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Chapter 1. Fundamental Theory
Chapter 1. Fundamental Theory

... 2) det(AB) = det(A)det(B) , for square matrices A and B . 3) det(AT ) = det(A); det(A* ) = [det(A)]*; det(A† ) = [det(A)]* . 4) det(A−1 ) = ...
Metric fluctuations and decoherence
Metric fluctuations and decoherence

Quantum correlations - Uniwersytet otwarty UG
Quantum correlations - Uniwersytet otwarty UG

Fault-tolerant quantum computation
Fault-tolerant quantum computation

... realize subtle interference phenomena in systems with many degrees of freedom? If so, these systems are bound to behave in ways that will surprise and delight us. ...
Lecture 5
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Holonomic Quantum Computation with Josephson Networks
Holonomic Quantum Computation with Josephson Networks

Just enough on Dirac Notation
Just enough on Dirac Notation

... ket |ψi is a quantum state whose wavefuntion is ψ(x). It is a fairly subtle distinction, but it is rather like the difference between a physical vector (eg the velocity of a particle) and the list of its components in a particular basis. The latter is a particular representation of the former, and s ...
The density matrix renormalization group
The density matrix renormalization group

Semiconductor qubits for quantum computation
Semiconductor qubits for quantum computation

Semiconductor qubits for quantum computation
Semiconductor qubits for quantum computation

... - hidden information! - Wave function collapse prevents us from directly accessing the information ...
What Does Quantum Mechanics Suggest About Our
What Does Quantum Mechanics Suggest About Our

The Learnability of Quantum States
The Learnability of Quantum States

... Theorem: No public-key quantum money scheme can be information-theoretically secure. Proof Sketch: A counterfeiter with unlimited computation time can do this… Let U be an ensemble of possible quantum money states Initially, U0 contains s for every s{0,1}n ...
quantum scale
quantum scale

Introduction: effective spin
Introduction: effective spin

Derivation of the Pauli exchange principle
Derivation of the Pauli exchange principle

Numerical Methods Project: Feynman path integrals in quantum
Numerical Methods Project: Feynman path integrals in quantum

Quantum structures in general relativistic theories
Quantum structures in general relativistic theories

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Photonic realization of nonlocal memory effects and non

Berry phase correction to electron density of states in solids
Berry phase correction to electron density of states in solids

On the Control of Open Quantum Systems in the Weak Coupling Limit
On the Control of Open Quantum Systems in the Weak Coupling Limit

Particle control in a quantum world
Particle control in a quantum world

Observables and Measurements
Observables and Measurements

Quantum Circuits. Intro to Deutsch. Slides in PPT.
Quantum Circuits. Intro to Deutsch. Slides in PPT.

... Universality in the quantum circuit model Classically, any function f(x) can be computed using just nand and fanout; we say those operations are universal for classical computation. Suppose U is an arbitrary unitary transformation on n qubits. Then U can be composed from controlled-not gates and si ...
fn1_1h_qm2_cr
fn1_1h_qm2_cr

... Quantum Numbers The third quantum number, ml, is the orbital. Every sublevel has one or more orbitals. The s sublevel has 1 orbital, the p sublevel has 3 orbitals, the d sublevel has 5 orbitals, etc. These orbital can be indicated by the number ml = l, l-1, …0, -1, … -l The fourth quantum number, m ...
Slide 1
Slide 1

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Quantum decoherence

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