Bounds for the Superfluid Fraction from Exact Quantum Monte Carlo Local Densities
arXiv:0707.4094 · doi:10.1103/PhysRevB.76.052503
Abstract
For solid 4He and solid p-H2, using the flow-energy-minimizing one-body phase function and exact T=0 K Monte Carlo calculations of the local density, we have calculated the phase function, the velocity profile and upper bounds for the superfluid fraction f_s. At the melting pressure for solid 4He we find that f_s < 0.20-0.21, about ten times what is observed. This strongly indicates that the theory for the calculation of these upper bounds needs substantial improvements.
arXiv commentto be published in Phys. Rev. B (Brief Reports)
References in corpus (9)
- Quantum phase transition from a superfluid to a Mott insulator in a gas of ultracold atoms
- On the Supersolid State of Matter
- Ring exchanges and the supersolid phase of 4He
- The fate of vacancy-induced supersolidity in 4He
- Bose Einstein Condensation of incommensurate solid 4He
- Bose Einstein Condensation in solid 4He
- Search for Superfluidity in Solid Hydrogen
- Superflow in Solid 4He
- Supersolid He Likely Has Nearly Isotropic Superflow
Cited by in corpus (8)
- Solid 4He and the Supersolid Phase: from Theoretical Speculation to the Discovery of a New State of Matter? A Review of the Past and Present Status of Research
- Path integral Monte Carlo ground state approach: Formalism, implementation, and applications
- Leggett's bound for amorphous solids
- Quantum crystallography of Rydberg-dressed Bose gases on a square lattice
- Andreev-Lifshitz Supersolid Hydrodynamics Including the Diffusive Mode
- Generation Efficiencies for Propagating Modes in a Supersolid
- Dynamics of Supersolid state: normal fluid, superfluid, and supersolid velocities
- Impurity-controlled vortex mobility and pair-breaking in fermionic superfluid rings