Title: Quantum Information Processing
1 Quantum Information Processing
-
- A. Hamed Majedi
-
- Institute for Quantum Computing (IQC)
- and
- RF/Microwave Photonics Group
- ECE Dept., University of
Waterloo -
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3Outline
- Limits of Classical Computers
- Quantum Mechanics
- Classical vs. Quantum Experiments
- Postulates of quantum Mechanics
- Qubit
- Quantum Gates
- Universal Quantum Computation
- Physical realization of Quantum Computers
- Perspective of Quantum Computers
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5Moores Law
The of transistors per square inch had doubled
every year since the invention of ICs.
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7Limits of Classical Computation
- Reaching the SIZE Operational time limits
- 1- Quantum Physics has to be considered for
device operation. - 2- Technologies based on Quantum Physics
could improve the clock-speed of microprocessors,
decrease power dissipation miniaturize more!
(e.g. Superconducting - processors based on RSFQ, HTMT Technology)
- Is it possible to do much more? Is there any
new kind of information processing based on
Quantum Physics?
8Quantum Computation Information
- Study of information processing tasks can be
accomplished using Quantum Mechanical systems.
Quantum Mechanics
Computer Science
Information Theory
Cryptography
9Quantum Mechanics History
- Classical Physics fail to explain
- 1- Heat Radiation Spectrum
- 2- Photoelectric Effect
- 3- Stability of Atom
- Quantum Physics solve the problems
- Golden age of Physics from 1900-1930 has been
formed - by Planck, Einstein, Bohr, Schrodinger,
Heisenberg, Dirac, Born,
10Classical vs Quantum Experiments
- Classical Experiments
- Experiment with bullets
- Experiment with waves
- Quantum Experiments
- Two slits Experiment with electrons
- Stern-Gerlach Experiment
11Exp. With Bullet (1)
12Exp. With Bullet (2)
13Exp. With Bullet (3)
(c)
(b)
14Exp. with Waves (1)
wave source
H1
H1
H2
15Exp. with Waves (2)
wave source
H1
H2
16Two Slit Experiment (1)
(c)
17Two Slit Experiment (2)
18Two Slit Exp. With Observer
Interference disappeared!
H1
H2
? Decoherence
19Results from Experiments
- Two distinct modes of behavior (Wave-Particle
- Duality)
- 1- Wave like 2-
Particle-like - Effect of Observations can not be ignored.
- Indeterminacy (Heisenberg Uncertainty
Principle) - Evolution and Measurement must be
distinguished
20Stern-Gerlach Experiment
21QM Physical Concepts
- Wave Function
- Quantum Dynamics (Schrodinger Eq.)
- Statistical Interpretation (Born Postulate)
-
22Bit Quantum Bits (1)
23More Quantum Bits
24Qubit (1)
- A qubit has two possible states
- Unlike Bits, qubits can be in superposition state
- A qubit is a unit vector in 2D Vector Space
- (2D Hilbert Space)
- are orthonormal
computational basis - We can assume that
25Qubit (2)
- A measurement yields 0 with probability
1 with - probability
- Quantum state can not be recovered from qubit
measurement. - A qubit can be entangled with other qubits.
- There is an exponentially growing hidden
quantum information.
26Math of Qubits
- Qubits can be represented in Bloch Sphere.
27Quantum Gates
- A Quantum Gate is any transformation in Bloch
sphere allowed by laws of QM, that is a Unitary
transformation. - The time evolution of the state of a closed
system is described by Schrodinger Eq.
28Example of Quantum Gates
Hadamard gate
Phase gate
29 Universal Computation
- Classical Computing Theorem
- Any functions on bits can be computed from
the composition of NAND gates alone, known as
Universal - gate.
- Quantum Computing Theorem
- Any transformation on qubits can be done from
composition of any two quantum gates. - e.g. 3 phase gates 2 Hadamard gates, the
universal computation is achieved. - No cloning Theorem
- Impossible to make a copy from unknown qubit.
30Measurement
- A measurement can be done by a projection of each
- in the basis states, namely
and . - Measurement can be done in any orthonormal
and linear combination of states . - Measurement changes the state of the system
can not - provide a snapshot of the entire system.
-
Probabilistic Classical Bit
M
Probabilistic Classical Bit
31Multiple Qubits
- The state space of n qubits can be represented
by Tensor - Product in Hilbert space with
orthonormal base vectors. E.g.
- states produced by Tensor Product is
separable measurement of one will not affect
the other. - Entangled state can not be represented by
Tensor Product - E.g.
32Multiple Qubit Gates
C-NOT Gate
Any Multiple qubit logic gate may be composed
from C-NOT and single qubit gate. C-NOT Gate is
Invertible gates. There is not an irretrievable
loss of information under the action of C-NOT.
33Physics Math Connections in QIP
Postulate 1
Postulate 2
Postulate 3
Postulate 4
Isolated physical system
Evolution of a physical system
Measurements of a physical system
Composite physical system
Hilbert Space
Unitary transformation
Measurement operators
Tensor product of components
34Physical Realization of QC
- Storage Store qubits for long time
- Isolation Qubits must be isolated from
environment to - decrease Decoherence
- Readout Measuring qubits efficiently reliably.
- Gates Manipulate individual qubits induce
controlled interactions among them, to do quantum
networking. - Precision Quantum networking measurement
should be implemented with high precision.
35DiVinZenco Checklist
- A scalable physical system with well
characterized qubits. - The ability to initialize the state of the
qubits. - Long decoherence time with respect to gate
operation time - Universal set of quantum gates.
- A qubit-specific measurement capability.
36Quantum Computers
- Ion Trap
- Cavity QED (Quantum ElectroDynamics)
- NMR (Nuclear Magnetic Resonance)
- Spintronics
- Quantum Dots
- Superconducting Circuits (RF-SQUID, Cooper-Pair
Box) - Quantum Photonic
- Molecular Quantum Computer
-
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38Perspective of Quantum Computation Information
- Quantum Parallelism
- Quantum Algorithms solve some of the complex
problems efficiently (Schors algorithm, Grover
search algorithm) - QC can simulate quantum systems efficiently!
- Quantum Cryptography A secure way of
exchanging keys such that eavesdropping can
always be detected. - Quantum Teleportation Transfer of
information using quantum entanglement.