Optical qubits http://focus.aps.org/ http://www.quantum.at/ http://www.qipirc.org/images/projects/image018.jpg.

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Presentation transcript:

Optical qubits http://focus.aps.org/ http://www.quantum.at/ http://www.qipirc.org/images/projects/image018.jpg

Outline Parametric down-conversion Single photon sources Linear-optical QC architectures

http://qist.lanl.gov/qcomp_map.shtml

Parametric down-conversion: source of entangled pairs of photons

Parametric down-conversion: typical setup

Parametric down-conversion: unusual setup Setup from Experimental Quantum Physics group at MPQ-Munchen

Single photons from atoms, atomic ensembles, artificial atoms and other photons Single photons are essential for optical quantum computing, quantum communication and cryptography Photons emitted by single atoms during spontaneous emission exhibit anti-bunching – only one photon can be emitted at a time, and it takes about the lifetime of the excited state to emit the next photon. Electromagnetically Induced Transparency can be used to make single photons from large, optically-thick atomic ensembles Artificial atoms, such as quantum dots, can also emit single photons PDC can be used as a “triggered” source of single photons: detecting a photon in the idler arm indicates that there is a single photon in the signal arm.

Atomic sources of single photons Cavity QED Cavity Laser Ultrafast laser excitation of atoms Pulse Spontaneous emission Laser pulse Lens Atom Photon

Atomic ensembles produce single photons “write” pulse creates a single photon detected by D1 and a collective excitation of atoms “read” pulse retrieves a single photon, measured by D2 and D3 demonstrated overall efficiency ~1.2% Alex Kuzmich and Dzmitry Matsukevich, GATech

Quantum dots and such... Can put them in a cavity... ... or excite them with ultrafast pulses and collect spontaneous emission. 1.3 micron photons from QDs (Toshiba/Cambridge)

PDC as a single photon source Detect a photon from the PDC process; that indicates presence of a single photon, the other half of the EPR pair.

Linear-optical QC architectures Knill - Laflamme – Milburn (KLM) proposal: - Conditional non-linear two-photon gates - Teleportation - Error correction Nonlinearity is the measurement; the gates are probabilistic, but heralded Need: - Single-photon source - Number-discriminating photon detectors - Feed-forward control and quantum memory (atoms!) Example: CNOT gate CNOT is performed if only one photon is detected; probability of success is 25%; scalability by teleporting the gates Control ancilla pair Input Output Target

Cluster state LOQC architecture Circuit model quantum computing: initialize, perform (conditional) gates, measure Cluster state quantum computing (Raussendorf and Briegel): prepare an entangled state, perform measurements. Cluster state can be efficiently (i.e. scalably) prepared using probabilistic entanglement; quantum memory is essential.

Four-qubit cluster state Weinfurter group, MPQ (2005)

Optical qubits: already practical! Single photons are already being used as quantum information carriers in quantum cryptosystems. MagiQ Technologies (USA) id Quantique (Switzerland)