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Quantum Parallelism and the Exact Simulation of Physical Systems

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Title: Quantum Parallelism and the Exact Simulation of Physical Systems


1
Quantum Parallelism and the Exact Simulation of
Physical Systems
  • Dan Cristian Marinescu
  • School of Computer Science
  • University of Central Florida
  • Orlando, Florida 32816, USA

2
Frontier(s)from Websters unabridged dictionary.
  • The part of a settled or civilized country
    nearest to an unsettled or uncivilized region.
  • Any new or incompletely investigated field of
    learning or thought.

3
What is a Quantum computer?
  • A device that harnesses quantum physical
    phenomena such as entanglement and superposition.
  • The laws of quantum mechanics differ radically
    from the laws of classical physics.
  • The unit of information, the qubit can exist as
    a 0, or 1, or, simultaneously, as both 0 and 1.

4
Does quantum computing represent the frontiers
of computing?
  • Is it for real? Can we actually build quantum
    computers? - Very likely, but it will take
    some time.
  • If so, what would a quantum computer allow us to
    do that is either unfeasible or impractical with
    todays most advanced systems? Exact
    simulation of physical systems, among other
    things.
  • Once we have quantum computers do we need new
    algorithms? Yes, we need quantum
    algorithms.
  • Is it so different from our current thinking that
    it requires a substantial change in the way we
    educate our students? Yes, it does.

5
Quantum computers now and then
  • All we have at this time is a 7 (seven) qubit
    quantum computer able to compute the prime
    factors of a small integer, 15.
  • To break a code with a key size of 1024 bits
    requires more than 3,000 qubits and 108 quantum
    gates.

6
Approximate computer simulation of physical
systems
  • Eniac and the Manhattan project. The first
    programs to run, simulation of physical
    processes.
  • Computer simulation new approach to scientific
    discovery, complementing the two well established
    methods of science experiment and theory.
  • Approximate simulation based upon a model that
    abstracts some properties of interest of a
    physical system.

7
Exact simulation of physical systems
  • How far do we want to go at the microscopic
    level? Molecular, atomic, quantum? - All of the
    above.
  • What about cosmic level? - Yes, of course.
  • Is it important? - - Yes (Feynman,
    1981) .
  • Who will benefit?
  • Natural sciences ? physics, chemistry, biology,
    astrophysics, cosmology,.
  • Application ? nanotechnology, smart materials,
    drug design,

8
Large problem state space
  • From black hole thermodynamics a system
    enclosed by a surface with area A has a number of
    observable states
  • c 3 x1010 cm/sec
  • h 1.054 x 10-34 Joules/second
  • G 6.672 x 10-8 cm3 g-1 sec-2
  • For an object with a radius of 1 Km ? N(A)
    e80

9
Acknowledgments
  • Some of the material presented is from the book
  • Approaching Quantum Computing
  • by Dan C. Marinescu and Gabriela M. Marinescu
  • to be published by Prentice Hall in June 2004
  • Work supported by National Science Foundation
    grants MCB9527131, DBI0296107,ACI0296035, and
    EIA0296179.

10
Contents
  • Computing and the Laws of Physics
  • Quantum Mechanics Computers
  • Qubits and Quantum Gates
  • Quantum Parallelism
  • Deutschs Algorithm
  • Virus Structure Determination and Drug Design
  • Summary

11
The limits of solid-state technologies
  • For the past two decades we have enjoyed Gordon
    Moores law. But all good things may come to an
    end
  • We are limited in our ability to increase
  • the density and
  • the speed of a computing engine.
  • Reliability will also be affected
  • to increase the speed we need increasingly
    smaller circuits (light needs 1 ns to travel 30
    cm in vacuum)
  • smaller circuits ? systems consisting only of a
    few particles are subject to Heissenberg
    uncertainty

12
Power dissipation and circuit density
  • The computer technology vintage year 2000
    requires some 3 x 10-18 Joules per elementary
    operation.
  • In 1992 Ralph Merkle from Xerox PARC calculated
    that a 1 GHz computer operating at room
    temperature, with 1018 gates packed in a volume
    of about 1 cm3 would dissipate 3 MW of power.
  • A small city with 1,000 homes each using 3 KW
    would require the same amount of power
  • A 500 MW nuclear reactor could only power some
    166 such circuits.

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Contents
  • Computing and the Laws of Physics
  • Quantum Mechanics Computers
  • Qubits and Quantum Gates
  • Quantum Parallelism
  • Deutschs Algorithm
  • Virus Structure Determination and Drug Design
  • Summary

15
A happy marriage
  • The two greatest discoveries of the 20-th century
  • quantum mechanics
  • stored program computers
  • led to the idea of
  • quantum computing and
  • quantum information theory

16
Quantum Quantum mechanics
  • Quantum ? Latin word meaning some quantity. In
    physics it is used with the same meaning as the
    word discrete in mathematics.
  • Quantum mechanics ? a mathematical model of the
    physical world.

