Dissertations / Theses on the topic 'Photo-induced charge'

The electronic material graphene has attracted much attention for its unique physical properties such as, linear band structure, high electron mobility, and room temperature ballistic conduction. The possibilities for device applications utilizing graphene show great variety, from transistors for computing to chemical sensors. Yet, there are still several basic physical properties such as thermal conductivity that need to be determined accurately. This work examines the thermal properties of graphene grown by the chemical vapor deposition technique. The thermoelectric power of graphene is studied in ambient and vacuum environments and is shown to be highly sensitive to surface charge doping. Exploiting this effect, we study the change in thermoelectric power due to introduction of gaseous species. The temperature dependent thermal conductivity of graphene is measured using a comparison method. We show that the major contribution to the thermal conductivity is the scattering of in-plane phonons. Graphene also shows promise as an optoelectronic material. We probe the Landau level structure of graphene in high magnetic fields using a differential photoconductivity technique. Using this method we observed the lifting of spin and valley degeneracies of the lowest Landau level in graphene.

Polymer-fullerene blend films are of increasing interest in the field of organic solar cells. This thesis describes the use of transient absorption spectroscopy (TAS) as a means to study charge generation and recombination in these blend films. In blend films of P3HT and PCBM, the absorption spectrum associated with the positive and negative charges have been identified and the transient decay kinetics analysed to reveal the mechanisms leading to charge recombination losses in the films. The effects of annealing treatment, along with the effects of decreasing polymer regioregularity or different polymer chain terminating end-groups on the blend film properties and morphology are also discussed. For films with a low concentration of PCBM in polystyrene, absorption and emission from the individual PCBM molecules are observed. As the PCBM concentration is increased, aggregation related changes causes the absorption in the visible region to increase disproportionately, an additional emission peak at higher energies to appear and a decrease in the lifetime of the PCBM triplet excited state. These changes are linked to electronic interactions between fullerenes in a molecular crystal form of PCBM. Blends of F8BT polymer with PCBM show poor photovoltaic device performance. This is explained by the quick deactivation of the F8BT excited state by Förster energy transfer to the PCBM. As the PCBM excited state is stable compared to the charge separated state, the PCBM triplet is formed via inter-system crossing from the singlet to be the final product of photoexcitation. The high energy of the charge separated state is interpreted as a result of the high F8BT HOMO energy.

En esta tesis doctoral se han estudiado procesos fundamentales de reacciones de transferencia de carga en películas mesoporosas de dióxido de titanio sensitivizado con puntos cuánticos, en películas finas de mezclas polímero:puntos cuánticos y en dispositivos completos de mezclas del polímero PCPDTBT y puntos cuánticos de CdSe en operaciones de trabajo reales. Los resultados obtenidos permiten abordar la fabricación de dispositivos fotovoltaicos con un conocimiento de los procesos de recombinación que limitan la eficiencia de las celdas más amplio. Y por tanto, se demuestra la posibilidad de fabricar celdas solares basadas en puntos cuánticos con eficiencias iguales o superiores a los dispositivos fotovoltaicos orgánicos.
The fundamental processes of the charge transfer reactions between titania dioxide mesoporous films and quantum dots, in blend films of the semiconductor polymer P3HT and CdSe quantum dots and in complete devices fabricated with the polymer PDPCTBT and CdSe quantum dots in working conditions have been studied in this doctoral thesis. The obtained results allow the fabrication of photovoltaic devices with a deeper and wider knowledge of the recombination processes that limit the device efficiency. Therefore, it is demonstrated the possibility of fabrication of quantum dot based solar cells with efficiencies similar or higher than the organic photovoltaic devices.

