On the observability of Pauli crystals
arXiv:1707.09860 · doi:10.1038/s41598-017-14952-2
Abstract
The best known manifestation of the Fermi-Dirac statistics is the Pauli exclusion principle: no two identical fermions can occupy the same one-particle state. This principle enforces high order correlations in systems of many identical fermions and is responsible for a particular geometric arrangement of trapped particles even when all mutual interactions are absent [1]. These geometric structures, called Pauli crystals, are predicted for a system of identical atoms trapped in a harmonic potential. They emerge as the most frequent configurations in a collection of single-shot pictures of the system. Here we study how fragile Pauli crystals are when realistic experimental limitations are taken into account. The influence of the number of single-shots pictures available to analysis, thermal fluctuations and finite efficiency of detection are considered. The role of these sources of noise on the possibility of experimental observation of Pauli crystals is shown and conditions necessary for the detection of the geometrical arrangements of particles are identified.
arXiv comment11 pages, 6 figures
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Cited by in corpus (10)
- Observation of Pauli Crystals
- Counting statistics for non-interacting fermions in a rotating trap
- Universal tetramer and pentamer in two-dimensional fermionic mixtures
- Continuous simultaneous measurement of position and momentum of a particle
- Pauli crystal melting in shaken optical traps
- Statistical interaction description of Pauli crystals in two-dimensional systems of harmonically confined fermions
- Pauli crystals -- interplay of symmetries
- Pauli crystal superradiance
- Optimized Observable Readout from Single-shot Images of Ultracold Atoms via Machine Learning
- Optimal configurations and "Pauli crystals" of quantum clusters