All-to-all coupled quantum computing with atomic ensembles in an optical cavity
A quantum computer uses interactions between atomic ensembles mediated by an optical cavity mode to perform quantum computations and simulations. Using the cavity mode as a bus enables all-to-all coupling and execution of non-local gates between any pair of qubits. Encoding logical qubits as collective excitations in ensembles of atoms enhances the coupling to the cavity mode and reduces the experimental difficulty of initial trap loading. By using dark-state transfers via the cavity mode to enact gates between pairs of qubits, the gates become insensitive to the number of atoms within each collective excitation, making it possible to prepare an array of qubits through Poissonian loading without feedback.
1. A method of quantum information processing, the method comprising:
trapping an array of atom ensembles within a cavity;
coupling the array of atom ensembles to a resonant optical mode of the cavity; and
transferring, via the resonant optical mode of the cavity, quantum information between at least two atom ensembles in the array of atom ensembles without accessing Rydberg states of the at least two atom ensembles.
2. The method of claim 1 , further comprising:
performing a Rydberg gate between excitations within the at least two atom ensembles.
3. The method of claim 1 , further comprising, before coupling the array of atom ensembles to the resonant optical mode of the cavity:
initializing an atom ensemble in the array of atom ensembles in a Dicke state such that a matrix element representing a photon emission by the atom ensemble into the resonant optical mode is collectively enhanced.
4. The method of claim 3 , wherein initializing the atom ensemble in the Dicke state comprises using a Rydberg blockade.
5. The method of claim 1 , wherein transferring the quantum information is from two atom ensembles in the array of atom ensembles to a third atom ensemble in the array of atom ensembles.
6. The method of claim 5 , further comprising:
performing a local Rydberg gate on the quantum information transferred to the third atom ensemble.
7. The method of claim 1 , wherein transferring the quantum information is from a first pair of atom ensembles in the array of atom ensembles to a second pair of atom ensembles in the array of atom ensembles, and further comprising:
performing a local Rydberg gate on the quantum information transferred to the second pair of atom ensembles.
8. The method of claim 1 , wherein transferring the quantum information comprises performing a dark-state transfer of the quantum information from a first atom ensemble in the array of atom ensembles to a second atom ensemble in the array of atom ensembles via the resonant optical mode of the cavity.
9. The method of claim 8 , wherein performing the dark-state transfer comprises:
causing the first atom ensemble to emit a photon into the resonant optical mode of the cavity; and
causing the second atom ensemble to absorb the photon.
10. The method of claim 9 , wherein the photon encodes a quantum state of the first atom ensemble.
11. The method of claim 8 , wherein the dark-state transfer is a first dark-state transfer, the second atom ensemble has at least two internal energy states, and further comprising:
performing a second dark-state transfer of quantum information from a third atom ensemble in the array of atom ensembles to the second atom ensemble via the resonant optical mode of the cavity.
12. The method of claim 11 , wherein the first dark-state transfer and the second dark-state transfer occur simultaneously.
13. The method of claim 1 , wherein the at least two atom ensembles in the array of atom ensembles comprise a first atom ensemble and a second atom ensemble separated in the array of atom ensembles by at least one other atom ensemble.
14. The method of claim 1 , further comprising:
encoding quantum information, by the array of atom ensembles, using a W state.
15. The method of claim 14 , further comprising:
creating the W state using a Rydberg blockade.
16. A system comprising:
a cavity;
a first laser, optically coupled to the cavity, to trap an array of atom ensembles within the cavity; and
a second laser, in optical communication with the array of atom ensembles, to illuminate a first atom ensemble in the array of atom ensembles with a laser pulse, the laser pulse causing the first atom ensemble to transfer quantum information to a second atom ensemble in the array of atom ensembles via a photon coupled into a resonant optical mode of the cavity without accessing Ryberg states of the first atom ensemble or the second atom ensemble.
17. The system of claim 16 , wherein the first laser is configured to generate a standing-wave optical lattice in the cavity with different atom ensembles in the array of atom ensembles trapped in respective lattice sites of the standing-wave optical lattice.
18. The system of claim 16 , further comprising:
a beam-scanning element, in optical communication with the array of atom ensembles and the second laser, to direct the laser pulse emitted by the second laser to the first atom ensemble.