Crystalline order in superfluid 3He films
arXiv:cond-mat/0601565 · doi:10.1103/PhysRevLett.98.045301
Abstract
We predict an inhomogeneous phase of superfluid 3He films in which translational symmetry is spontaneously broken in the plane of the film. This phase is energetically favored over a range of film thicknesses, $D_{c_2}(T)<D<D_{c_1}(T)$, separating distinct homogeneous superfluid phases. The instability at the critical film thickness, $D_{c_2}\approx 9 ξ(T)$, is a single-mode instability generating striped phase order in the film. Numerical calculations of the order parameter and free energy indicate a second-order instability to a periodic lattice of degenerate B-like phases separated by domain walls at $D_{c_1}\approx 12 ξ(T)$. The striped phase should be identifiable in transport and nuclear magnetic resonance experiments.
4 pages, 4 figures