Abstract

We find the pressure, due to the thermal excitations of superfluid helium, at the interface with a solid. The separate contributions of phonons, R−R^- rotons and R+R^+ rotons are derived. The pressure due to R−R^- rotons is shown to be negative and partially compensates the positive contribution of R+R^+ rotons, so the total roton pressure is positive but several times less than the separate R−R^- and R+R^+ roton contributions. The pressure of the quasiparticle gas is shown to account for the fountain effect in HeIIHeI I. An experiment is proposed to observe the negative pressure due to R−R^- rotons.

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