Le travail de thèse porte sur les méthodes de synthèse de nanostructures de dioxyde de titane et de leurs études physicochimiques afin de préciser les corrélations entre la morphologie, le dopage métallique, les caractéristiques structurales avec l'efficacité photocatalytique. Le grand intérêt pour les nanomatériaux TiO2 réside dans la mise au point de nouvelles sources d'énergie ou la conservation de l’environnement par des processus photocatalytiques. Cependant, la limitation principale de TiO2 est du au large gap électronique (eV ~3,2) du polymorphe Anatase. Ainsi, un des objectifs importants pour l'amélioration de l’efficacité des nanomatériaux TiO2 est d'augmenter leur photoactivité en décalantla création de paires d'électron-trou de l’UV à la gamme du visible. D'ailleurs, on a montré que l'utilisation de nanostructures 1D de TiO2 (nanotubes) a amélioré la collection de charges, en favorisant leur transport dans les structures 1D, qui par conséquent réduit au minimum la recombinaison et prolonge les durées de vie des électrons.La première partie de ce travail est dédiée à la synthèse des nanopoudres TiO2 dopées par des ions métalliques (Ag, Cu, Eu) préparés par sol-gel. Même avec différents éléments de dopage qui apparemment peuvent adopter le même état de valence (2+) (Cu2+, Ag2+, Eu2+), différents comportements ont été démontrés pour l'incorporation efficace de ces ions dans la structure de TiO2. L'anomalie entre les rayons ioniques des différents éléments utilisés module le rapport du dopage substitutionnel. Ceci est en effet réalisé pour Cu2+ mais dans moins d'ampleur pour Ag2+ tandis que les ions d'europium forment une ségrégation de phase Eu2Ti2O7. La dégradation de colorants de bleu de méthylène (MB) a étéaméliorée légèrement avec les échantillons dopés Ag. La raison a été attribuée aux clusters métalliques Ag qui ont été en effet mis en évidence à travers leur bande d’absorption plasmonique. La deuxième partie porte sur des couches minces de TiO2 dopés (Cu, Ag, et Eu) qui ont été élaborés par sol-gel et spin-coating et dipcoating. Les paramètres optimaux ont été obtenus pour réaliser les films cristallins mais présentant une organisation mésoporeuse qui dépend également du processus de dopage. Des études de Photocatalyse ont été également réalisées et l'efficacité des films ont été comparées en fonction des éléments dopants. La troisième partie de la thèse est liée à la modification morphologique des nanoparticules pour former des nanotubes à l'aide de la méthode hydrothermale sous pression contrôlée. Un plan d'expérience basé sur la méthode Taguchi a été utilisé pour la détermination des paramètres optimaux.Les nanotubes TiO2 augmentent la surface spécifique en comparaison avec les nanoparticules. La dégradation de bleu deméthylène par les nanotubes a montré une efficacité photocatalytique plus élevée qu’avec les nanopoudres TiO2 pures etdopés Ag
The thesis work is focused on the synthesis methods of titanium dioxide nanostructures and their physico-chemical studies in order to point out the correlations between the morphology, metal doping, structural features with the photocatalytic efficiency. The great interest on TiO2 nanomaterials deals with new sources of energy or in the environment preservation through the photocatalytic properties. However, the main limitations is due to the wide band gap (~3.2 eV) of the anatase polymorph. Thus, a major objective for improvement of the performance of TiO2 nanomaterials is to increase theirphotoactivity by shifting the onset of the electron-hole pairs creation from UV to the visible range. Moreover, it was found that using onedimensional (1-D) TiO2 (nanotubes) improved the charge collection by 1D nanostructures which consequently minimizes the recombination and prolongate the electron lifetimes. The first part of this work is focused on the synthesis of TiO2 nanopowders doped with metallic ions (Ag, Cu, Eu) prepared by Solgel. Even with different doping elements which apparently can adopt the same valence state (2+) such as (Cu2+, Ag2+,Eu2+), different behaviors were demonstrated for the effective incorporation of these ions in the host structure of TiO2. The discrepancy between ionic radii of the different used elements modulates the ratio of the substitutional doping. This is indeed achieved for Cu2+ but in less extent for Ag2+ while Europium ions form segregated phase as Eu2Ti2O7. The experiments on the degradation of methylene blue (MB)dyes have shown slight improvement with Ag-doped samples. The reason was tentatively attributed to the Ag clusters which were indeed demonstrated through their plasmon optical band. The second part of the work concerns thin films of TiO2 doped (Cu, Ag, and Eu) which