A theoretical model describing photophysics of π-conjugated aggregates, such as molecular crystals and polymer thin films, is developed. A Holstein-like Hamiltonian expressed with a multi-particle basis set is used to evaluate absorption and photoluminescence (PL) spectra. An analysis with line strength ratio proves to be a powerful diagnostic tool to obtain additional spectral signatures with which to distinguish H- vs. J-aggregation. For the H-aggregates absorption peak ratio, A0-0/A0-1, diminishes as the excitonic coupling increases. Also the PL peak ratio, I0-0/I0-1, is zero at T=0K with no disorder and the value increases as temperature and disorder increase. By contrast the J-aggregates show the opposite trends. Furthermore we will show the PL peak ratio provides a direct measurement of the exciton coherence length for a linear J-aggregate and could be expressed as I0-0/I0-1 = Ncoh/l2. We will also show that it is inversely proportional to square root of temperature (T-1/2). Applying our theory to the herringbone style oligoacene molecular crystals, we show the lowest singlet exciton states are highly influenced by charge transfer (CT) states and the well known energetic gap in two polarized absorption spectra, so called Davydov Splitting (DS), is a product of the interaction. We have successfully reproduced the DS for all three oligoacenes without any free parameters. Inspired by the CT contribution in oligoacene crystals, we further develop Wannier-Mott exciton model and apply to disorder-free polydiacetylene (PDA) quantum wires, which have been shown to be extremely emissive. We will show the quantum wire is a J-aggregate and we once again derive the peak ratio and the coherence size relation, I0-0/I0-1 = kNcoh/l2, where k is a prefactor close to unity. Typical photophysical properties of polymer p-stacks such as those occurring in P3HT films are well explained by the simple linear H-aggregate model. However several groups have started seeing more J-like behaviors amongst “improved” (less disordered) polymer films such as increased values of A0-0/A0-1 and I0-0/I0-1 and higher radiative rates. With the new perception of a single polymer chain being a J-aggregate, we apply our new theory to p-stack of polymer chains. We call this HJ-aggregate model since the interchain interaction induces H-aggregation. In the study we show a competition between intrachain and interchain interactions that leads to unique photophysical features. The new model is capable of explaining a wide range of polymer systems and most importantly the theory uncovers the mechanism of the improved polymer films; reducing disorder urges increasing intrachain reactions within each chain, thus enhancing more J-like spectral features. / Chemistry

Currently, there is a great interest towards developing organic semiconductors for use in solar cells and lighting displays. Derivatives of one of the most important chromophores, diketopyrrolopyrrole (DPP), are commonly employed as the active material in field-effect transistors, as they exhibit high hole mobilities. The intramolecular structure of 2T-DPP-2T with four thiophene units(T) is classified as a donor-acceptor-donor (DAD) chromophore, where the bithiophene units are donors and the DPP unit is the acceptor. The absorption spectrum of the aggregated form of a polymer based on the 2T-DPP-2T repeat units in 1,1,2,2-tetrachloroethane solution (TCE) was measured by Janssen et. al. The spectrum is red-shifted relative to a unaggregated polymer, which is an identifying feature of a J-aggregate. In addition, the ratio of the first two vibronic peaks decreases substantially in going from the unaggregated phase to the aggregate, which is an identifying feature of an H-aggregate. These contradicting behaviors were also observed by Punzi et. al. for an aggregate of the 2T-DPP-2T chromophore. Such behavior cannot be explained by the classical Frenkel-Holstein model. One challenge has been that the intermolecular charge transfer (ICT) plays an important role in the absorption and emission spectrum in the molecular aggregates of DPP. The bulk of this thesis has been to expand the Frenkel-CT-Hosltein model to include intramolecular and intermolecular charge transfer. The model accounts unusual red-shifted H-aggregates observed in the experiments. The experimental spectra of two different DPP-based chromophores are successfully reproduced with our theoretical model. Furthermore, based on perturbative expression for ICT coupling, an effective Frenkel Holstein (EFH) model is proposed and employed to successfully simulate the absorption and emission spectrum of DPP4T aggregates, as long as charge-transfer coupling is smaller than the energy gap between the Frenkel- and ICT excitations. The emission spectrum of DPP4T is also successfully reproduced by this new model, including the temperature dependence. / Chemistry

