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Quantum Parallelism and the Exact Simulation of Physical Systems

Quantum Parallelism and the Exact Simulation of Physical Systems. Dan Cristian Marinescu School of Computer Science University of Central Florida Orlando, Florida 32816 , USA. Frontier(s)… from Webster’s unabridged dictionary.

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Quantum Parallelism and the Exact Simulation of Physical Systems

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  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 Webster’s 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. Computing Frontiers, Ischia, April 14, 2004

  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. Computing Frontiers, Ischia, April 14, 2004

  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 today’s 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. Computing Frontiers, Ischia, April 14, 2004

  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. Computing Frontiers, Ischia, April 14, 2004

  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. Computing Frontiers, Ischia, April 14, 2004

  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,… Computing Frontiers, Ischia, April 14, 2004

  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 Computing Frontiers, Ischia, April 14, 2004

  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. Computing Frontiers, Ischia, April 14, 2004

  10. Contents • Computing and the Laws of Physics • Quantum Mechanics & Computers • Qubits and Quantum Gates • Quantum Parallelism • Deutsch’s Algorithm • Virus Structure Determination and Drug Design • Summary Computing Frontiers, Ischia, April 14, 2004

  11. The limits of solid-state technologies • For the past two decades we have enjoyed Gordon Moore’s 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 Computing Frontiers, Ischia, April 14, 2004

  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. Computing Frontiers, Ischia, April 14, 2004

  13. Computing Frontiers, Ischia, April 14, 2004

  14. Contents • Computing and the Laws of Physics • Quantum Mechanics & Computers • Qubits and Quantum Gates • Quantum Parallelism • Deutsch’s Algorithm • Virus Structure Determination and Drug Design • Summary Computing Frontiers, Ischia, April 14, 2004

  15. A happy marriage… • The two greatest discoveries of the 20-th century • quantum mechanics • stored program computers led to the idea of quantum computingand quantum information theory Computing Frontiers, Ischia, April 14, 2004

  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. Computing Frontiers, Ischia, April 14, 2004

  17. Heissenberg’s 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 Born’s Nobel prize lecture on December 11, 1954) Computing Frontiers, Ischia, April 14, 2004

  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. Computing Frontiers, Ischia, April 14, 2004

  19. Deterministic versus probabilistic photon behavior Computing Frontiers, Ischia, April 14, 2004

  20. Computing Frontiers, Ischia, April 14, 2004

  21. Contents • Computing and the Laws of Physics • Quantum Mechanics & Computers • Qubits and Quantum Gates • Quantum Parallelism • Virus Structure Determination and Drug Design • Summary Computing Frontiers, Ischia, April 14, 2004

  22. One qubit • Mathematical abstraction • Vector in a two dimensional complex vector space (Hilbert space) • Dirac’s notation ket  column vector bra  row vector bra  dual vector (transpose and complex conjugate) Computing Frontiers, Ischia, April 14, 2004

  23. State description Computing Frontiers, Ischia, April 14, 2004

  24. Computing Frontiers, Ischia, April 14, 2004

  25. 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 Computing Frontiers, Ischia, April 14, 2004

  26. Computing Frontiers, Ischia, April 14, 2004

  27. Qubit measurement Computing Frontiers, Ischia, April 14, 2004

  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 Computing Frontiers, Ischia, April 14, 2004

  29. Two qubits Computing Frontiers, Ischia, April 14, 2004

  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. Computing Frontiers, Ischia, April 14, 2004

  31. Measuring two qubits (cont’d) • 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 Computing Frontiers, Ischia, April 14, 2004

  32. Measuring two qubits (cont’d) • 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. Computing Frontiers, Ischia, April 14, 2004

  33. Measuring two qubits (cont’d) • 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. Computing Frontiers, Ischia, April 14, 2004

  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 Computing Frontiers, Ischia, April 14, 2004

  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. Computing Frontiers, Ischia, April 14, 2004

  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". Computing Frontiers, Ischia, April 14, 2004

  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. Computing Frontiers, Ischia, April 14, 2004

  38. Computing Frontiers, Ischia, April 14, 2004

  39. Computing Frontiers, Ischia, April 14, 2004

  40. 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. Computing Frontiers, Ischia, April 14, 2004

  41. Identity transformation, Pauli matrices, Hadamard Computing Frontiers, Ischia, April 14, 2004

  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. Computing Frontiers, Ischia, April 14, 2004

  43. Computing Frontiers, Ischia, April 14, 2004

  44. The two input qubits of a two qubit gates Computing Frontiers, Ischia, April 14, 2004

  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. Computing Frontiers, Ischia, April 14, 2004

  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. Computing Frontiers, Ischia, April 14, 2004

  47. Contents • Computing and the Laws of Physics • Quantum Mechanics & Quantum Computers • Qubits and Quantum Gates • Quantum Parallelism • Deutsch’s Algorithm • Virus Structure Determination and Drug Design • Summary Computing Frontiers, Ischia, April 14, 2004

  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 Computing Frontiers, Ischia, April 14, 2004

  49. A quantum circuit (cont’d) • If the second input is zero then the transformation done by the circuit is Computing Frontiers, Ischia, April 14, 2004

  50. A quantum circuit (cont’d) • 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). Computing Frontiers, Ischia, April 14, 2004

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