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Is information processing a physical phenomenon

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How much information is needed to store the result for the toss of two coins ? ... 400 qubits = 10120 bits (holographic bound....Davies, 2006). The Feynman processor. ... – PowerPoint PPT presentation

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Title: Is information processing a physical phenomenon


1
Is information processing a physical phenomenon?
  • G.J. Milburn
  • The University of Queensland

2
The BITatom of information.
  • Transistor ON 1
  • Transistor OFF 0
  • Mutually exclusive alternatives.
  • One bit.
  • the information needed to store the result of a
    single coin toss.

C. Shannon
3
The BITatom of information.
  • How much information is needed to store the
    result for the toss of two coins ?
  • HH00, HT01, TH10, TT11
  • Four outcomes ----- two bits.

4
Paths to a quantum computer.
  • The beginning
  • R.P. Feynman, 1982
  • Simulating physics with computers,

5
Feynmans question.
  • Can a quantum system be simulated efficiently
    by a conventional computer ?
  • NO !

6
What is a quantum system ?
  • THE QUANTUM PRINCIPLE.
  • The physical universe is irreducibly random.
  • Given complete knowledge of the state of a
    physical system, there is at least one
    measurement the results of which are completely
    random.

7
How is quantum physics possible ?
  • CERTAINTY WITHIN UNCERTAINTY
  • Given complete knowledge of a physical state
    there is at least one measurement the results of
    which are completely certain.

8
How is quantum physics possible ?
  • We can compute the odds.
  • The probability of any measurement can be
    calculated.
  • Butto compute the odds we need a new
    mathematicsprobability amplitudes.
  • Not 0 or 1 but 0 and 1.the superposition
    principle.

9
A quantum coin toss.
  • A single photon at a beam splitter.
  • 50 of light is reflected or transmitted.

10
A one photon bit ?
Probability of reflection 1/2 Probability of
transmission1/2 Prob. Count photon at
U1/2 Prob. Count photon at D 1/2 Is this
a coin-toss ? Does this encode one bit?
11
A one photon bit ?
  • Toss a photon twice.

Is this like tossing a coin twice ?
12
A one photon bit? No.
  • Experiment
  • detection at U is certain.
  • Irreducible randomness is made certain !

13
The one photon qubit.
State of photon after beam splitter ? Not
reflected or transmitted. Not logical 1 or
0. It is a superposition of both
possibilities. It is a qubit.
14
Quantum parallel input.
  • superposition of binary strings.
  • Length 2

Two physical qubits can encode four binary
numbers simultaneously. The output is a
superpostion of all biary strings of length two.
15
Quantum parallel computation
N physical qubits can encode 2N binary numbers
simultaneously A quantum computer can process
all 2N numbers in parallel on a single machine
with N physical qubits. Very hard to simulate
a quantum computer on a classical computer.
400 qubits 10120 bits (holographic
bound.Davies, 2006).
16
The Feynman processor.
  • A physical computer operating by quantum rules.
  • could it compute more efficiently than a
    conventional computer ?

17
Computational efficiency.
  • Efficiency
  • How many steps are required to compute a function
    (how many operations per second)?
  • How does the number of steps depend on the size
    of the problem.

18
Computational efficiency example
  • Find the prime factors of
  • 2385269 (1001000110010101110101)
  • How ?divide by 2.no
  • Divide by 3.no
  • And so on until
  • Divide by 541yes... 2385269 541 x 4409
  • In general to factor integer X, need
    steps.
  • Add one digit to X, need about three times as
    many steps that is an exponential increase !

19
Deutsch and quantum parallelism.
  • D. Deutsch, Oxford, 1985
  • Quantum theory, the Church-Turing principle and
    the universal quantum computer.
  • Prepare input as a superposition of all possible
    inputs.
  • Run computer once to give all possible values of
    the calculation.

20
Quantum parallel input.
  • Superposition of all calculations in a single
    machine.

21
Shor algorithm.
  • Peter Shor, ATT, USA, 1993
  • a quantum algorithm to find prime factors of
    large composites N
  • public key cryptography no longer safe !
  • Key step
  • find the period of the function
  • (x is random, but GCD(x,N)1)

22
Example.
  • Factor 15.
  • Order4
  • Calculate
  • Factors GCD(48,15)3, GCD(50,15)5

23
Factoring on a QC
  • Finding the period is exponentially hard on a
    classical computer..or so we think!
  • A QC can find it in one run (most of the time).
  • Given the period, the rest is trivial for a
    classical computer.

24
The implications of efficient factoring.
  • Current public key encryption assumes there is no
    efficient algorithm for finding the prime factors
    with a conventional computer.
  • Shors algorithm is impossible in a classical
    world.
  • If a QC is built, current encryption protocols
    are insecure

25
Computation is a physical process.
  • Hardware determines the algorithm.
  • Computers are physical objects and computations
    are physical processes. What computers can and
    cannot do are determined by the laws of physics
    alone and not by pure mathematics. Deutsch.
  • computation is not a machine process..it is
    an abstract mathematical process that exists only
    relative to conscious observers.. Searle.

26
Synthetic reality
  • Feynman, 1982
  • Can physical reality be efficiently simulated ?
  • Feynman-Deutsch principle
  • Every finitely realisable physical system can
    be perfectly simulated by a universal (quantum)
    Turing machine operating by finite means.

27
Feynman-Deutsch principle and measurement.
  • The virtual graduate student part one.

28
Bohrs insight.
  • Quantum measurement theory
  • ...however far the phenomenon transcend the
    scope of classical physical explanation, the
    account of all evidence must be expressed in
    classical terms (Bohr, 1934)

29
Feynman-Deutsch principle and measurement.
  • The virtual graduate student part two.

30
Quantum measurement.
  • Feynman-Deutsch principle
  • (Measurement formulation)
  • The results of all finitely describable
    physical measurement systems can be perfectly
    simulated by a universal quantum computer
    operating by finite means, producing finite
    measurement records.

31
Simulate consciousness on a QC ?
  • Can we simulate Alice as well ?
  • We do not know the operating system of the brain.
  • Can we monitor the state of a QC from one step to
    the next ?
  • NO !

32
Conclusion.
  • Quantum computing machines enable new algorithms
    that cannot be realised in a classical world.
  • The algorithms can be powerful physical
    simulators.
  • The physics determines the algorithm.
  • The hardware matters...
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