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Laser Cosmology
Laser Cosmology

approximation of thermal equilibrium for quantum gases with
approximation of thermal equilibrium for quantum gases with

Beyond the Cookie Cutter Paradigm
Beyond the Cookie Cutter Paradigm

Phase-Coherent Transport through a Mesoscopic System: A New Probe V 80, N
Phase-Coherent Transport through a Mesoscopic System: A New Probe V 80, N

... spectroscopy of mesoscopic systems, as have other spectroscopies such as optical absorption. For example, a measurement of the tunneling current through a quantum dot as a function of temperature, voltage, and magnetic field yields information about the electronic many-body states present there. Unf ...
chap3
chap3

Main
Main

... that a particular outcome of a measurement cannot be understood as revealing the pre-existing definite value of some underlying hidden variable [6, 7]. Whether the origin of the speed-up of our algorithm can be explained by contextuality is an open question. In this work, we present an oracle-based ...
Product Vacua with Boundary States
Product Vacua with Boundary States

Slide 1
Slide 1

... • T has no classical analog; it is a quantum mechanical vector, literally “like spin” (iso = ‘like’), so it follows the same addition rules as S, L, J, etc... ...
Mixed quantum–classical dynamics
Mixed quantum–classical dynamics

On the Theory of Intramolecular Energy Transfer
On the Theory of Intramolecular Energy Transfer

... corresponding semiclassical trajectory (i.e. the one whose actions match the quantum numbers via a semiclassical relation). 1 They display regular (rather than chaotic) contour patterns. Indeed, semiclassically calculated wavefunctions are expected to compare well with the quantum-mechanical ones, i ...
Localization transition in a ballistic quantum wire
Localization transition in a ballistic quantum wire

in PPT
in PPT

... • Good randomness is usually verified by a series of statistical tests. • There exist chaotic systems, of deterministic nature, that pass all existing randomness tests. Uchida et al., Nat. Phot. 2, 728 (2008) • Do these tests really certify the presence of randomness? ...
Quantum Computers - Computing Sciences
Quantum Computers - Computing Sciences

... detectors behind the slits but before the screen Look to see if the photons are behaving like particles or like waves after they had passed the slits but before they hit the far screen ...
Lecture 22/23 1  Quantum  Mechanics
Lecture 22/23 1 Quantum Mechanics

Packard Poster-2 - Northwestern University Mesoscopic Physics
Packard Poster-2 - Northwestern University Mesoscopic Physics

... Cooper pairs of electrons are naturally created. Though the constituent electrons of these pairs form a single quantum object, they are spatially separated by a coherence length x which can extend several hundred nanometers. As this length scale is now easily accessible to modern nanolithographic te ...
5.1 Revising the Atomic Model - Somerset Academy Silver Palms
5.1 Revising the Atomic Model - Somerset Academy Silver Palms

Evolving Notions of Security for Quantum Protocols
Evolving Notions of Security for Quantum Protocols

Chapter 6 Electronic Structure of Atoms
Chapter 6 Electronic Structure of Atoms

Quantum Optics and Quantum Information with - GdR-IQFA
Quantum Optics and Quantum Information with - GdR-IQFA

... -> Design of Continuous-Variable QKD protocols where : * The non-commuting observables are the quadrature operators X and P * The transmitted light contains weak coherent pulses (about 10 photons) with a gaussian modulation of amplitude and phase * The detection is made using shot-noise limited homo ...
II: Experimental Atomic Spectroscopy
II: Experimental Atomic Spectroscopy

... which, historically, were identified by their appearance as “sharp,” “principal,” “diffuse,” and “fundamental”. With a large enough dispersion it could be noted that the lines were either doublets or triplets with separation of, at most, a few Angstroms. For sodium (Z = 11) the first two subshells a ...
Conservation Laws - University of Toronto Physics
Conservation Laws - University of Toronto Physics

Quantum graphs and the integer quantum Hall effect
Quantum graphs and the integer quantum Hall effect

2014-15 Archived Abstracts
2014-15 Archived Abstracts

... heat and a T^2 resistivity. Studying the evolution of the T¬ dependence of these observables as a function of a control parameter leads to the identification both of the presence and the nature of the quantum phase transition in candidate systems. In this study we measure the transport properties of ...
Ultracold chemistry and its reaction kinetics
Ultracold chemistry and its reaction kinetics

Part 1 - SCIPP
Part 1 - SCIPP

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Particle in a box



In quantum mechanics, the particle in a box model (also known as the infinite potential well or the infinite square well) describes a particle free to move in a small space surrounded by impenetrable barriers. The model is mainly used as a hypothetical example to illustrate the differences between classical and quantum systems. In classical systems, for example a ball trapped inside a large box, the particle can move at any speed within the box and it is no more likely to be found at one position than another. However, when the well becomes very narrow (on the scale of a few nanometers), quantum effects become important. The particle may only occupy certain positive energy levels. Likewise, it can never have zero energy, meaning that the particle can never ""sit still"". Additionally, it is more likely to be found at certain positions than at others, depending on its energy level. The particle may never be detected at certain positions, known as spatial nodes.The particle in a box model provides one of the very few problems in quantum mechanics which can be solved analytically, without approximations. This means that the observable properties of the particle (such as its energy and position) are related to the mass of the particle and the width of the well by simple mathematical expressions. Due to its simplicity, the model allows insight into quantum effects without the need for complicated mathematics. It is one of the first quantum mechanics problems taught in undergraduate physics courses, and it is commonly used as an approximation for more complicated quantum systems.
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