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When ∆E p < 0, it represents the W state.
The method can be generalized to prepare W state among any number of atomic ensembles.
Region III implies that the free energy of the CB state is greater than the W state, which demonstrates that the W state is stable.
When ΔE h < 0, it implies that the W state is more stable.
On the contrary, the W state is more stable for shallow and thick nanoholes.
We propose a way to prepare W state among atomic ensembles via stimulated Raman adiabatic passage (STIRAP) technique.
Fig. 2 Schematic illustrations of wetting states of a droplet on a nanohole-patterned surface with the W state (a) and the CB state (b) and on a nanopillar-patterned surface with the W state (c) and the CB state (d).
The W state is more stable while the pillar height and radii are smaller than the critical values.
We propose a scheme for generating a two-atom entangled state and an N-atom W state using adiabatic evolution of dark eigenstates in cavity QED.
Generally, for a system of a droplet placed on a nanopatterned surface, the final state is either the W state or the CB state.
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