<p dir="ltr">Understanding the fundamentals of exciton transport is essential to better inform the design and application of quantum dot superlattices (QDSLs) in light harvesting systems. Exciton transport is subject to a complex energy landscape where the forces that govern delocalization distances are a result of the wavefunction of the exciton and environmental incoherent forces. By changing the temperature of the surroundings, the exciton will transition between two motivating transport methods: a wave-like ballistic method of diffusion and a particle-like Brownian method of diffusion. Mixing these regimes of transport demonstrates how ENAQT can motivate a maximum amount of transport at an intermediate temperature. This thesis examines measurements made on CsPbBr₃ QDSLs, demonstrating the difference between these two transport mechanisms and the role of dimensionality on the ability of excitons to transport.</p>

As traditional solar technologies approach theoretical efficiency limits, novel approaches are necessary to continue to improve the power generation capacity of photovoltaics. Two complementary multiexcitonic processes, singlet fission (SF) and triplet-triplet annihilation upconversion (TTA-UC), show great promise in this field, allowing access to regions of the solar spectrum inefficiently harvested by silicon cells. In designing and optimizing systems for SF and TTA-UC, macromolecular scaffolds are particularly attractive, enabling the simultaneous tuning of electronic coupling between chromophores as well as their intermolecular packing. The high modularity of these scaffolds allows for easy adjustment of component ratios or the introduction of new units to further adjust dynamics or morphology. As such, macromolecular systems have also been employed in various condensed and solid phase systems which may more readily be incorporated into photovoltaics. Herein, we expand the scope of macromolecular architectures to new domains for SF and TTA-UC. In Chapter 1, we summarize the guiding principles for the optimization of these processes, and follow with a discussion of existing oligomeric, macromolecular, and self-assembled systems. In Chapter 2, an amphiphilic block copolymer (BCP) is introduced to explore SF in self-assembled micelles. We find that SF dynamics can be controlled by modifying BCP block ratios, as well as by co-assembly with a variety of dopants. In Chapter 3, this amphiphilic BCP scaffold is adapted to TTA-UC, and we highlight the importance of micellar swelling in enabling this process. In Chapter 4, electron donors are incorporated into polymers alongside pendent SF chromophores to explore both intra- and intermolecular charge transfer. We observe the formation of long-lived charge separated states prompted by SF, with dynamics tunable by solvent polarity, donor strength, and mode of interaction. And in Chapter 5, a series of hetero-oligomers are presented to explore SF at interfaces between classic acenes and the less-studied dipyrrolonaphthyridinedione. We reinforce the essential role of charge transfer states in mediating or deactivating singlet fission in a tunable fashion based on chromophore energetics. In sum, this work further demonstrates the essential role macromolecular engineering will play in the continued development of SF and TTA-UC.

Strong resonant dipole-dipole interactions in flexible Rydberg aggregates enable the formation of excitons, many-body states which collectively share excitation between atoms. Exciting the most energetic exciton of a linear Rydberg chain whose outer two atoms on one end are closely spaced causes the initiation of an exciton pulse for which electronic excitation and diatomic proximity propagate directed through the chain. The emerging transport of excitation is largely adiabatic and is enabled by the interplay between atomic motion and dynamical variation of the exciton. Here, we demonstrate the coherent splitting of such pulses into two modes, which induce strongly different atomic motion, leading to clear signatures of nonadiabatic effects in atomic density profiles. The mechanism exploits local nonadiabatic effects at a conical intersection, turning them from a decoherence source into an asset. The conical intersection is a consequence of the exciton pulses moving along a linear Rydberg chain and approaching an additional linear, perpendicularly aligned Rydberg chain. The intersection provides a sensitive knob controlling the propagation direction and coherence properties of exciton pulses. We demonstrate that this scenario can be exploited as an exciton switch, controlling direction and coherence properties of the joint pulse on the second of the chains. Initially, we demonstrate the pulse splitting on planar aggregates with atomic motion one-dimensionally constrained and employing isotropic interactions. Subsequently, we confirm the splitting mechanism for a fully realistic scenario in which all spatial restrictions are removed and the full anisotropy of the dipole-dipole interactions is taken into account. Our results enable the experimental observation of non-adiabatic electronic dynamics and entanglement transport with Rydberg atoms. The conical intersection crossings are clearly evident, both in atomic mean position information and excited state spectra of the Rydberg system. This suggests flexible Rydberg aggregates as a test-bench for quantum chemical effects in experiments on much inflated length scales. The fundamental ideas discussed here have general implications for excitons on a dynamic network.

