Methods for preparing entangled quantum states
View Patent ↗Various embodiments of the present invention are directed to methods for generating an entangled state of qubits. In one embodiment of the present invention, a method for preparing an entangled state of qubits comprises providing a probe and N non-interacting qubits, each qubit comprises a linear superposition of two basis states. The probe is transmitted into an interaction region that separately couples the probe to each of the qubits and produces a number of different probes. A linear superposition of states is output from the interaction region, each state in the linear superposition of states comprises a tensor product of entangled basis states and one of the different probes. The linear superposition of states is projected into one of the entangled states by measuring the state of the probe.
1. A method for preparing an entangled state of qubits, the method comprising:
providing a probe and N non-interacting qubits, each qubit comprises a linear superposition of two basis states;
transmitting the probe into an interaction region that separately couples the probe to each of the qubits and produces a number of different probe states;
outputting from the interaction region a linear superposition of states, each state in the linear superposition of states is an entangled state of tensor product basis states and one of the different probe states; and
projecting the linear superposition of states into one of the entangled states by measuring the state of the probe.
2. The method of claim l wherein the probe is a coherent state and the N non-interacting qubits further comprises one or more of:
matter-based qubits;
photon-based qubits;
a linear superpositions of two quantum dot states; and
a linear superposition of two magnetic states.
3. The method of claim 1 wherein the detector is a photon number detector.
4. The method of claim 1 wherein the detector is an X quadrature homodyne detector.
5. The method of claim 1 wherein the interaction region further comprises one or more dipole coupling mediums, each medium characterized by an interaction Hamiltonian:
Ĥ= χâ † â{circumflex over (σ)} z
where χ is a constant that represents the coupling strength between the probe and basis states of the qubit,
â † â is a number operator that operates on the probe, and
6. The method of claim 1 wherein the interaction region further comprises one or more cross-Kerr interaction mediums, each medium characterized by a cross-Kerr interaction Hamiltonian:
Ĥ= χâ † â{circumflex over (b)} † {circumflex over (b)}
where χ is a constant that represents the coupling strength between the probe and basis states of the qubit,
â † â is a number operator that operates on the probe, and
{circumflex over (b)} † {circumflex over (b)} is a number operator that operates on a photon basis state.
7. The method of claim 1 wherein the interaction region further comprises one or more interaction mediums, each medium characterized by an interaction Hamiltonian:
Ĥ= χ{circumflex over (σ)} z ( â † e iφ +âe − φ )
where χ is a constant that represents the coupling strength between the probe and basis states of the qubit,
and
â † e iφ +âe −iφ is a quadrature operator of the probe and is determined by the angle φ.
8. The method of claim 1 , wherein the method further comprises a correction operation that removes phase shifts acquired by the entangled states.
9. A method for preparing an entangled state of qubits, the method comprising:
providing a probe and N non-interacting qubits, each qubit comprises a linear superposition of two basis states;
transmitting the probe into an interaction region that separately couples the probe to each of the qubits and produces a number of different phase-shifted probe states;
outputting from the interaction region a linear superposition of states, each state in the linear superposition of states is an entangled state of tensor product basis states and one of the phase-shifted probe states; and
transmitting the phase-shifted probe state to a homodyne detector that projects the linear superposition of states into one of the entangled states by measuring the state of the coherent state.
10. The method of claim 9 , wherein the probe is a coherent state and the N non-interacting qubits further comprises one or more of:
matter-based qubits;
photon-based qubits;
a linear superpositions of two quantum dot states; and
a linear superposition of spin magnetic moments.
11. The method of claim 9 , wherein the detector is an X quadrature homodyne detector.
12. The method of claim 9 , wherein the interaction region further comprises dipole coupling mediums, each medium characterized by an interaction Hamiltonian:
Ĥ= χâ † â{circumflex over (σ)} z
where â † â is a number operator that operates on the probe,
χ is a constant that represents the coupling strength between the probe and basis states of the qubit, and
13. The method of claim 9 , wherein the interaction region further comprises cross-Kerr interaction mediums, each medium characterized by a cross-Kerr Hamiltonian:
Ĥ= χâ † â{circumflex over (b)} † {circumflex over (b)}
where χ is a constant that represents the coupling strength between the probe and basis states of the qubit,
â † â is a number operator that operates on the probe, and
{circumflex over (b)} † {circumflex over (b)} is a number operator that operates on a photon basis state.
14. The method of claim 13 , wherein the interaction region further comprises applying a quadrature rotation operation to the probe output from the interaction region.
15. The method of claim 9 , wherein the method further comprises a correction operation that removes phase shifts acquired by the entangled states.
16. A method for preparing an entangled state of qubits, the method comprising:
providing a probe and N non-interacting qubits, each qubit comprises a linear superposition of two basis states;
transmitting the probe into an interaction region that separately couples the probe to each of the qubits and produces a number of different translated coherent states;
outputting from the interaction region a linear superposition of states, each state in the linear superposition of states is an entangled state of tensor product basis states and one of the translated probe states; and
transmitting the displaced probe state to a photon number detector that projects the linear superposition of states into one of the entangled states by measuring the state of the coherent state.
17. The method of claim 16 wherein the probe is a coherent state and the N non-interacting qubits further comprise one or more of:
matter-based qubits;
a linear superpositions of two quantum dot states; and
a linear superposition of spin magnetic moments.
18. The method of claim 16 wherein the detector is a photon number detector.
19. The method of claim 16 wherein the interaction region further comprises one or more interaction mediums, each medium characterized by an interaction Hamiltonian:
Ĥ= χ{circumflex over (σ)} z ( â † e iφ +âe − φ )
where χ is a constant that represents the coupling strength between the probe and basis states of the qubit,
and
â † e iφ +âe −iφ is a quadrature operator of the probe and is determined by the angle φ.
20. The method of claim 19 , wherein the interaction region further comprises applying a probe displacement operation to the probe output from the interaction region.
21. The method of claim 16 , wherein the method further comprises a correction operation that removes phase shifts acquired by the entangled states.