Категории: Все - quantum

по Simnett Dale 9 лет назад

376

IQT Conference 2015

Eigenvalues are specific values in a matrix of probability representing either position or momentum, known as eigenstates, and must be measured for identification. The Hamiltonian and Lagrangian are functions that describe all possible states of a system'

IQT Conference 2015

Schedule Attached

Terminology

Hamiltonian vs Lagrangian

Both are functions representing all possible states of the position and motion/momentum at a point in time. Hamiltonian H(q,p,t) function of momentum Lagrangian L(q,q dot, t) function of velocity

Eigenvalues

An eigenvalue is a known quantity of either position or momentum in a matrix of probability. The picture represents the infinite possible states that could occur and the red box is the known quantity, the eigenstate of the object. The wave function collapses to an eigenvalue. Notes: - Can be an eigenvalue in one of two physical quantities known as eigenstates (position or momentum) - Eigenvalue must be measured to be identified

An eigenvalue is a known quantity of either position or momentum in a matrix of probability.

The picture represents the infinite possible states that could occur and the red box is the known quantity, the eigenvalue.

Notes:
- Can be an eigenvalue in one of two physical quantities known as eigenstates (position or momentum)
- Eigenvalue must be measured to be identified

Perturbing Hamiltonian A slight disturbance is applied to the system. The perturbing hamiltonian is a mathematical approximation scheme which compares the behaviour of the complicated system to a simpler "known" system result and allows a prediction of the behaviour of the system

Math

Partial Derivatives

Function in 3-D
Create function which represents the rate of change for one variable while keeping all others constant

IQT Conference 2015

Quantum Spin

Light/Atoms can be quantum or classical Spin is only quantum Hydrogen all has same size, mass, spin
Stern Gerlach Experiment has no classical explanation

Wave-Particle Duality Revisited

Beam Splitter
Only experiment that peer reviewed journal will accept as proof of single photon source

Only zero peak in the middle will prove there is only one photon produced (small peak indicates noise)

2 Golden Rules of Quantum Mechanics Quantum Coin Flip

Experiment
Any pair of polarizers at 90deg to each other allows no light through
Polarization of Light
How do you get one photon? Light is harmonic oscillator with a certain amount of energy (based on Planck) Therefore, whatever energy you detect, divide by planck's number and get number of photons Getting good at lowering the voltage with extreme position
For light going through polarizer: Iout=Iincos2theta Classic - Possibilities - Goes through or doesn't go through cos^2(theta) represents the probability that it will go through Each photon has that probability but the entire probability would only be seen after a large number of photons
Introduction
Quantum mechanics is easy as long as you give up your interpretation of reality Rule 1 : You can be here, there, here and there Rule 2 : Rule 1 works as long as you don't look (measure) Everytime you measure, you change the information you are trying to get
What is it?
Rule: Constant transition rate (probability of changing eigenstate per unit time) from one eigenstate to another eigenstate in a continuum, effected by a perturbation
Wikipedia

Keynote:  Raymond LaFlamme, IQC Director

Biography:
Subtopic

Quantum clocks - If you started two clocks at the beginning of time. They would be off at most be 3 s (accuracy of 1 part in 10^17)

Everyone is trying to prove quantum mechanics wrong but... nothing yet. IQC is working on Control

Everything that you encrypt today will be decrypted in the future. Thank you Quantum computing.

The only reasons we won't be able to build a quantum computer is: 1) The engineering hurdles are too big 2) Quantum mechanics is not the right theory to describe reality (this would be pretty amazing in itself - push in the right direction)

The limit of classic computers is about 30-40 quantum bits 1 regular bit can be represented by 2 states (0 or 1) 1 quantum bit can be represented by an infinite number of states ???? Deterministic - 0 or 1 - must be one of them Quantum - 0 or 1 or a probability of states in between

Quantum Information - Language to talk to atoms and molecules

Qubits - Can be 0 or 1 or (infinite states between 0 and 1)