Criterion for Bose-Einstein condensation in traps and self-bound systems
arXiv:0804.1672 · doi:10.1103/PhysRevA.78.035603
Abstract
The internal one-particle density matrix is discussed for Bose-Einstein condensates with finite number of particles in a harmonic trap. The outcome of the digonalization of the density matrix depends on the choice of the internal coordinates: The Pethick-Pitaevskii-type internal density matrix, whose analytical eigenvalues and eigenfunctions are evaluated, yields a fragmented condensate, while the Jacobi-type internal density matrix leads to an ideal condensate. We give a criterion for the choice of the internal coordinates: In the macroscopic limit the internal density matrix should have eigenvalues and eigenfunctions of an ideal Bose-Einstein condensate, this being a very physical condition for cases where the system is also an ideal Bose condensation in the laboratory frame. One choice fulfilling this boundary condition is given by the internal Jacobi coordinates, while the internal coordinates with respect to the center of mass do not satisfy the condition. Based on our criterion, a general definition of the internal one-particle density matrix is presented in a self-bound system, consisting of interacting bosons.
Shortened to Brief report
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- Nonlocalized Clustering and Evolution of Cluster Structure in Nuclei
- Nuclear Alpha-Particle Condensates
- Trapped two-component Fermi gases with up to six particles: Energetics, structural properties, and molecular condensate fraction
- Internal One-Particle Density Matrix for Bose-Einstein Condensates with Finite Number of Particles in a Harmonic Potential
- Repulsive Four-Body Interactions of Particles and Quasi-Stable Nuclear -Particle Condensates in Heavy Self-Conjugate Nuclei
- Relative and center-of-mass motion in the attractive Bose-Hubbard model
- Alpha-Particle Condensation in Nuclear Systems