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Decoherence in Solid State Qubits
Decoherence in Solid State Qubits

Topological quantum computation
Topological quantum computation

Observation of Distinct Two-Photon Transition Channels in CdTe
Observation of Distinct Two-Photon Transition Channels in CdTe

... intermediate confinement regime (diameter higher than 6 nm, Bohr radius for CdTe is 7.5 nm [29]). Even so, the reported degenerate 2PA spectrum, for CdTe QDs does not include the region for the lowest energy transition (1S3/2 (h) → 1S(e)), and the available data are limited to specific wavelengths. ...
Semiclassical approximations in wave mechanics
Semiclassical approximations in wave mechanics

Quantum error correction
Quantum error correction

Quantum Monte Carlo simulations of solids W. M. C. Foulkes
Quantum Monte Carlo simulations of solids W. M. C. Foulkes

J. Phys. Chem. B 106, 8271, 2002
J. Phys. Chem. B 106, 8271, 2002

Full-Text PDF
Full-Text PDF

... The main point here is that for an electronic structure, the (D → ∞)-limit is beguilingly simple and exactly computable for any atom and molecule. For D finite, but very large, the electrons are confined to harmonic oscillations about the fixed positions attained in the (D → ∞)-limit. Indeed, in thi ...
PPT
PPT

In Search of Quantum Reality
In Search of Quantum Reality

A Dissertation entitled Quantum Theory of Ion
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Electronic structure of quantum dots

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Three Myths About Time Reversal in Quantum Theory 1. Introduction

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Three myths about time reversal in quantum theory

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Quantum Computation and Quantum Information 10th Anniversary

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... output and, when the control carries |1 >, inverts the target. Two repeated CNOTs cancel out, but three non-canceling CNOTs, that alternate controls and targets, swap quantum states and are referred to as a SWAP gate. T OFFOLI GATE has three inputs and outputs. It is similar to the CNOT gate, but in ...
Quantum Transport in Finite Disordered Electron Systems
Quantum Transport in Finite Disordered Electron Systems

Introduction to Quantum Entanglement
Introduction to Quantum Entanglement

Superconducting Qubits and Circuits: Artificial Atoms Coupled to
Superconducting Qubits and Circuits: Artificial Atoms Coupled to

Consciousness in the universe A review of the ‘Orch OR’ theory ScienceDirect
Consciousness in the universe A review of the ‘Orch OR’ theory ScienceDirect

... Consciousness has often been argued to be a sequence of discrete moments. William James [27] described the “specious present, the short duration of which we are immediately and incessantly sensible” (though James was vague about duration, and also described a continual ‘stream of consciousness’). Th ...
Compatibility of Quark and Resonant Picture Excited Baryon
Compatibility of Quark and Resonant Picture Excited Baryon

Quantum theory of ion-atom interactions
Quantum theory of ion-atom interactions

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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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