were elaborated by spin coating and dip coating. The optimal parameters were obtained to achieve crystalline films but presenting mesoporous organisation which also depends on the doping process. Photocatalysis investigations were also realized and the efficiency of the films compared as function of the doping elements.The third part of the thesis is related to the morphological modification from nanoparticles to nanotubes by using the hydrothermal method with controlled pressure. An experimental design based on Taguchi Method was employed for the determination of the optimal parameters. TiO2 nanotubes increase the surface area in comparison with TiO2nanoparticles. TiO2 nanotubes were tested for the methylene blue degradation and show a higher photocatalytic efficiency than TiO2 nanopowders and TIO2 doped with Ag

Der Gegenstand der vorliegenden Arbeit ist die Untersuchung von photoinduzierten Energietransferprozessen (EET) und Elektronentransferprozessen (ET) in Modellsystemen, die als potentiell geeignet für eine Nutzung in der artifiziellen Photosynthese angesehen werden. Den beiden wesentlichen Zugängen zur Architektur artifizieller Photosynthese-Systeme entsprechend wurden vergleichend kovalente und sich selbst organisierende Systeme untersucht. In beiden Zugängen wurden ähnliche chemische Komponenten als optisch aktive Moleküle eingesetzt, insbesondere Phthalocyanine mit einem Silizium-Zentralatom (SiPc). Durch eine Kombination von stationären und zeitaufgelösten optisch-spektroskopischen Methoden konnten die lichtinduzierten ET- und EET-Prozesse identifiziert und quantifiziert werden. Im ersten Teil der Arbeit wurden mehrere kovalent gebundene Triaden und eine Pentade untersucht. In allen Systemen finden sehr effiziente ET und EET Prozesse statt. Es wurde gezeigt, dass das Lösungsmittel großen Einfluss auf die photophysikalischen Eigenschaften der Systeme ausübt. Die Lebensdauer des ladungsseparierten Zustandes variiert von 1,7 ns in Toluol bis 30 ps in DMF. Im zweiten Teil der Arbeit wurde erstmals gezeigt, dass sich in wässriger Lösung ein supramolekularer Komplex, bestehend aus einem Beta-Cyklodextrin (CD), einem konjugierten Subphthylocyanin (SubPc), einem Porphyrin (Por) und einem SiPc bilden kann. Letzteres wurde über unterschiedliche Ketten an zwei CDs kovalent gebunden. Die Selbstorganisation wird über hydrophobe Wechselwirkungen vermittelt und die Bildung der Komplexe ist sehr effizient. Nach selektiver Anregung von SubPc finden sequenzielle ET- und EET-Prozesse von SubPc zu SiPc statt. Das Por spielt die Rolle einer energetischen und elektronischen Brücke und ermöglicht die ET und EET-Prozesse von SubPc zu SiPc. Die Ladungsrekombination in den Grundzustand geschieht innerhalb von 1,7 ns.
The main objective of the present thesis was to conduct investigations of photo-induced electron transfer (ET) and excitation energy transfer (EET) processes in model compounds that are considered potentially appropriate for use in artificial photosynthesis. Two approaches have been used to construct the artificial photosynthetic systems, namely covalent and supramolecular approach. In both systems similar optically active molecules have been employed, particularly silicon-based phthalocyanines (SiPc). A comparative study between the covalently-linked and self-assembled systems had been conducted. For these purposes, thorough spectroscopic measurements in the UV/Vis range had been performed on these conjugates. A combination of steady-state and time-resolved experiments allowed an identification and quantification of the photo-induced ET and EET processes. In the first part of the work several covalently bound triads and a pentad bearing a central SiPc unit were studied. In all systems highly efficient ET and EET processes take place. It was found that the solvent exerts great influence on the photophysical properties of the systems. The lifetime of the charge-separated state varied from 1.7 ns (toluene) down to 30 ps (DMF). In the second part of the thesis, for the first time the formation of ternary supramolecular complexes consisting of a beta-cyclodextrin (CD), a conjugated subphthalocyanine (SubPc), a porphyrin (Por) and a series of SiPcs substituted axially with two CDs via different spacers was shown. These components are held in water by host-guest interactions and the formation of these host-guest complexes was found to be very efficient. Upon excitation of the SubPc-part of the complex sequential ET and EET processes from SubPc to SiPc take place. The Por dye acts as a transfer bridge enabling these processes. The probability of ET is controlled by the linker between CD and SiPc. Charge recombination to the ground state occurs within 1.7 ns.

