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Cavity Quantum Electrodynamics with Ultracold Atoms
Cavity Quantum Electrodynamics with Ultracold Atoms

EGAS41
EGAS41

... Dielectronic recombination of H-like highly charged ions O.Yu. Andreev, L.N. Labzowsky, A.V. Prigorovsky CP 2, p62 Progress in the analysis of the odd parity configurations of tantalum atom B. Arcimowicz, J. Dembczyński CP 3, p63 Population transfer in four-level atomic or molecular systems with fa ...
Interaction between Atomic Ensembles and Optical
Interaction between Atomic Ensembles and Optical

... Heinzen & Feld, 1987). Studies have concentrated on fundamental aspects of the system such as the vacuum Rabi splitting (Agarwal, 1984; Boca et al., 2004; Brennecke et al., 2007; Colombe et al., 2007; Kaluzny et al., 1983; Raizen et al., 1989; Thompson et al., 1992; Zhu et al., 1990), nonclassical l ...
Single and double bosonic stimulation of THz emission in polaritonic systems
Single and double bosonic stimulation of THz emission in polaritonic systems

Microscopic Probing and Manipulation of Ultracold
Microscopic Probing and Manipulation of Ultracold

book chapter on saddle point searches
book chapter on saddle point searches

Optical Pumping
Optical Pumping

Graphene plasmonics: A platform for strong light
Graphene plasmonics: A platform for strong light

Attosecond real time observation of ionization and electron
Attosecond real time observation of ionization and electron

... decreased and approaches nowadays the ultimate limit of a single field oscillation, which corresponds to ~ 2.5 femtosecond (10-15 s) for visible light. During this development, the advances in optical technology opened more and more fields in not only atomic, but also molecular and solid-state physi ...
Individual Trapped Atoms for Cavity QED Quantum
Individual Trapped Atoms for Cavity QED Quantum

pdf
pdf

Quantum Dynamics of Condensates, Atomtronic Systems, and
Quantum Dynamics of Condensates, Atomtronic Systems, and

Ph.D. thesis - Chin Lab at the University of Chicago
Ph.D. thesis - Chin Lab at the University of Chicago

Deviation from Universality in Collisions of Ultracold 6Li2 Molecules
Deviation from Universality in Collisions of Ultracold 6Li2 Molecules

... This quantum Langevin model assumes a large number of available exit channels in the short-range part of the interaction potential, leading to a unit probability of loss there, and leaving the decay rate dependent on only the longrange van der Waals interaction between collision partners. It has bee ...
Experiments and theory in cold and ultracold collisions
Experiments and theory in cold and ultracold collisions

... scale of temperature (energy divided by Boltzmann’s constant k B ) plotted against the de Broglie wavelength for atomic sodium. The term a 0 represents the Bohr radius of the H atom. ...
Manipulating Bose-Einstein condensates with laser light Shin Inouye
Manipulating Bose-Einstein condensates with laser light Shin Inouye

Bragg spectroscopy of quantum gases: Exploring physics in one
Bragg spectroscopy of quantum gases: Exploring physics in one

A high finesse optical resonator for cavity QED experiments
A high finesse optical resonator for cavity QED experiments

Local-Field Effects and Nanostructuring for Controlling Optical
Local-Field Effects and Nanostructuring for Controlling Optical

... and improving the linear and nonlinear optical properties of materials. Within my studies, two approaches are considered: nanostructuring and invoking local-field effects. These broad topics involve various projects that I have undertaken during my Ph. D. research. The first project is on composite ...
Atom-Wall interaction
Atom-Wall interaction

Fluctuations in Quantum Degenerate Fermi Gases
Fluctuations in Quantum Degenerate Fermi Gases

drastically
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... The Mollow Absorption Spectrum of a Neutral QD . . . . . . . . . . 37 Band Structure and Energy Level Diagram of The Trion State . . . . 44 Trion Mollow Absorption Spectrum . . . . . . . . . . . . . . . . . . . 46 Signatures of Heavy-light Hole Mixing . . . . . . . . . . . . . . . . . 54 Signature o ...
Vers un plan détaillé (début 08/11/01)
Vers un plan détaillé (début 08/11/01)

Universitat Autonoma de Barcelona Facultat de Ciencies, Departament de F sica
Universitat Autonoma de Barcelona Facultat de Ciencies, Departament de F sica

Laser cooling of trapped ions - Quantum Optics and Spectroscopy
Laser cooling of trapped ions - Quantum Optics and Spectroscopy

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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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