La compréhension des interrelations entre la microstructure et les processus électroniques dans les polymères semi-conducteurs est d’une importance primordiale pour leur utilisation dans des hétérostructures volumiques. Dans cette thèse de doctorat, deux systémes diffèrents sont étudiés ; chacun de ces systèmes représente une approche diffèrente pour optimiser les matériaux en termes de leur microstructure et de leur capacité à se mettre en ordre au niveau moléculaire. Dans le premier système, j’ai effectué une analyse complète des principes de fonctionnement d’une cellule photovoltaïque hybride à base des nanocristaux d’oxyde de zinc (ZnO) et du poly (3-hexylthiophène) (P3HT) par absorption photoinduite en régime quasi-stationnaire (PIA) et la spectroscopie PIA en pompage modulé dépendant de la fréquence. L’interface entre le donneur (le polymère P3HT) et l’accepteur (les nanoparticules de ZnO), où la génération de charges se produit, joue un rôle important dans la performance des cellules photovoltaïques hybrides. Pour améliorer le mécanisme de génération de charges du P3H: ZnO, il est indispensable de modifier l’interface entre ses constituants. Nous avons démontré que la modification d’interface moléculaire avec cis-bis (4, 40 - dicarboxy-2, 20bipyridine) ruthénium (II) (N3-dye) et a-Sexithiophen-2 yl-phosphonique (6TP) a améliorée le photocourant et la performance dans les cellules P3HT: ZnO. Le 6TP et le N3 s’attachent à l’interface du ZnO, en augmentant ainsi l’aire effective de la surface donneur :accepteur, ce qui contribue à une séparation de charge accrue. De plus, le 6TP et le N3 réduisent la densité de pièges dans le ZnO, ce qui réduit le taux de recombinaison des paires de charges. Dans la deuxième partie, jai introduit une matrice hôte polymérique de polystyréne à masse molaire ulra-élevée, qui se comporte comme un solide pour piéger et protéger une solution de poly [2-méthoxy, 5- (2´-éthyl-hexoxy) -1,4-phénylènevinylène- PPV] (MEHPPV) pour utilisation dans des dispositifs optoèlectroniques quantiques. Des travaux antérieurs ont montré que MEH-PPV en solution subit une transition de conformation, d’une conformation enroulé à haute température (phase bleue) à une conformation de chaîne étendue à basse température (phase rouge). La conformation de la chaîne étendue de la solution MEH-PPV favorise les caractéristiques nécessaires à l’amélioration des dispositifs optoélectroniques quantiques, mais la solution ne peut pas être incorporées dans le dispositif. J’ai démontré que la caractéristique de la phase rouge du MEH-PPV en solution se maintient dans une matrice hôte polymérique de polystyrène transformé de masse molaire très élevée, qui se comporte comme un solide (gel de MEH-PPV/UHMW PS), par le biais de la spectroscopie de photoluminescence (PL) dépendant de la température (de 290K à 80 K). La phase rouge du gel MEH-PPV/UHMW PS se manifeste par des largeurs de raie étroites et une intensité augmentée de la transition 0-0 de la progression vibronique dans le spectre de PL ainsi qu’un petit décalage de Stokes entre la PL et le spectre d’absorption à basse température. Ces approches démontrent que la manipulation de la microstructure et des propriétés électroniques des polymères semi-conducteurs ont un impact direct sur la performance de dispositifs pour leurs développements technologiques continus. / Understanding the interrelations between microstructure and electronic processes in polymeric semiconductors is of great importance for their use in bulk heterostructures, as the active part of power-converting devices such as organic photovoltaic cells or light emitting diodes, as well as for quantum optoelectronics applications. In this doctoral thesis, two different systems are investigated; each of these systems represents a different approach to optimize materials in terms of microstructure and their ability to order on the molecular level. In the first system, by means of quasi-steady-state photoinduced absorption (PIA) and pump-modulation-frequency-dependent PIA spectroscopy, I performed a comprehensive analysis of the working principles of a hybrid photovoltaic cell based on nanocrystals of zinc oxide (ZnO) and poly(3-hexylthiophene) (P3HT). The interface surface area between donor (polymer P3HT) and acceptor (ZnO nanocrystals), where charge generation occurs, plays a significant role in the performance of the hybrid photovoltaic cells. To improve the charge generation mechanism of P3HT: ZnO, it is therefore essential to modify the P3HT: ZnO interface area. We demonstrated that molecular interface modification with cis-bis(4,40-dicarboxy-2,20bipyridine) ruthenium (II) (N3-dye) and a-Sexithiophen-2-yl-phosphonic Acid (6TP) as interface modifiers enhanced the photocurrent and performance in P3HT: ZnO cells. 