Thesis (PhD)--Stellenbosch University, 2013.
ENGLISH ABSTRACT: Low-dimensional materials are known to undergo phase transitions to differently or- dered states, when cooled to lower temperatures. These phases often show a periodic modulation of the charge density (called a charge density wave – CDW) coupled with a periodic perturbation of the crystal lattice (called a periodic lattice distortion – PLD). Although many experiments have been performed and much has been learnt about CDW phases in low-dimensional materials, the reasons for their existence are still not fully understood yet. Many processes, involving either strong electron–electron or electron–lattice coupling, have been observed which all might play a role in explaining the formation of different phases under different conditions. With the availability of femtosecond lasers it has become possible to study materials under highly nonequilibrium conditions. By suddenly introducing a known amount of energy into the system, the equilibrium state is disturbed and the subsequent relax- ation processes are then observed on timescales of structural and electronic responses. These experiments can deliver valuable information about the complex interactions between the different constituents of condensed matter, which would be inaccessible under equilibrium conditions. We use time resolved electron diffraction to investigate the behaviour of a CDW system perturbed by a short laser pulse. From the observed changes in the diffraction patterns we can directly deduce changes in the lattice structure of our sample. A femtosecond electron diffraction setup was developed at the Laser Research In- stitute in Stellenbosch, South Africa. Short laser pulses produce photo electrons which are accelerated to an energy of 30 keV. Despite space charge broadening effects, elec- tron pulses shorter than 500 fs at sample position can be achieved. Technical details of this system and its characterisation as well as sample preparation techniques and analysis methods are described in detail in this work. Measurements on two members of the quasi-two-dimensional transition metal di- chalcogenides, namely 4Hb-TaSe2 and 1T-TaS2, are shown and discussed. Both show fast (subpicosecond) changes due to the suppression of the PLD and a rapid heating of the lattice. When the induced temperature rise heats the sample above a phase tran- sition temperature, a complete transformation into the new phase was observed. For 4Hb-TaSe2 we found that the recovery to the original state is significantly slower if the PLD was completely suppressed compared to only disturbing it. On 1T-TaS2 we could not only study the suppression of the original phase but also the formation of the higher energetic CDW phase. Long (100 ps) time constants were found for the tran- sition between the two phases. These suggest the presence of an energy barrier which has to be overcome in order to change the CDW phase. Pinning of the CDW by de- fects in the crystal structure result in such an energy barrier and consequently lead to a phase of domain growth which is considerably slower than pure electron or lattice dynamics.
AFRIKAANSE OPSOMMING: Dit is bekend dat lae-dimensionele materie fase oorgange ondergaan na anders ge- ori¨enteerde toestande wanneer afgekoel word tot laer temperature. Hierdie fases toon dikwels ’n periodiese modulasie van die elektron digtheid (genoem ’n “charge density wave” – CDW), tesame met ’n periodiese effek op die kristalrooster (genoem ’n “peri- odic lattice distortion” – PLD). Alhoewel baie eksperimente al uitgevoer is en al baie geleer is oor hierdie CDW fase, is die redes vir hul bestaan nog steeds nie ten volle verstaan nie. Baie prosesse, wat of sterk elektron–elektron of elektron–fonon interaksie toon, is al waargeneem en kan ’n rol speel in die verduideliking van die vorming van die verskillende fases onder verskillende omstandighede. Met die beskikbaarheid van femtosekonde lasers is dit nou moontlik om materie onder hoogs nie-ewewig voorwaardes te bestudeer. Deur skielik ’n bekende hoeveel- heid energie in die stelsel in te voer, word die ewewigstaat versteur en word die daar- opvolgende ontspanning prosesse waargeneem op die tydskaal van atomies struktu- rele en elektroniese bewiging. Hierdie eksperimente kan waardevolle inligting lewer oor