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Experimental one-way quantum computing

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Title: Experimental one-way quantum computing


1
Experimental one-way quantum computing
Student presentation by Andreas Reinhard
2
Outline
  1. Introduction
  2. Theory about OWQC
  3. Experimental realization
  4. Outlook

3
Introduction
  • Standard model
  • Computation is an unitary (reversible) evolution
    on the input qubits
  • Balance between closed system and accessibility
    of qubitsgt decoherence, errors
  • Scalability is a problem

4
Introduction
  • A One-Way Quantum Computer1
  • proposed for a lattice with Ising-type
    next-neighbour interaction
  • Hope that OWQM is more easlily scalable
  • Error threshold between 0.11 and 1.4 depending
    on the source of the error2 (depolarizing,
    preparation, gate, storage and measurement
    errors)
  • Start computation from initial "cluster" state of
    a large number of engangled qubits
  • Processing measurements on qubits gt one-way,
    irreversible

1R. Raussendorf, H. J. Briegel, A One-Way Quantum
Computer, PhysRevLett.86.5188, 2001 2R.
Raussendorf, et al., A fault-tolerant one-way
quantum computer, ph/050135v1, 2005
5
Cluster states
  • Start from highly entangled configuration of
    "physical" qubits.Information is encoded in the
    structure "encoded" qubits
  • quantum processing measurements on physical
    qubits
  • Measure "result" in output qubits
  • How to entangle the qubits?

6
Entanglement of qubits with CPhase operations
  • Computational basis
  • Notation
  • Prepare "physical" 2-qubit state (not entangled)
  • CPhase operation gthighly entangled state


7
Cluster states
  • Prepare the 4-qubit state
  • and connect "neighbouring" qubits with CPhase
    operations.The final state is highly entangled
  • Nearest neighbour interaction sufficient for full
    entanglement!

Cluster state
8
Operations on qubits
  • Prepare cluster state
  • We can measure the state of qubit j in an
    arbitrarily chosen basis
  • Consecutive measurements on qubits 1, 2, 3
    disentangle the state and completely determine
    the state of qubit 4.
  • The state of "output" qubit 4 isdependent on the
    choses bases.
  • Thats the way a OWQC works!

9
A Rotation
  • Disentangle qubit 1 from qubits 2, 3, 4
  • and project the state on gt
    post selection

Single qubit rotation
10
SU(2) rotation gates
  • A general SU(2) rotation and 2-qubit gates
  • CPhase operations single qubit rotations
    universal quantum computer!

11
A one-way Quantum Computer
  • Initial cluster structure ltgt algorithm
  • The computation is performed with consecutive
    measurements in the proper bases on the physical
    qubits.
  • Classical feedforward makesa OWQC deterministic

Clusters are subunits of larger clusters.
12
Experimental realization1
  • A OWQC using 4 entangled photons
  • Polarization states of photons physical qubits
  • Measurements easily performable. Difficulty
    Preperation of the cluster state

1P. Walther, et al, Experimental one-way quantum
computing, Nature, 434, 169 (2005)
13
Experimental setup
  • Parametric down-conversion with a nonlinear
    crystal
  • PBS transmits H photons and reflects V photons
  • 4-photon events
  • gt Highly entangled state
  • Entanglement achieved through post-selection
  • Equivalent to proposed cluster state under
    unitary transformations on single qubits

14
State tomography
  • Prove successful generation of cluster state gt
    density matrix
  • Measure expectation valuesin order to
    determine all elements
  • Fidelity

15
Realization of a rotationand a 2-qubit gate
  • Output characterized by state tomography
  • Rotation
  • 2-qubit CPhase gate

16
Problems of this experiment
  • Noise due to imperfect phase stability in the
    setup (and other reasons). gt low fidelity
  • Scalability probability of n-photon coincidence
    decreases exponentially with n
  • No feedforward
  • No storage
  • Post selection
  • gt proof of principle experiment

17
Outlook
  • 3D optical lattices with Ising-type interacting
    atoms
  • Realization of cluster states on demand with a
    large number of qubits
  • Cluster states of Rb-atoms realized in an optical
    lattice1
  • Filling factor a problem
  • Single qubit measurements not realized
    (adressability)

1O. Mandel, I. Bloch, et al., Controlled
collisions for multi-particle entanglement of
optically trapped atoms, Nature 425, 937 (2003)
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