6TP and N3 attach to the ZnO interface, thus increasing the donor:acceptor interface area that contributes to enhanced charge separation. Furthermore, 6TP and N3 reduce the ZnO traps that reduces recombination. In the second part, I introduced a processed solid-like ultra-high-molecular-weight polystyrene polymeric host matrix to trap and protect poly [2-methoxy, 5-(2’-ethylhexoxy)- 1,4-phenylene vinylene-PPV] (MEH-PPV) solution for use in quantum optoelectronic devices. Previous work by others has shown that MEH-PPV in solution undergoes a conformation transition from coiled conformation at high temperatures (blue-phase) to a chain-extended conformation at low temperatures (red-phase). The chain-extended conformation of MEH-PPV solution favours the characteristics needed to improve quantum optoelectronic devices, however the solution cannot be incorporated into the device. We demonstrated that the red-phase feature of MEH-PPV in solution maintains in a processed solid-like ultra-high-molecular-weight polystyrene polymeric host matrix (MEH-PPV/UHMWPS gels), by means of temperature-dependent photoluminescence (PL) spectroscopy (ranged from 290K down to 80 K). The red-phase of MEH-PPV/UHMW PS gels manifest itself as narrow linewidths and enhanced 0-0 line strength in the PL spectrum as well as a small stokes shifts between the PL and absorption spectra at low temperatures. These approaches demonstrate that microstructure manipulation and electronic properties of polymeric semiconductors have a direct impact on the device performance for their continued technological developments.

Ce manuscrit est consacré à la physique des polaritons dans deux matériaux semiconducteurs à grand gap : ZnO et GaN. Les paramètres polaritoniques de ces matériaux ont été déterminés avec précision grâce à une étude combinant différentes techniques spectroscopiques linéaires et non-linéaires (réflectivité continue, autocorrélation, photoluminescence et mélange à quatre ondes dégénérées). L’interprétation de ces résultats conduit à une meilleure compréhension des processus d’interaction au sein du semiconducteur : le rôle important des interactions polariton-phonon LO dans l’élargissement polaritonique a notamment pu être mis en évidence. Ce travail effectué sur des échantillons massifs est indispensable pour mener au mieux l’étude de l’effet laser à polaritons dans des microcavités présentée dans la seconde partie de ce manuscrit. Pour cette étude, deux microcavités massives semblables, une à base de ZnO l’autre de GaN, ont été réalisées. Les qualités photoniques de ces structures sont à l’état de l’art : elles présentent un bon facteur de qualité (Q ≈ 1000) et un faible désordre photonique. Le régime de couplage fort ainsi que l’effet laser à polaritons sont observés jusqu'à température ambiante. Enfin, l’établissement de diagrammes de phases permet de mettre en exergue le rôle important des phonons LO dans l’abaissement du seuil laser. / This manuscript is devoted to the physics of polaritons in two wide band gap semiconductor : ZnO and GaN. The polaritonic parameters of these materials have been accurately determined through a study which combines linear and non-linear spectroscopies (continuous reflectivity, autocorrelation, photoluminescence and degenerate four-wave mixing). The interpretation of these results lead to a better understanding of the interaction processes in the semiconductor : the important role played by the polariton-LO phonon interactions in the polaritonic damping is highlighted and particularly for ZnO. This preliminary work on bulk samples is essential for a suitable study of polariton lasing in microcavities like it is presented in the second part of this manuscript. For this study, two similar microcavities, one based on ZnO and another on GaN. The photonic properties of these structures are at the state of the art : they have a good quality factor (Q ≈ 1,000) and have a low photon disorder. The strong coupling regime and the polariton lasing are observed to room temperature. Finally, the establishment of phase diagrams allows to highlight the important role of LO phonons in reduction of the laser threshold.