die komplekse interaksies tussen die verskillende atomiese komponente van ge- kondenseerde materie, wat ontoeganklik sou wees onder ewewig voorwaardes. Ons gebruik elektrondiffraksie met tyd resolusie van onder ’n pikosekonde om die gedrag van ’n CDW stelsel te ondersoek nadat dit versteur is deur ’n kort laser puls. Van die waargenome veranderinge in die diffraksie patrone kan ons direk aflei watse veranderinge die kristalstruktuur van ons monster ondergaan. ’n Femtosekonde elektronendiffraksie opstelling is ontwikkel by die Lasernavors- ingsinstituut in Stellenbosch, Suid-Afrika. Kort laser pulse produseer foto-elektrone wat dan na ’n energie van 30 keV versnel word. Ten spyte van Coulomb afstoting ef- fekte, kan elektron pulse korter as 500 fs by die monster posisie bereik word. Tegniese besonderhede van hierdie opstelling, tegnieke van die voorbereiding van monsters asook analise metodes word volledig in hierdie tesis beskryf. Metings op twee voorbeelde van kwasi-tweedimensionele semi-metale, naamlik 4Hb-TaSe2 en 1T-TaS2, word gewys en bespreek. Beide wys ’n vinnige (subpikosekon- de) verandering as gevolg van die versteuring van die PLD en ’n vinnige verhitting van die kristalrooster. Wanneer die ge¨ınduseerde temperatuur bo die fase oorgang tempe- ratuur styg, is ’n volledige transformasie na die nuwe fase waargeneem. Vir 4Hb-TaSe2 het ons gevind dat die herstelling na die oorspronklike toestand aansienlik stadiger is as die PLD heeltemal viernietig is in vergelyking met as die PLD net versteur is. Met 1T-TaS2 kon ons nie net alleenlik die vernietiging van die oorspronklike fase sien nie, maar ook die vorming van ’n ho¨er energie CDW fase. Lang (100 ps) tydkonstante is gevind vir die oorgang tussen die twee fases. Hierdie dui op die teenwoordigheid van ’n energie-versperring wat eers oorkom moet word om die CDW fase voledig te ver- ander. Vaspenning van die CDW deur defekte in die kristalstruktuur veroorsaak so’n energie versperring en gevolglik lei dit tot ’n fase van groeiende CDW gebiede wat heelwat stadiger as pure elektron of kritalrooster dinamika is.

Thesis (Ph.D)--Chemistry and Biochemistry, Georgia Institute of Technology, 2010.
Committee Chair: Perry, Joseph; Committee Member: Bunz, Uwe; Committee Member: Lyon, Andrew; Committee Member: Marder, Seth; Committee Member: Trebino, Rick. Part of the SMARTech Electronic Thesis and Dissertation Collection.

This thesis is concerned with the photophysical and nonlinear optical responses, and applications of a set of conjugated polymers and small molecules in the visible and near-IR spectral regions. Poly(phenylene ethynylene) PPE polymers were substituted with conjugated side-arms in a cruciform fashion to determine the impacts of electronic coupling on the one-photon (1PA), two-photon (2PA), and excited state absorption (ESA) properties of the co-polymer system. The cruciform-like PPEs showed significant changes in their nonlinear and phophysical behavior relative to their linear models, including shifts and splittings of the 1PA bands due to moderate mixing of the lowest singlet excited states, an increase in the 2PA cross section (δ) values, and an increase in the yield of triplet excited-state species. The cruciform-like PPE polymers exhibited effective optical pulse suppression of femtosecond and nanosecond laser pulses over a broad spectral range of ~200 nm in the visible and near-IR. The suppression capability of the cruciform-like PPEs exceeded the best reported value for alkyl-substituted PPE polymers. The spectroscopic effects due to conjugation length, structural configuration, and intramolecular charge transfer (ICT) are discussed for a family of bent donor-acceptor-donor (D-A-D) -type conjugated oligomers, which incorporate electron-rich triarylamine donors and electron-deficient triarylborane acceptor units into its conjugated structure. These organoborane oligomers are highly fluorescent and exhibit strong 2PA in the visible region with δ values as large as 1410 GM, as well as overlapping ESA bands attributed to singlet-singlet and triplet-triplet absorption. Saturation of the molar absorptivity, ε, and δ was observed at less than two repeat monomer units due to conformational disorder in the oligomer with increasing length. Positive solvatochromism of fluorescence with solvent shifts as