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Lecture28
Lecture28

2.2
2.2

Generating Single Photons on Demand I Vladan Vuletic
Generating Single Photons on Demand I Vladan Vuletic

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20040929114512301

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... The Letter by Deng et al. [1] presents an analytic theoretical description of matter-wave superradiance [2] which claims to go beyond previous theoretical frameworks. I show here that the theory presented in this Letter is not a description of superradiance per se, but rather an elegant perturbative ...
Hyperfine Structure of Rubidium
Hyperfine Structure of Rubidium

... 1. Be safe. If the current is greater than 76mA; wear safety goggles, take off watches, rings, etc. You know the drill. 2. Do not touch the optical surface of any optical component. Make sure the center of all optical surfaces is at approximately the same height. Adjust each optical surface so the l ...
Electricity & Optics Physics 24100 Lecture 22 – Chapter 31 sec. 1-4,6
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... associated with each photon absorption event is much smaller than the momentum of a thermal atom, several thousand absorption-emission events are required to significantly change the atom’s velocity. Therefore laser cooling has only been demonstrated with atoms that can be optically cycled many time ...
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... 1. In the ground state the electron occupies the lowest available energy level. 2. The electron can jump to a higher energy level (excited state) if it absorbs energy. 3. The excited state is instable. 4. Electron falls back to a lower energy level. 5. Energy given off as a photon. The energy of the ...
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... x2 . This would be the situation if particle 1 and 2 moved in external potentials but felt no mutual interaction. In the case of positronium, we usually have the opposite problem of zero external potential but the electron and positron (antielectron) attract each other with a potential related to th ...
Lecture 13 - UD Physics
Lecture 13 - UD Physics

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Population inversion

In science, specifically statistical mechanics, a population inversion occurs while a system (such as a group of atoms or molecules) exists in a state with more members in an excited state than in lower energy states. It is called an ""inversion"" because in many familiar and commonly encountered physical systems, this is not possible. The concept is of fundamental importance in laser science because the production of a population inversion is a necessary step in the workings of a standard laser.
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