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Umesh V. Vazirani University of California, Berkeley Quantum Mechanics & Quantum Computation Lecture 5: Quantum Gates Time evolution of a quantum system

Umesh V. Vazirani University of California, Berkeley · PDF fileUmesh V. Vazirani University of California, Berkeley Quantum Mechanics & Quantum Computation Lecture 5: Quantum Gates

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Page 1: Umesh V. Vazirani University of California, Berkeley · PDF fileUmesh V. Vazirani University of California, Berkeley Quantum Mechanics & Quantum Computation Lecture 5: Quantum Gates

Umesh V. Vazirani University of California, Berkeley

Quantum Mechanics & Quantum Computation

Lecture 5: Quantum Gates

Time evolution of a quantum system

Page 2: Umesh V. Vazirani University of California, Berkeley · PDF fileUmesh V. Vazirani University of California, Berkeley Quantum Mechanics & Quantum Computation Lecture 5: Quantum Gates

Axiom 1. Superposition principle

Axiom 2. Measurement

Axiom 3. Unitary evolution

Axioms of quantum mechanics

Page 3: Umesh V. Vazirani University of California, Berkeley · PDF fileUmesh V. Vazirani University of California, Berkeley Quantum Mechanics & Quantum Computation Lecture 5: Quantum Gates

Superposition

• Allowable states of k-level system: unit vector in a k-dimensional complex vector space (called a Hilbert space).

Page 4: Umesh V. Vazirani University of California, Berkeley · PDF fileUmesh V. Vazirani University of California, Berkeley Quantum Mechanics & Quantum Computation Lecture 5: Quantum Gates

Measurement

• A measurement is specified by choosing an orthonormal basis.

• The probability of each outcome is the square of the length of the projection onto the corresponding basis vector.

• The state collapses to the observed basis vector.

Page 5: Umesh V. Vazirani University of California, Berkeley · PDF fileUmesh V. Vazirani University of California, Berkeley Quantum Mechanics & Quantum Computation Lecture 5: Quantum Gates

Evolution

• How does the state evolve in time?

Page 6: Umesh V. Vazirani University of California, Berkeley · PDF fileUmesh V. Vazirani University of California, Berkeley Quantum Mechanics & Quantum Computation Lecture 5: Quantum Gates

Evolution

• How does the state evolve in time? By a rotation of the Hilbert space!

Page 7: Umesh V. Vazirani University of California, Berkeley · PDF fileUmesh V. Vazirani University of California, Berkeley Quantum Mechanics & Quantum Computation Lecture 5: Quantum Gates

Example: evolution of a qubit.

It is a rigid body rotation, meaning that the angles between vectors are preserved.

Page 8: Umesh V. Vazirani University of California, Berkeley · PDF fileUmesh V. Vazirani University of California, Berkeley Quantum Mechanics & Quantum Computation Lecture 5: Quantum Gates

• Rotation of the space is a linear transformation. Represent by a matrix:

• Example

Rotation Matrix

Page 9: Umesh V. Vazirani University of California, Berkeley · PDF fileUmesh V. Vazirani University of California, Berkeley Quantum Mechanics & Quantum Computation Lecture 5: Quantum Gates

• Rotation of the space is a linear transformation. Represent by a matrix:

• Example

Rotation Matrix

Page 10: Umesh V. Vazirani University of California, Berkeley · PDF fileUmesh V. Vazirani University of California, Berkeley Quantum Mechanics & Quantum Computation Lecture 5: Quantum Gates

• Rotation of the space is a linear transformation. Represent by a matrix:

• Example

Rotation Matrix

Page 11: Umesh V. Vazirani University of California, Berkeley · PDF fileUmesh V. Vazirani University of California, Berkeley Quantum Mechanics & Quantum Computation Lecture 5: Quantum Gates
Page 12: Umesh V. Vazirani University of California, Berkeley · PDF fileUmesh V. Vazirani University of California, Berkeley Quantum Mechanics & Quantum Computation Lecture 5: Quantum Gates

Quantum gates

U

Page 13: Umesh V. Vazirani University of California, Berkeley · PDF fileUmesh V. Vazirani University of California, Berkeley Quantum Mechanics & Quantum Computation Lecture 5: Quantum Gates

“Bit flip”

“Phase flip”

Page 14: Umesh V. Vazirani University of California, Berkeley · PDF fileUmesh V. Vazirani University of California, Berkeley Quantum Mechanics & Quantum Computation Lecture 5: Quantum Gates

Bit flip rotation axis

Phase flip

Page 15: Umesh V. Vazirani University of California, Berkeley · PDF fileUmesh V. Vazirani University of California, Berkeley Quantum Mechanics & Quantum Computation Lecture 5: Quantum Gates

“Hadamard transform”

Page 16: Umesh V. Vazirani University of California, Berkeley · PDF fileUmesh V. Vazirani University of California, Berkeley Quantum Mechanics & Quantum Computation Lecture 5: Quantum Gates

“Hadamard transform”

Page 17: Umesh V. Vazirani University of California, Berkeley · PDF fileUmesh V. Vazirani University of California, Berkeley Quantum Mechanics & Quantum Computation Lecture 5: Quantum Gates

“Bit flip”

“Phase flip”

“Hadamard transform”

Page 18: Umesh V. Vazirani University of California, Berkeley · PDF fileUmesh V. Vazirani University of California, Berkeley Quantum Mechanics & Quantum Computation Lecture 5: Quantum Gates

• One-qubit gates:

• What is the dimension of two-qubit gates?

is a 4x4 unitary matrix.

U

Page 19: Umesh V. Vazirani University of California, Berkeley · PDF fileUmesh V. Vazirani University of California, Berkeley Quantum Mechanics & Quantum Computation Lecture 5: Quantum Gates

“CNOT”

Page 20: Umesh V. Vazirani University of California, Berkeley · PDF fileUmesh V. Vazirani University of California, Berkeley Quantum Mechanics & Quantum Computation Lecture 5: Quantum Gates
Page 21: Umesh V. Vazirani University of California, Berkeley · PDF fileUmesh V. Vazirani University of California, Berkeley Quantum Mechanics & Quantum Computation Lecture 5: Quantum Gates
Page 22: Umesh V. Vazirani University of California, Berkeley · PDF fileUmesh V. Vazirani University of California, Berkeley Quantum Mechanics & Quantum Computation Lecture 5: Quantum Gates