large as ~70 nm was observed as a result of ICT from the arylamine donors to boryl-centered acceptor sites. The excited-state dynamics also show sensitivity to the solvent environment. Experimental findings suggest that these organoborane oligomers may have potential use as nonlinear material for optical power limiting (OPL) and two-photon sensing applications. The spectral properties of two bis-donor chromophores, (bis(diarylamino)biphenyl (TPD) and distyrylthiophene (DST), were investigated with and without the presence of AgNPs in order to better understand the local-field enhancement and subsequent effects on the photophysics and nonlinear behavior of 2PA dyes. While little changes were observed in the excited-state dynamics, measurements of nanoparticle aggregate-dye composite solutions with TPD revealed a 1.6-enhancement in the two-photon excited fluorescence signal. OPL measurements of nanosecond laser pulses at 532 nm revealed a reduction in threshold energy by a factor of 2 in solutions containing TPD and AgNP aggregates, relative to solutions of TPD alone. DST shows exceptional solubility (>1 M) in several organic solvents and exhibits a 2PA spectrum that overlaps well with its singlet-singlet and triplet-triplet ESA bands. Consequently, DST exhibits effective optical limiting of nanosecond laser pulses through two-photon induced excited-state absorption over a broad spectral range of approximately 200 nm in the red and near-IR.

The main objective of this thesis is the study of the optical and optoelectronic properties of organic semiconducting materials. At the beginning of this thesis is shown the growing interest in these materials and their practical application. The theoretical part presents the current state of knowledge of studied problematic related to optical phenomena and the transport of charge carriers in organic semiconductors, photochormic phenomena of reversible molecular switch and charge transfer in DNA biopolymeric matrix. Experimental section, which consists of selected author’s publications, includes study of the charge transport, photochromic reversible switching and the role of dopant in pi-conjugated organic polymer system. Conductive and semiconductive characteristics of the DNA biopolymer have been aslo studied. Conductive and photoconductive techniques together with measurement of the optical characteristics have been used for organic semiconductors characterization.

The rapidly increasing power conversion efficiencies (PCEs) of organic solar cells (OSCs) above 10% were made possible by concerted international research activities in the last few years, aiming to understand the processes that lead to the generation of free charge carriers following photon absorption. Despite these efforts, many details are still unknown, especially how these processes can be improved already at the drawing board of molecular design. To unveil this information, dicyanovinyl end-capped oligothiophene derivatives (DCVnTs) are used as a model system in this thesis, allowing to investigate the impact of small structural changes on the molecular properties and the final solar cells. On thin films of a methylated DCV4T derivative, the influence of the measurement temperature on the charge carrier generation process is investigated. The observed temperature activation in photoinduced absorption (PIA) measurements is attributed to an increased charge carrier mobility, increasing the distance between the charges at the donor/acceptor (D/A) interface and, thus, facilitating their final dissociation. The correlation between the activation energy and the mobility is confirmed using a DCV6T derivative with lower mobility , exhibiting a higher activation energy for charge carrier generation. Another parameter to influence the charge carrier generation process is the molecular structure. Here, alkyl side chains with varying length are introduced and their influence on the intramolecular energy levels as well as the absorption and emission properties in pristine and blend films with the acceptor C60 are examined. The observed differences in intermolecular order (higher order for shorter side chains) and phase separation in blend layers (larger phase separation for shorter side chains) are confirmed in PIA measurements upon comparing the temperature dependence of