Quench dynamics of a disordered array of dissipative coupled cavities

We investigate the mean-field dynamics of a system of interacting photons in an array of coupled cavities in presence of dissipation and disorder. We follow the evolution of on an initially prepared Fock state, and show how the interplay between dissipation and disorder affects the coherence properties of the cavity emission and that these properties can be used as signatures of the many-body phase of the whole array.Comment: 8 pages, 10 figures, new reference adde

On the radiative lifetime of free-moving two-dimensional excitons

A simple microscopic mechanism explaining the linear dependence of the radiative lifetime of free-moving two-dimensional excitons on their effective temperature is suggested. It is shown that there exists a characteristic effective temperature (of about few Kelvin) defined by the exciton-acoustic phonon interaction at which the radiative lifetime is minimal. Below this temperature the lifetime starts to increase with decreasing temperature. The correspondence with previous theoretical and experimental results is discussed.Comment: 5 pages, 3 figures. Final versio

Creation of entangled states in coupled quantum dots via adiabatic rapid passage

Quantum state preparation through external control is fundamental to established methods in quantum information processing and in studies of dynamics. In this respect, excitons in semiconductor quantum dots (QDs) are of particular interest since their coupling to light allows them to be driven into a specified state using the coherent interaction with a tuned optical field such as an external laser pulse. We propose a protocol, based on adiabatic rapid passage, for the creation of entangled states in an ensemble of pairwise coupled two-level systems, such as an ensemble of QD molecules. We show by quantitative analysis using realistic parameters for semiconductor QDs that this method is feasible where other approaches are unavailable. Furthermore, this scheme can be generically transferred to some other physical systems including circuit QED, nuclear and electron spins in solid-state environments, and photonic coupled cavities.Comment: 10 pages, 2 figures. Added reference, minor changes. Discussion, results and conclusions unchange

Microcavity polariton-like dispersion doublet in resonant Bragg gratings

Periodic structures resonantly coupled to excitonic media allow the existence of extra intragap modes ('Braggoritons'), due to the coupling between Bragg photon modes and 3D bulk excitons. This induces unique and unexplored dispersive features, which can be tailored by properly designing the photonic bandgap around the exciton resonance. We report that one-dimensional Braggoritons realized with semiconductor gratings have the ability to mimic the dispersion of quantum-well microcavity polaritons. This will allow the observation of new nonlinear phenomena, such as slow-light-enhanced nonlinear propagation and an efficient parametric scattering at two 'magic frequencies'

Quantum well polaritons : strong and weak coupling regimes

The work described in this thesis is a theoretical investigation of the properties of exciton-polaritons in quantum wells (QWs). The polariton effect is first studied in the case of a completely coherent interaction between QW excitons and bulk photons, i.e. in the so called strong coupling limit. Then, an incoherent damping rate for the exciton states is included and the resulting modifications in the polariton dispersion are analyzed. A microscopic model which accounts for the scattering of QW excitons by random impurities is also proposed. In the strong coupling limit, a definitive and correct description of the QW polariton dispersion, for both confined and radiative modes, is obtained when the exciton- photon coupling is treated non perturbatively. A self-consistent perturbation theory which qualitatively agrees with the obtained results is also formulated. With increasing the incoherent damping, the orthogonality between radiative and confined polariton states is not affected, but a phase transition from the strong coupling regime to a weak coupling one occurs for both modes. The crossover between the two regimes is attributed to a topological change of the polariton dispersion curves when the damping rate reaches a critical value. A microscopic approach dealing with scattering of excitons by random impurities is formulated in terms of a quadratic Hamiltonian for QW excitons, bulk photons and localised impurities. By analyzing the preliminary results based on the calculation of the relevant eigenstates, the mixing between radiative and confined modes is observed.EThOS - Electronic Theses Online ServiceGBUnited Kingdo

Ellipsometric Porosimetry for the Microstructure Characterization of Plasma-Deposited SiO2-Like Films

SiO2 layers have been deposited from Ar/O2/hexamethyldisiloxane mixtures in a remote expanding thermal plasma setup enabling a good control of both the ion flux (by changing the deposition chemistry and the arc plasma parameters) as well as the ion energy. This latter is achieved by an additional rf substrate biasing or a tailored ion biasing technique, i.e. a low frequency pulse-shaped bias. The role of the ion energy and ion-to-growth flux ratio on the film microstructure and densification at low substrate temperature (100ºC) has been investigated by means of ellipsometric porosimetry. This technique monitors the refractive index change due to the adsorption (and desorption) of ethanol vapors in the volume of macro-meso-micro pores in the SiO2 layer. From the analysis of the adsorption isotherm and the presence of hysteresis during the desorption step as a function of the equilibrium partial pressure, the open porosity in the layer can be determined. It is found that both biasing techniques lead to densification of the deposited layer, which experiences a transition from micro-/ mesoporosity to microporosity and eventually non-porosity, as function of the increasing ion energy. Although both biasing techniques lead to a comparable critical ion energy value per deposited SiO2 unit (about 100 eV), the ion-to-growth flux ratio and ion energy are not found to be interchangeable parameters. In fact, in the case of the rf bias, the meso- and large micropores are first affected leading to a quantitative decrease of porosity, i.e. from 11% to 3% at an ion energy less than 20 eV. A further increase in ion energy eventually reduces the presence of smaller micropores leading to non porous films at energy of 45 eV. When the pulse-shaped biasing technique is adopted, the micro- and mesopores are simultaneously affected over the whole range of available ion energy, leading to a non porous layer only at very high energy values, i.e. 240 eV. This difference is attributed to the increasing ion-to-growth flux ratio accompanying the rf biasing, as a consequence of the rf plasma generation in front of the substrate

Quantum well polaritons: Strong and weak coupling regimes

The work described in this thesis is a theoretical investigation of the properties of exciton-polaritons in quantum wells (QWs). The polariton effect is first studied in the case of a completely coherent interaction between QW excitons and bulk photons, i.e. in the so called strong coupling limit. Then, an incoherent damping rate for the exciton states is included and the resulting modifications in the polariton dispersion are analyzed. A microscopic model which accounts for the scattering of QW excitons by random impurities is also proposed. In the strong coupling limit, a definitive and correct description of the QW polariton dispersion, for both confined and radiative modes, is obtained when the exciton- photon coupling is treated non perturbatively. A self-consistent perturbation theory which qualitatively agrees with the obtained results is also formulated. With increasing the incoherent damping, the orthogonality between radiative and confined polariton states is not affected, but a phase transition from the strong coupling regime to a weak coupling one occurs for both modes. The crossover between the two regimes is attributed to a topological change of the polariton dispersion curves when the damping rate reaches a critical value. A microscopic approach dealing with scattering of excitons by random impurities is formulated in terms of a quadratic Hamiltonian for QW excitons, bulk photons and localised impurities. By analyzing the preliminary results based on the calculation of the relevant eigenstates, the mixing between radiative and confined modes is observed