17
Heissenbergs uncertainty principle
  • ... Quantum Mechanics shows that not only the
    determinism of classical physics must be
    abandoned, but also the naive concept of reality
    which looked upon atomic particles as if they
    were very small grains of sand. At every instant
    a grain of sand has a definite position and
    velocity. This is not the case with an electron.
    If the position is determined with increasing
    accuracy, the possibility of ascertaining its
    velocity becomes less and vice versa.' (Max
    Borns Nobel prize lecture on December 11, 1954)

18
Milestones in quantum computing
  • 1961 - Rolf Landauer decrees that computation is
    physical and studies heat generation.
  • 1973 - Charles Bennet studies the logical
    reversibility of computations.
  • 1981 - Richard Feynman suggests that physical
    systems including quantum systems can be
    simulated exactly with quantum computers.
  • 1982 - Peter Beniof develops quantum mechanical
    models of Turing machines.
  • 1984 - Charles Bennet and Gilles Brassard
    introduce quantum cryptography.
  • 1985 - David Deutsch reinterprets the
    Church-Turing conjecture.
  • 1993 - Bennet, Brassard, Crepeau, Josza, Peres,
    Wooters discover quantum teleportation.
  • 1994 - Peter Shor develops a clever algorithm for
    factoring large integers.

19
Deterministic versus probabilistic photon behavior
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Contents
  • Computing and the Laws of Physics
  • Quantum Mechanics Computers
  • Qubits and Quantum Gates
  • Quantum Parallelism
  • Virus Structure Determination and Drug Design
  • Summary

22
One qubit
  • Mathematical abstraction
  • Vector in a two dimensional complex vector space
    (Hilbert space)
  • Diracs notation
  • ket ? column
    vector
  • bra ? row vector
  • bra ? dual vector (transpose and complex
    conjugate)

23
State description
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A bit versus a qubit
  • A bit
  • Can be in two distinct states, 0 and 1
  • A measurement does not affect the state
  • A qubit
  • can be in state or in state or in
    any other state that is a linear combination of
    the basis state
  • When we measure the qubit we find it
  • in state with probability
  • in state with probability

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Qubit measurement
28
Two qubits
  • Represented as vectors in a 2-dimensional Hilbert
    space with four basis vectors
  • When we measure a pair of qubits we decide that
    the system it is in one of four states
  • with probabilities

29
Two qubits
30
Measuring two qubits
  • Before a measurement the state of the system
    consisting of two qubits is uncertain (it is
    given by the previous equation and the
    corresponding probabilities).
  • After the measurement the state is certain, it is
  • 00, 01, 10, or 11 like in the case of a
    classical two bit system.

31
Measuring two qubits (contd)
  • What if we observe only the first qubit, what
    conclusions can we draw?
  • We expect the system to be left in an uncertain
    sate, because we did not measure the second qubit
    that can still be in a continuum of states. The
    first qubit can be
  • 0 with probability
  • 1 with probability

32
Measuring two qubits (contd)
  • Call the post-measurement state when we
    measure the first qubit and find it to be 0.
  • Call the post-measurement state when we
    measure the first qubit and find it to be 1.

33
Measuring two qubits (contd)
  • Call the post-measurement state when we
    measure the second qubit and find it to be 0.
  • Call the post-measurement state when we
    measure the second qubit and find it to be 1.

34
Bell states - a special state of a pair of qubits
  • If and
  • When we measure the first qubit we get the
    post measurement state
  • When we measure the second qubit we get the
    post mesutrement state

35
This is an amazing result!
  • The two measurements are correlated, once we
    measure the first qubit we get exactly the same
    result as when we measure the second one.
  • The two qubits need not be physically constrained
    to be at the same location and yet, because of
    the strong coupling between them, measurements
    performed on the second one allow us to determine
    the state of the first.

36
Entanglement (Verschrankung)
  • Discovered by Schrodinger.
  • An entangled pair is a single quantum system in a
    superposition of equally possible states. The
    entangled state contains no information about the
    individual particles, only that they are in
    opposite states.
  • Einstein called entanglement Spooky action at a
    distance".

37
Classical gates
  • Implement Boolean functions.
  • Are not reversible (invertible). We cannot
    recover the input knowing the output.
  • This means that there is an irretrievable loss of
    information.

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One qubit gates
  • I ? identity gate leaves a qubit unchanged.
  • X or NOT gate? transposes the components of an
    input qubit.
  • Y gate.
  • Z gate ? flips the sign of a qubit.
  • H ? the Hadamard gate.

