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Quantum information processing

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Title: Quantum information processing


1
Quantum information processing
  • Myungshik Kim
  • Queens University, Belfast

2
What is quantum information processing?
  • A research in quantum information processing is
    to understand how quantum mechanics can improve
    acquisition, transmission and processing of
    information.
  • Review article Bennett DiVincenzo, Nature 404,
    247 (2000)
  • Who may be involved?
  • Computer scientists What are difficult problems
    ?
  • Mathematicians Coding and information theory
  • Electrical engineers electronic quant info
    processor
  • Chemists Chemical quantum devices
  • Physicists Developer of quantum theory

3
Quantum coherence
PBS
  • Example 1
  • By focusing a ?/2 pulse on a two level atom
  • Example 2
  • Schroedinger cat states
  • ? denotes the amplitude of a coherent state
  • By nonlinear Kerr interaction


Kerr medium
4
Why quantum coherence?
  • Consider the density operator
  • Recall Youngs double slit interference
  • Allows massive parallelism in quantum computation

Classical
Quantum
5
What is entanglement ?
  • Two important ingredients
  • Random
  • Deterministic

Type II nonlinear crystal
Energy momentum conservation
One photon is ? polarised the other ? polarised
? polarised
? or ?
? or ?
? polarised
HongMandel, PRL 59, 2044 (1987) Kwiat et al.,
PRL 75, 4337 (1995)
6
  • There are four basis states
  • They are so called the Bell states
  • Braunstein et al. PRL 68, 3259 (1992)
  • States maximally violating Bells inequality

Bell
7
  • How about
    ?
  • Is it entangled? Yes, as far as a?0 b?1.
  • How do we define a degree of entanglement?
  • For a pure state, the von Neumann entropy is a
    useful tool.
  • Find ? for two particles
  • Find the reduced density operator for one
    particle
  • Substitute ?1 into the definition of the von
    Neumann entropy to find out the degree of
    entanglement
  • S -Tr ?1 ln
    ?1.

8
How to manufacture an arbitrary entangled state?
  • White Kwiat (PRL 83, 3103 (1999))
  • a) Twin photons are emitted
  • at two identical down-conversion
  • crystals. The crystals are oriented
  • so that the optic axis of the first
  • (second) lies in the vertical
  • (horizontal) plane
  • b) Adjustable quarter- half-wave
  • plates and polarising beam splitters
  • allow polarisation analysis
  • in any basis.

9
  • Experimentally reconstructed
  • density matrices of states that are
  • a)
  • b)
  • c)

10
  • Is a mixed state always classical?
  • Eh? What is a mixed state?
  • Why mixed states? As soon as a quantum state is
    embedded in an environment, the pure state
    becomes mixed.

11
A mixed state is not always classical.
  • Consider
  • For ab1/?2 the density operator describes a
    pure state and for b0 a classical mixture.
  • There should be some critical point when the
    system loses quantum nature (entanglement).
  • We need to define a measure of entanglement for a
    mixed state.

12
Multi-particle entanglement BouwmeesterZeiling
er, PRL 82, 1345 (1999)
  • Three-particle entanglement
  • so called GHZ(Greenberger-Horne-Zeilinger) state
  • Generation
  • Use type II interaction
  • Two pairs are generated
  • GHZ for four simultaneous clicks
  • How do we define a degree
  • of entanglement? Any use?
  • Sackett Wineland,
  • Experimental entanglement of four paritcles,
  • Nature 404, 256 (2000)

13
Higher-dimensional entanglement
  • Quantum information processing for qubits.
  • Quantum effects for a d-dimensional system
    qudits
  • Most quantum systems require the use of an
    infinite dimensional vector space.
  • Possibility to test experimentally.
  • Laser
  • Provide a test ground for paradoxes in quantum
    mechanics.
  • Photonic state Defined in phase space-continuous
    variables
  • Braunstein error correction for continuous
    quantum variables, PRL 80, 4084 (1998)
  • Braunstein, quantum error correction for
    communication with linear optics, Nature 394, 47
    (1998)
  • BraunsteinLloyd, quantum computation over
    continuous variables, PRL 82, 1784 (1999)
  • BotoBraunstein, quantum interferometric optical
    lithography, PRL 85, 2733 (2000)
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