A neutral-atom qubit architecture where long-lived hyperfine ground states encode (|0\rangle, |1\rangle), and entangling interactions are turned on transiently by laser excitation to high-lying Rydberg states. This is the core hardware model for modern optical-tweezer neutral-atom processors.
Physics
Single-qubit states are typically encoded in hyperfine “clock” states of alkali atoms (e.g., (^{87}\mathrm{Rb}), (^{133}\mathrm{Cs})).
Two-qubit entangling gates exploit the Rydberg blockade effect: if one atom is excited to a Rydberg state, nearby atoms are shifted out of resonance, suppressing simultaneous excitation and enabling conditional dynamics.
Hamiltonian
A standard driven Rydberg-array Hamiltonian (rotating frame) is:
where projects onto the Rydberg state, is the Rabi drive, detuning, and (van der Waals) or in resonant dipole regimes.
Blockade condition for two atoms :
suppresses double excitation , enabling controlled-phase entangling gates.
Figure

Why it matters
- Native all-to-all reconfigurability (via tweezer rearrangement) at array level.
- Strong, switchable interactions for fast entangling gates.
- A direct path from analog simulation to digital gate-based computing on the same hardware family.
Key Metrics
| Metric | Value | Notes | Fidelity reference |
|---|---|---|---|
| (qubit lifetime) | 1–10 s | Hyperfine clock states in optical traps; vacuum-limited | Evered et al. 2023 |
| (coherence) | 1–4 s | With spin-echo; limited by trap-induced dephasing | Evered et al. 2023 |
| 1Q gate fidelity | 99.5–99.90% | Global and local Raman gates | Evered et al. 2023 |
| 2Q gate fidelity (CZ) | 99.5% | Rydberg blockade CZ; SOTA with erasure conversion | Evered et al. 2023 |
| Gate time (2Q) | 200–500 ns | Rydberg pulse sequence | Evered et al. 2023 |
| Architecture scale | 100–1000+ physical atoms | Optical tweezer arrays; reconfigurable | henriet-2020-quantum-computing-with-neutral, wu-2020-a-concise-review-of |
| 2Q gate mechanism | Rydberg blockade | van der Waals interaction | jaksch-2000-rydberg-gate |
| Operating temperature | ~10–50 μK | Laser-cooled; in ultrahigh vacuum | Evered et al. 2023 |
| Fault-tolerant logical gate regime | Not yet established | Active experimental frontier | henriet-2020-quantum-computing-with-neutral |