Orientador: Gilberto Medeiros Ribeiro / Tese (doutorado) - Universidade Estadual de Campinas, Instituto de Fisica Gleb Wataghin / Made available in DSpace on 2018-08-09T10:48:50Z (GMT). No. of bitstreams: 1 GonzalezHernandez_FelixGuillermo_D.pdf: 12837677 bytes, checksum: 70e82c96ea88ab1de4fa785d908c9af6 (MD5) Previous issue date: 2007 / Resumo: Medidas experimentais foram realizadas para determinar as escalas de tempo de relaxação e decoerência do spin eletrônico como bit quântico. A estrutura dos estados de exciton foi investigada com o objetivo de servir como estados intermediários na manipulação do spin. O sistema utilizado para o estudo de decoerência é um ensemble de pontos quânticos auto-formados semicondutores. Dois temas servem como eixos centrais dos três experimentos desenvolvidos nesta tese: a polarização de spin e o fator g de Landé. No primeiro experimento, ao incluir o efeito do reservatório térmico, foi obtido o grau de polarização do spin (populações dos níveis up e down) para as camadas s e p. O desdobramento dos níveis orbitais em subníveis de spin permitiu obter a magnitude do fator g para estes estados. Mudando a orientação do campo magnético, foram observadas as anisotropias do tensor g e a sua relação com os detalhes do potencial de confinamento. Estas características permitiram inferir o tempo de relaxação T1. A medida da polarização resolvida no tempo foi realizada através de es-pectroscopia óptica de bombeio-prova. Os pulsos de luz e o campo magnético transverso permitem que uma polarização líquida seja inicializada. A rotação de Kerr permitiu observar oscilações desta polarização em torno do campo magnético com freqüência determinada pelo fator g. A perda da coerência de fase do spin resulta no decaimento destas oscilações numa escala de tempo T2. Medidas realizadas num ensemble de spins implicam em que o tempo de decoerência encontra-se limitado pela escala de defasagem T¤2< T2. Uma técnica semelhante à refocalização por spin-eco em experimentos de ressonância magnética nuclear, foi aplicada utilizando pulsos de laser para reverter a defasagem do ensemble. Tanto a possibilidade de medir o sinal de eco como o tempo de decoerência foram medidos como função da temperatura. A estrutura de níveis de exciton e a sua distribuição no ensemble foi estudada também com espectroscopia de bombeio-prova. Foram observados batimentos quânticos entre os níveis de estrutura fina do exciton para sis-temas 0D e 2D limitados pelo tempo de recombinação / Abstract: Experimental measurements were carried out to determine the scales of the relaxation and decoherence time for the electronic spin as quantum bit. The structure of the exciton states was investigated with the objective to serve as intermediate states in the spin manipulation. The system studied for the implementation of the quantum computation is an ensemble of self-assembled semiconductor quantum dots. Two subjects serve as central axes of the three experiments developed in this thesis: the spin polarization and the Landé g-factor. In the first experiment, when including the effect of the thermal reservoir, the degree of spin polarization (populations for the up and down levels) was measured for layers s and p. The splitting of the orbital levels in spin sublevels allowed to get the magnitude of factor g for these states. Changing the orientation of the magnetic field, the g-tensor anisotropies and its relation with the details of the confinement potential had been observed. These characteristics had allowed to infer the relaxation time T1. The time resolved polarization measurement was carried out by optical pump-probe spectroscopy. The pulses of light and the transverse magnetic field allow the initialization of a net polarization. The Kerr rotation allowed to observe oscillations of this polarization around the magnetic field with frequency determined for factor g. The loss of the spin phase coherence results in the decay of these oscillations in a time scale T2. Measurements carried out in an ensemble of spins imply that the decoherence time is limited by the ensemble dephasing time T¤2 < T2. A technique similar to the spin-echo refocalization in nuclear magnetic resonance experiments using laser pulses was applied to reverse the ensemble dephasing. The possibility to measure the echo signal and the decoherence time was measured as a function of the temperature. The structure of exciton levels and its distribution in ensemble were also studied with pump-probe spectroscopy. Quantum beats were observed be-tween the fine structure exciton levels for 0D and 2D systems, yet limited by the recombination time / Doutorado / Física da Matéria Condensada / Doutor em Ciências

