Abstract
Experiments on films reveal an attractive Casimir-like force at the bulk point and in the superfluid regime. Previous work has explained the magnitude of this force at the transition and deep in the superfluid region but not the substantial attractive force immediately below the point. Utilizing a simple mean-field calculation renormalized by critical fluctuations we obtain an effective Casimir force that is qualitatively consistent with the scaling function obtained by collapse of experimental data.
- Received 24 January 2007
DOI:https://doi.org/10.1103/PhysRevE.76.030601
©2007 American Physical Society