Method and apparatus for fault-tolerant quantum communication based on solid-state photon emitters

• US 8,913,900 B2
• Filed: 10/11/2006
• Issued: 12/16/2014
• Est. Priority Date: 10/11/2005
• Status: Active Grant

• Current Assignee: President and Fellows of Harvard College (Harvard Corporation)
• Original Assignee: President and Fellows of Harvard College (Harvard Corporation)
• Inventors: Lukin, Mikhail, Taylor, Jacob M., Childress, Lilian I., Sorensen, Anders S.
• Primary Examiner(s): Li, Shi K
• Application Number:
  US12/090,020
• Publication Number:
  US 20110222848A1
• Time in Patent Office: 2,988 Days
• Field of Search: 398/173, 398/180
• US Class Current: 398/176
• CPC Class Codes: H04B 10/70 Photonic quantum communication
• CPC Class Codes: H04B 10/90 Non-optical transmission systems, e.g. transmission systems employing non-photonic corpuscular radiation

Abstract

A novel method and apparatus for long distance quantum communication in realistic, lossy photonic channels is disclosed. The method uses single emitters of light as intermediate nodes in the channel. One electronic spin and one nuclear spin coupled via the contact hyperfine interaction in each emitter, provide quantum memory and enable active error purification. It is shown that the fixed, minimal physical resources associated with these two degrees of freedom suffice to correct arbitrary errors, making our protocol robust to all realistic sources of decoherence. The method is particularly well suited for implementation using recently-developed solid-state nano-photonic devices.

Claims

1. A method for producing entangled pairs of quantum bits (“

qubits”

) at long distances, using physical systems with two qubits per system, wherein each physical system is at a different location, comprising the steps of;

generating short distance entangled pairs based on state-selective elastic light scattering;

generating an entanglement connection, wherein said step of generating an entanglement connection comprises a technique for taking two entangled pairs at short distance, and by local operations on one element of each pair, obtaining to a single entangled pair at a longer distance, and

performing entanglement purification to improve entanglement of said single entangled pair, wherein said entanglement purification purifies both bit errors and phase errors using only two qubits at each physical location and an additional unused non-local qubit at a distant physical location.

2. A method for producing entangled pairs of quantum bits according to claim 1, further comprising the step of performing entanglement purification to improve the entanglement of a longer distance pair.

3. A method for producing entangled pairs of quantum bits according to claim 2, wherein said step of performing entanglement purification uses un-used, non-local qubits to improve the entanglement of a final pair.

4. A system for generating entanglement between two solid-state single photon emitters comprising:

a coherent light source;

a plurality of nodes, each node comprising a single photon emitter with several levels, each with different probabilities for coherent scattering of the light source via state-selective elastic light scattering; and

means for generating entanglement between optically-active qubits in a first node and a second node by interference of the scattered light at a beam splitter.

5. A system according to claim 4 further comprising a photonic cavity resonant with the coherent light source but not the solid state emitter.

6. A method of quantum communication in a system comprising a plurality of nodes, comprising the steps of:

generating entanglement between optically-active qubits in a first node and a second node adjacent said first node;

mapping an optically-active qubit onto a memory qubit;

leaving an optically-active qubit available to generate entanglement between unconnected nodes;

projectively measuring from a third node adjacent said second node four Bell states in a manifold involving both the optically-active qubit and the memory qubit associated with an emitter at said second node; and

using the outcomes of the measurements of the four Bell states to obtain a singlet state in a remaining pair of memory qubits and implementing a deterministic entanglement swap to produce a memory qubit entanglement between said second and third nodes approximately mirroring said optically-active qubit entanglement between said first and second nodes.