the triplet exciton lifetimes. A proposed correlation between the side chain length and the coupling between D and A, which is crucial for efficient charge transfer, is not confirmed. The presented flat heterojunction solar cells underline this conclusion, giving similar photocurrent densities for all compounds. Differences in PCE are related to shifts of the energy levels and the morphology of the blend layer in bulk heterojunction devices. Furthermore, the impact of the electric field on the charge carrier generation yield is investigated in a proof-of-principle study, introducing PIA measurements in transmission geometry realized using semitransparent solar cells. The recombination analysis of the photogenerated charge carriers reveals two recombination components. Trapped charge carriers or bound charge pairs at the D/A interface are proposed as an explanation for this result. The miscibility of D and A, which can be influenced by heating the substrate during layer deposition, is of crucial importance to obtain high PCEs. In this work, the unusual negative influence of the substrate temperature on DCV4T:C60 blend layers in solar cells is investigated. By using optical measurements and structure determination tools, a rearrangement of the DCV4T crystallites is found to be responsible for the reduced absorption and, therefore, photocurrent at higher substrate temperature. The proposed blend morphology at a substrate temperature of 90° C is characterized by a nearly complete demixing of the D and A phases. This investigation is of particular relevance, because it shows the microscopic origins of a behavior that is contrary to the increase of the PCE upon substrate heating usually reported in literature. Finally, the optimization steps to achieve a record PCE of 7.7% using a DCV5T derivative as donor material are presented, including the optimization of the substrate temperature, the active layer thickness, and the transport layers
Der rasante Anstieg des Wirkungsgrads von organischen Solarzellen über die Marke von 10% war nur durch länderübergreifende Forschungsaktivitäten während der letzten Jahre möglich. Trotz der gemeinsamen Anstrengungen, die Prozesse, die zwischen der Absorption der Photonen und der Ladungsträgererzeugung liegen, genauer zu verstehen, sind einige Fragen jedoch immer noch ungelöst, z.B. wie diese Prozesse schon auf dem Reißbrett durch die gezielte Änderung bestimmter Molekülstrukturen optimiert werden können. Um dieses Ziel zu erreichen, werden in dieser Arbeit Dicyanovinyl-substituierte Oligothiophene (DCVnTs) verwendet. Diese Materialien bieten die Möglichkeit, kleine strukturelle Änderungen vorzunehmen, deren Einfluss auf die molekularen und auf die Solarzelleneigenschaften untersucht werden soll. Der Einfluss der Messtemperatur auf den Prozess der Ladungsträgertrennung wird hier an einer methylierten DCV4T-Verbindung in einer dünnen Schicht untersucht. Die bei photoinduzierter Absorptionsspektroskopie (PIA) beobachtete Aktivierung dieses Prozesses mit zunehmender Temperatur wird auf eine erhöhte Ladungsträgerbeweglichkeit zurückgeführt. Der dadurch erhöhte effektive Abstand der Ladungen an der Grenzfläche zwischen Donator (D) und Akzeptor (A) erleichtert die endgültige Trennung der Ladungsträger. Durch den Vergleich mit einer DCV6T-Verbindung wird der Zusammenhang zwischen der Aktivierungsenergie und der Beweglichkeit bekräftigt. Die kleinere Beweglichkeit äußert sich dabei in einer größeren Aktivierungsenergie. Darüber hinaus kann der Ladungsträgergenerationsprozess auch von der Molekülstruktur abhängen. In dieser Arbeit wird untersucht, wie sich die Länge von Alkylseitenketten auf die Energieniveaus der Moleküle, aber auch auf die Absorptions- und Lumineszenzeigenschaften der Materialien in reinen und in Mischschichten mit dem Akzeptor C60 äußert. Die ermittelten Unterschiede bezüglich der Molekülordnung (geordneter für kürzere Seitenketten) und der Phasengrößen in Mischschichten (größere Phasen bei kürzerer Kettenlänge) werden in der Untersuchung der Temperaturabhängigkeit der Lebensdauer von Triplettexzitonen mittels PIA-Messungen bestätigt. Für Solarzellen ist von Bedeutung, ob sich die Seitenkettenlänge auf die Wechselwirkung zwischen D und A auswirkt. Der vermutete Zusammenhang wird hier nicht bestätigt. Ein ähnlicher Photostrom