of the B-phase are described sim-
ply in terms ofasingle scalarparameter. Figure 15.3gives an example of this
type of behaviour, and it also serves as a dramatic illustration of the existence of
superfluidity.As noted above in section 14.2.2,^3 Heisahighlyviscousliquidabove
TTTC,so that thedampingofavibratingwireis verylarge. When theliquid is cooled
belowTTTC, however, the damping falls off rapidly, varying as exp(−/kkkBT),the
usualBoltzmannfactor, atlow temperatures as the normalfluid isfrozen out. At
thelowest temperatures thevibratorbehaves asif in a vacuum withadamping
coefficient 100 000 times less than atTTTC. - The fact that the pairs haveS= 1 means that they are magnetic. Thebehaviour
ofthe superfluid isthus profoundly influencedbyappliedmagneticfields. This
is so even in the B-phase, which becomes unstable if a large enough field (of
order 0.4T)is applied,the superfluidreverting to the more magneticA-phase. The
wholephasediagram changes, whichiswhytheB= 0 qualification was needed