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Quantum Information Processing A. Hamed Majedi Institute for Quantum Computing (IQC) and RF/Microwave & Photonics Group ECE Dept., University of Waterloo

Quantum Information Processing

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A. Hamed Majedi Institute for Quantum Computing (IQC) and RF/Microwave & Photonics Group ECE Dept., University of Waterloo. Quantum Information Processing. Outline. Limits of Classical Computers Quantum Mechanics - PowerPoint PPT Presentation

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Page 1: Quantum Information Processing

Quantum Information Processing

A. Hamed Majedi

Institute for Quantum Computing (IQC)

and

RF/Microwave & Photonics Group

ECE Dept., University of Waterloo

Page 2: Quantum Information Processing
Page 3: Quantum Information Processing

Outline

• 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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3

Your Computer

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Moore’s Law

The # of transistors per square inch had doubled every year since the invention of ICs.

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4

How small can they be?

Here Quantum mechanics comesinto play

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Limits 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?

Page 8: Quantum Information Processing

Quantum Computation & Information

• Study of information processing tasks can be accomplished using Quantum Mechanical systems.

QuantumMechanics

ComputerScience

InformationTheory

Cryptography

Page 9: Quantum Information Processing

Quantum 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, …

Page 10: Quantum Information Processing

Classical vs Quantum Experiments

• Classical Experiments Experiment with bullets

Experiment with waves

• Quantum Experiments Two slits Experiment with electrons

Stern-Gerlach Experiment

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Exp. With Bullet (1)

Gun

wall

H1

H2

(a)

detector

wall

P1(x)

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Exp. With Bullet (2)

Gun

wall

H1

H2

(a)

detector

wall

P2(x)

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Exp. With Bullet (3)

Gun

wall

H1

H2

(a)

P2(x)

P1(x)

(c)(b) (c)

(x))P(x)(P(x)P 2121

12

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Exp. with Waves (1)

wave source H1

H2

H1

detector

wall

I1(x)

I2(x)

(b)

Page 15: Quantum Information Processing

Exp. with Waves (2)detector

wall

I1(x)

I2(x)

(b) (c)

2

2112 (x)(x)(x)I hh

H1

H2

wave source

Page 16: Quantum Information Processing

Two Slit Experiment (1)

source of electrons

wall

H1

H2

(a)

detector

wall

P2(x)

P1(x)

(b) (c)(c)

(x))P(x)(P(x)P 2121

12

Results intuitively expected

Page 17: Quantum Information Processing

Two Slit Experiment (2)

source of electrons

wall

H1

H2

(a)

detector

wall

P2(x)

P1(x)

(b) (c)

?(x)P12

Results observed

Page 18: Quantum Information Processing

Two Slit Exp. With Observer

source of electrons

detector

wall

P2(x)

P1(x)

(b) (c)

(x)P(x)P(x)P 2112

Interference disappeared!

light source

“⇨ Decoherence”

H1

H2

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Results 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

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Stern-Gerlach Experiment

S

N

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QM Physical Concepts

• Wave Function

• Quantum Dynamics (Schrodinger Eq.)

• Statistical Interpretation (Born Postulate)

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Bit & Quantum Bits (1)V(t)

t 1

V(t)

t0

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More Quantum Bits

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Qubit (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 &

&

&

1

01

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Qubit (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.

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Math of Qubits

• Qubits can be represented in Bloch Sphere.

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Quantum 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.

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Example of Quantum Gates

• NOT gate: X

• Z gate: Z

• Hadamard gate:

H

P• Phase gate:

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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.

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Measurement

• 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.

M

Probabilistic Classical Bit

Probabilistic Classical Bit

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Multiple 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.

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Multiple Qubit Gates

A

B

A

B A

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.

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Physics & 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

Page 34: Quantum Information Processing

Physical 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.

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DiVinZenco 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.

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Quantum 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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Spintronics

Cavity QED

Atom Chip

RF-SQUID

Cooper

Pair Box

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Perspective of Quantum Computation & Information

• Quantum Parallelism• Quantum Algorithms solve some of the complex

problems efficiently (Schor’s 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.