41
Identity transformation, Pauli matrices, Hadamard
42
CNOT a two qubit gate
  • Two inputs
  • Control
  • Target
  • The control qubit is transferred to the output as
    is.
  • The target qubit
  • Unaltered if the control qubit is 0
  • Flipped if the control qubit is 1.

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The two input qubits of a two qubit gates
45
State space dimension of classical and quantum
systems
  • Individual state spaces of n particles combine
    quantum mechanically through the tensor product.
    If X and Y are vectors, then
  • their tensor product X Y is also a vector,
    but its dimension is
  • dim(X) x dim(Y)
  • while the vector product X x Y has dimension
  • dim(X)dim(Y).
  • For example, if dim(X) dim(Y)10, then the
    tensor product of the two vectors has dimension
    100 while the vector product has dimension 20.

46
Parallelism and Quantum computers
  • In quantum systems the amount of parallelism
    increases exponentially with the size of the
    system, thus with the number of qubits (e.g. a 21
    qubit quantum computer is twice as powerful as a
    20 qubit quantum computer).
  • A quantum computer will enable us to solve
    problems with a very large state space.

47
Contents
  • Computing and the Laws of Physics
  • Quantum Mechanics Quantum Computers
  • Qubits and Quantum Gates
  • Quantum Parallelism
  • Deutschs Algorithm
  • Virus Structure Determination and Drug Design
  • Summary

48
A quantum circuit
  • Given a function f(x) we can construct a
    reversible quantum circuit consisting of Fredking
    gates only, capable of transforming two qubits as
    follows
  • The function f(x) is hardwired in the circuit

49
A quantum circuit (contd)
  • If the second input is zero then the
    transformation done by the circuit is

50
A quantum circuit (contd)
  • Now apply the first qubit through a Hadamad gate.
  • The resulting sate of the circuit is
  • The output state contains information about f(0)
    and f(1).

51
Quantum parallelism
  • The output of the quantum circuit contains
    information about both f(0) and f(1). This
    property of quantum circuits is called quantum
    parallelism.
  • Quantum parallelism allows us to construct the
    entire truth table of a quantum gate array having
    2n entries at once. In a classical system we can
    compute the truth table in one time step with 2n
    gate arrays running in parallel, or we need 2n
    time steps with a single gate array.
  • We start with n qubits, each in state 0gt and we
    apply a Walsh-Hadamard transformation.

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Contents
  • Computing and the Laws of Physics
  • Quantum Mechanics and Computers
  • Qubits and Quantum Gates
  • Quantum Parallelism
  • Deutschs Algorithm
  • Virus Structure Determination and Drug Design
  • Summary

55
Deutschs problem
  • Consider a black box characterized by a transfer
    function that maps a single input bit x into an
    output, f(x). It takes the same amount of time,
    T, to carry out each of the four possible
    mappings performed by the transfer function f(x)
    of the black box
  • f(0) 0
  • f(0) 1
  • f(1) 0
  • f(1) 1
  • The problem posed is to distinguish if

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A quantum circuit to solve Deutschs problem
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Evrika!!
  • By measuring the first output qubit qubit we are
    able to determine performing
    a single evaluation.

64
Contents
  • Computing and the Laws of Physics
  • Quantum Mechanics and Computers
  • Qubits and Quantum Gates
  • Quantum Parallelism
  • Deutschs Algorithm
  • Virus Structure Determination and Drug Design
  • Summary

65
Sindbis virus reconstruction and pseudo-atomic
modeling. The reconstruction computed at 11Å
(top half of first two panels) and 22Å (bottom
half of first two panels), viewed along a
two-fold axis and represented as a surface-shaded
solid (left panel) and as a thin, non-equatorial
section (middle panel). The 11Å reconstruction,
which shows significantly greater detail compared
to that in the 22Å map available approximately
one year ago, provides more accurate data for
fitting atomic models as illustrated in the right
panel, which is an enlarged view of the boxed
area in the middle panel.
66
Final remarks
  • A tremendous progress has been made in quantum
    computing and quantum information theory during
    the past decade.
  • Motivation ? the incredible impact this
    discipline could have on how we store, process,
    and transmit data and knowledge in this
    information age.

67
Final remarks (contd)
  • Computer and communication systems using quantum
    effects have remarkable properties.
  • Quantum computers enable efficient simulation of
    the most complex physical systems we can
    envision.
  • Quantum algorithms allow efficient factoring of
    large integers with applications to cryptography.
  • Quantum search algorithms speedup considerably
    the process of identifying patterns in apparently
    random data.
  • We can improve the security of our quantum
    communication systems because eavesdropping on a
    quantum communication channel can be detected
    with high probability.

68
Summary
  • Quantum computing and quantum information theory
    is truly an exciting field.
  • It is too important to be left to the physicists
    alone.
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