AntalyaQuantumComputingTutorial
... Heisenberg uncertainty principle says we cannot determine both the position and the momentum of a quantum particle with arbitrary precision. In his Nobel prize lecture on December 11, 1954 Max Born says about this fundamental principle of Quantum Mechanics : ``... It shows that not only the determin ...
... Heisenberg uncertainty principle says we cannot determine both the position and the momentum of a quantum particle with arbitrary precision. In his Nobel prize lecture on December 11, 1954 Max Born says about this fundamental principle of Quantum Mechanics : ``... It shows that not only the determin ...
final report - Cordis
... projected entangled pair state (PEPS) in a square lattice must be the same up to a trivial gauge freedom. This allows us to characterize the existence of any local or spatial symmetry in the state. As an application of these results we prove that a SU(2) invariant PEPS with half-integer spin cannot ...
... projected entangled pair state (PEPS) in a square lattice must be the same up to a trivial gauge freedom. This allows us to characterize the existence of any local or spatial symmetry in the state. As an application of these results we prove that a SU(2) invariant PEPS with half-integer spin cannot ...
art 1. Background Material
... certain circumstances. In particular, when treating heavy particles (e.g., macroscopic masses and even heavier atoms), it is often possible to use Newton dynamics. Briefly, we will discuss in more detail how the quantum and classical dynamics sometimes coincide (in which case one is free to use the ...
... certain circumstances. In particular, when treating heavy particles (e.g., macroscopic masses and even heavier atoms), it is often possible to use Newton dynamics. Briefly, we will discuss in more detail how the quantum and classical dynamics sometimes coincide (in which case one is free to use the ...
Lecture8
... Week 8. Quantum mechanics – raising and lowering operators, 1D harmonic oscillator • harmonic oscillator eigenvalues and eigenfunctions • matrix representation • motion of a minimumuncertainty wave packet • 3D harmonic oscillator • classical limit ...
... Week 8. Quantum mechanics – raising and lowering operators, 1D harmonic oscillator • harmonic oscillator eigenvalues and eigenfunctions • matrix representation • motion of a minimumuncertainty wave packet • 3D harmonic oscillator • classical limit ...
File
... the use of instructors in teaching their courses and assessing student learning. Dissemination or sale of any part of this work (including on the World Wide Web) will destroy the integrity of the work and is not permitted. The work and materials from it should never be made available to students exc ...
... the use of instructors in teaching their courses and assessing student learning. Dissemination or sale of any part of this work (including on the World Wide Web) will destroy the integrity of the work and is not permitted. The work and materials from it should never be made available to students exc ...
Quantum mechanical interaction-free measurements | SpringerLink
... interacting with the object). For example, assume it is known that an object is located in one out of two boxes. Looking and not finding it in one box tells us that the object is located inside the other box. A more sophisticated example of obtaining information in a nonlocal way is the measurement ...
... interacting with the object). For example, assume it is known that an object is located in one out of two boxes. Looking and not finding it in one box tells us that the object is located inside the other box. A more sophisticated example of obtaining information in a nonlocal way is the measurement ...
Momentum - gandell
... • Momentum cannot be created or destroyed. • The amount of momentum in the universe is constant. • This means that the total momentum in the system doesn’t change. ...
... • Momentum cannot be created or destroyed. • The amount of momentum in the universe is constant. • This means that the total momentum in the system doesn’t change. ...
BLIND QUANTUM COMPUTATION 1. Introduction and Background
... than conjectures on computational hardness. One exciting example of such an application is the idea of Universal Blind Quantum Computation.[ABE08][BFK09] 2. Blind Quantum Computation as a Quantum Interactive Proof Model One initial discussion of Blind Quantum Computation is due to Aharonov, Ben-Or, ...
... than conjectures on computational hardness. One exciting example of such an application is the idea of Universal Blind Quantum Computation.[ABE08][BFK09] 2. Blind Quantum Computation as a Quantum Interactive Proof Model One initial discussion of Blind Quantum Computation is due to Aharonov, Ben-Or, ...
NIU Physics PhD Candidacy Exam - Spring 2017 Quantum Mechanics
... You know that the concept of potential energy is not applicable in relativistic situations. One consequence of this is that the only fully relativistic quantum theories possible are quantum field theories. However, there do exist situations where a particle’s motion is “slightly relativistic” (e.g., ...
... You know that the concept of potential energy is not applicable in relativistic situations. One consequence of this is that the only fully relativistic quantum theories possible are quantum field theories. However, there do exist situations where a particle’s motion is “slightly relativistic” (e.g., ...
atom interferometer - Center for Ultracold Atoms
... Ratio pols of all alkali (Rotations using vel multiplexing) ...
... Ratio pols of all alkali (Rotations using vel multiplexing) ...
Shor`s Algorithm for Factorizing Large Integers
... product of small prime factors. We’ll suppose q = 2. Construct a quantum computer with q 2 = 22 qubits (plus additional qubits for ‘workspace’). The base states are denoted |a, b = |a|b where a, b are binary vectors (i.e. vectors with entries 0,1) of length . Equivalently, a and b (called regi ...
... product of small prime factors. We’ll suppose q = 2. Construct a quantum computer with q 2 = 22 qubits (plus additional qubits for ‘workspace’). The base states are denoted |a, b = |a|b where a, b are binary vectors (i.e. vectors with entries 0,1) of length . Equivalently, a and b (called regi ...