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Incoming links: Rydberg blockade
The five DiVincenzo criteria are: a scalable collection of well-characterized qubits; preparation in a known fiducial quantum state; relevant coherence times long compared with quantum gate times; a universal quantum gate set; and qubit-specific quantum measurement. The criterion is useful control of the whole computation, including errors, rather than merely observing two resolved levels.[ref]
The Physical Implementation of Quantum Computation by David P. DiVincenzo. Section III, numbered requirements 1–5; Section IV's two communication requirements are additional
For trapped ions, the implementation is:
- Scalable characterized qubits. Two long-lived hyperfine structure levels or an optical ground/metastable pair in each ion encode . An ion trap confines individually addressed ions. Extending a chain adds qubits, but increasing motional complexity, addressing errors and heating limit straightforward scaling; segmented traps and transport can help.
- Initialization. Optical pumping prepares the internal quantum state. Doppler cooling and, where required, resolved sideband cooling prepare the shared motion used for quantum gates.
- Coherence. Long-lived internal levels give coherence much longer than controlled pulse times. Magnetic noise, laser noise, scattering and motional heating cause quantum decoherence; suitable clock-state encodings and control reduce these errors.
- Universal control. Resonant optical, microwave or Raman transitions give arbitrary one-qubit rotations. Shared motional normal modes, coupled through the Coulomb force, mediate entangling two-qubit gates. Together these supply a universal quantum gate set.
- Readout. State-selective cycling fluorescence, often with electron shelving, produces a bright/dark signal resolved for individual ions.
For trapped neutral atoms, the corresponding implementation is:
- Scalable characterized qubits. Long-lived ground-state hyperfine structure levels encode qubits in an optical lattice or an array of optical tweezers. Large arrays are feasible, but random loading, vacancies, atom loss and individual addressing must be controlled.
- Initialization. Cooling plus optical pumping prepares the internal quantum state. Filling or rearranging traps prepares a usable register; motional cooling is needed when the chosen quantum gate depends on motion.
- Coherence. Weak environmental coupling of neutral ground-state chemical atoms allows long coherence. Trap-light scattering, differential light shifts and magnetic noise limit it; switching traps or choosing suitable encodings can reduce these effects.
- Universal control. Microwave or Raman transitions implement one-qubit rotations. Ground-state chemical atoms do not have the ions' long-range Coulomb force, so that motional-bus construction cannot simply be copied. Controlled collisions or Rydberg blockade can nevertheless supply entangling two-qubit gates.
- Readout. State-dependent fluorescence or state-selective removal followed by imaging identifies a chosen qubit. Optical resolution, cross-talk and atom loss constrain repeated measurements.
Thus neither platform is forbidden from meeting a criterion in principle. Weak neutral-ground-state interactions make entangling control harder, but claiming that trapped neutral atoms cannot implement a universal quantum gate set would be false. Gate-model quantum algorithms using Rydberg blockade had already been demonstrated in a programmable neutral-atom processor by 2022.[ref]
Multi-qubit entanglement and algorithms on a neutral-atom quantum computer by T. M. Graham and others. Nature 604, 457–462 (2022), abstract and controlled-phase gate implementation
Rydberg atom Created 2026-10-18 Updated 2026-11-05
A Rydberg atom has an electron excited to a large principal quantum number . In a hydrogen-like model, the binding energy scales as and the orbital size as . The outer electron is therefore weakly bound and its motion extends far beyond the compact core.
These properties make Rydberg atoms sensitive to applied electric fields and useful for studying controllable interactions such as Rydberg blockade. A field ramp can ionize different excited states at different thresholds, enabling state-selective field ionization. Real multi-electron atoms depart from the simple hydrogen-like spectrum, especially when the outer electron penetrates the core.
Rydberg blockade 2026-10-24
Rydberg blockade suppresses simultaneous excitation of nearby chemical atoms into strongly interacting Rydberg atom states. If the interaction shifts the doubly excited level by much more than the excitation linewidth and coherent drive scale, a pulse resonant for one isolated chemical atom becomes off-resonant when a neighbour is already excited. The resulting conditional dynamics can implement an entangling two-qubit gate for neutral-atom qubits.
Stefan Scheel Created 2026-10-13 Updated 2026-11-05
A researcher in quantum optics whose joint work on Rydberg excitons connects highly excited atomic states with optical excitations in semiconductors. The 2014 study found evidence of Rydberg blockade: the presence of one large exciton suppresses the creation of another nearby.[ref]
Giant Rydberg Excitons in Cuprous Oxide by Tomasz Kazimierczuk and others. Abstract: dipole interactions and suppression of nearby excitation