Cette thèse est consacrée à l’étude expérimentale des propriétés magnéto-optiques intrinsèques des nanotubes de carbone mono-paroi par spectroscopie de photoluminescence résolue en temps.Un dispositif de microscopie optique confocale de grande ouverture numérique (NA = 0.95),incluant un cryostat magnétique, permet l’étude de nanotubes suspendus à l’échelle individuelle,à température cryogénique (jusqu’à 2 Kelvin) et sous champ magnétique (jusqu’à 7 Tesla). L’évolution des spectres et des déclins de photoluminescence avec le champ magnétique montre l’influence de l’effet Aharonov-Bohm sur les deux excitons singulets de plus basse énergie, c’est à-dire l’exciton fondamental qui est optiquement inactif (exciton noir) et un exciton d’énergie supérieure séparé de quelques milliélectronvolts qui est optiquement actif (exciton brillant). L’interprétation de ces résultats à partir d’un modèle d’équations de taux qui intègre le couplage Aharonov-Bohm entre ces deux excitons permet de déterminer séparément les durées de vie excitoniques et de fournir des informations quantitatives sur la relaxation de l’énergie depuis les niveaux supérieurs photo-excités. La relaxation de l’énergie suite à la photo-excitation de la transition S22 conduit à une efficacité de peuplement de l’état brillant quatre fois plus faible que celle de l’état noir, mais qui augmente significativement lorsque la relaxation se produit depuis les niveaux excitoniques KK’. D’autre part, le bon rapport signal à bruit obtenu dans les spectres de photoluminescence permet de révéler l’existence d’un couplage intrinsèque en champ nul entre l’exciton noir et l’exciton brillant ainsi que le maintien de la mobilité excitonique dans les nanotubes suspendus à la température de l’hélium liquide. / This thesis is dedicated to the experimental study of the intrinsic magneto-optical properties of single-walled carbon nanotubes through time-resolved photoluminescence spectroscopy. Measurements are performed on suspended nanotubes samples at the single-object level using a home-built confocal optical microscope with a large numerical aperture (NA = 0.95) operating at cryogenic temperature (down to 2K) and high magnetic field (up to 7T). The evolution of the photoluminescence spectra and decay signals with increasing magnetic fields shows the influence of the Aharonov-Bohm effect on the two lowest-energy singlet excitons, namely the ground exciton which is optically inactive (dark exciton) and an exciton lying a few millielectron volts higher in energy which is optically active (bright exciton). A model of these results based on rate equations and including the Aharonov-Bohm coupling between these two excitons enables to determine separately the excitons lifetimes and to derive quantitative information on the energy relaxation from the photo-excited higher levels. The energy relaxation following the photo-excitation of the S22 transition leads to a bright state population efficiency four times lower than that of the dark state, but it significantly increases when energy relaxation occurs from the KK’ excitonic levels. Thanks to a good signal to noise ratio, the photoluminescence spectra also reveal the presence of an intrinsic zero-field coupling between the dark and the brightexcitons, as well as an excitonic mobility preserved at liquid helium temperature in suspended nanotubes.

Cette thèse est consacrée à de nouveaux phénomènes en physique liées au spin et à la topologie des quasi-particules lumière-matière dans des hétérostructures. Elle est divisée en quatre parties. Chapitre 1 donne un fond nécessaire et introduit les propriétés fondamentales des polaritons et des excitons indirects dans des puits quantiques couplés. Chapitre 2 est concentré sur la dynamique de spin et sur formation de défauts topologiques dans des systèmes aux excitons indirects. Les 2 derniers chapitres considèrent les structures basées sur les microcavités. Chapitre 3 est consacré à la dynamique de spin des polaritons dans des oscillateurs paramétriques optiques. Finalement, chapitre 4 étudie les réseaux des microcavités en forme des piliers et introduit l’isolant topologique polaritonique. / The present thesis manuscript is devoted to new phenomena in physics of light-matter quasiparticles in heterostructures, related to spin and topology. It is divided into four parts. Chapter 1 gives a necessary background, introducing basic properties of microcavity polaritons and indirect excitons in coupled quantum wells. Chapter 2 is focused on spin dynamics and topological defects formation in indirect exciton many-body systems. The last 2 chapters are related to microcavity-based structures. Chapter 3 is devoted to polariton spin dynamics in optical parametric oscillators. Finally, Chapter 4 studies pillar microcavity lattices and introduces the polariton topological insulator.