Application of fourth sound to study the superfluid helium-4 and the recently discovered superfluid helium-3
H. Kojima
Abstract
H. Kojima
Abstract
Fourth sound is propagated in a superfluid placed in the tiny pores of tightly packed fine powder. Since it is a type of usual sound (pressure-density) propagation, fourth sound may be excited and detected by condenser transducers. In superfluid helium-4 fourth sound has been used (1) to determine the superfluid component density by measuring the sound velocity, and (2) to study the nature of persistent currents using Doppler-shifted fourth sound. In superfluid helium-3 propagation of fourth sound provided conclusive evidence of superfluidity of liquid helium below 2.6 mK. Superfluid component density and some anisotropic properties of superfluid helium-3 have been investigated using fourth sound.
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Fourth sound is propagated in a superfluid placed in the tiny pores of tightly packed fine powder. Since it is a type of usual sound (pressure-density) propagation, fourth sound may be excited and detected by condenser transducers. In superfluid helium-4 fourth sound has been used (1) to determine the superfluid component density by measuring the sound velocity, and (2) to study the nature of persistent currents using Doppler-shifted fourth sound. In superfluid helium-3 propagation of fourth sound provided conclusive evidence of superfluidity of liquid helium below 2.6 mK. Superfluid component density and some anisotropic properties of superfluid helium-3 have been investigated using fourth sound.
Key concepts: Superfluidity, Second sound, Superfluid helium-4, Roton, Sound (geography), Superfluid film, Physics, Helium