für alle untersuchten Verbindungen in Solarzellen mit planaren Heteroübergängen unterstreicht diese Schlussfolgerung. Unterschiede im Wirkungsgrad werden auf Änderungen der Energieniveaus und die Morphologie in Mischschichtsolarzellen zurückgeführt. Des Weiteren wird in einer Machbarkeitsstudie der Einfluss des elektrischen Felds auf die Generationsausbeute freier Ladungsträger untersucht. Dafür werden halbtransparente Solarzellen verwendet, die es ermöglichen, PIA-Messungen in Transmissionsgeometrie durchzuführen. Als mögliche Erklärung für das Auftreten zweier Rekombinationskomponenten in der Analyse des Rekombinationsverhaltens der durch Licht erzeugten Ladungsträger werden eingefangene Ladungsträger und gebundene Ladungsträgerpaare an der D/A-Grenzfläche genannt. Das Mischverhalten von D und A kann durch ein Heizen des Substrates während des Verdampfungsprozesses eingestellt werden, was von entscheidender Bedeutung für eine weitere Steigerung des Wirkungsgrades ist. Für DCV4T:C60-Mischschichtsolarzellen wird jedoch eine Verschlechterung des Wirkungsgrads zu höheren Substrattemperaturen beobachtet. Durch optische Messungen und Methoden zur Schichtstrukturbestimmung wird dieser Effekt auf eine Umordnung der DCV4T-Kristallite für hohe Substrattemperaturen und die damit verbundene Verringerung der Absorption und damit auch des Photostroms zurückgeführt. Bei einer Substrattemperatur von 90° C sind die D- und A-Komponenten fast vollständig entmischt. Dieses Beispiel ist von besonderer Bedeutung, weil hier die Ursachen für ein Verhalten aufgezeigt werden, das entgegen den Beispielen aus der Literatur eine Abnahme des Wirkungsgrads beim Aufdampfen der aktiven Schicht auf ein geheiztes Substrat zeigt. Schließlich werden die Optimierungsschritte dargelegt, mit denen Solarzellen mit einer DCV5T-Verbindung als Donatormaterial auf einen Rekordwirkungsgrad von 7,7% gebracht werden. Dabei wird die Substrattemperatur, die Dicke der aktiven Schicht und die Transportschichten angepasst

Artificial photosynthesis is used to harvest solar energy and store it in the form of chemical bonds. The system of interest in this study does this by splitting water into hydrogen and oxygen gas through a plasmon assisted process, collective oscillations from free electron gas. This is a renewable way to store energy that could be used as an alternative to fossil based fuel. In this study, a small part of this photo catalytic system is studied, namely the interaction between plasmonically active silver nanoparticles (Ag NPs) transferring photo-excited electrons via a linker molecule, 4-aminobenzoic acid (pABA). The pABA linker molecule transfers charge from the Ag surface to a semiconductor and a catalyst performing the water splitting. The pABA can bind in different ways onto the Ag-surface and the aim of this study is to examine which bond is strongest and which best enables charge transfer. To this purpose three systems where simulated quantum mechanically using a supercomputer. The total free energy of the systems was computed and compared. Out of the three studied binding sites, the hollow-site bond (pABA binding to three silver atoms) was found to have the lowest energy, meaningit's the strongest of the possible bonds. Additionally it was found that the band gap (the energy needed to transfer charge) for the pABA decreased when bound to the Ag-surface. The hollow-site bound pABA also had the smallest band gap, meaning it requires the least energy to transfer a charge and should therefore be the best bond fitted for the photo catalytic system.
Artificiell fotosyntes används för att absorbera solenergi och förvara den i formen av kemiska bindningar. Systemet som används i denna studie gör detta genom att splittra vatten till vätgas och syrgas genom en plasmon assisterad process. Detta är ett förnyelsebart sätt att förvara energi och kan användas som ett alternativ till fossila bränslen. I denna studie studeras en liten del utav detta fotokatalytiska system nämligen interaktionen där plasmonaktiva silvernanopartiklar (Ag NPs) överför foto-exciterade elektroner genom molekyllänken 4-aminobensoesyra (pABA). Molekyllänken pABA överför laddning från silverytan till en halvledare och en katalys som utför splittringen av vattnet. pABA kan binda på olika sätt tillen silveryta och denna studie syftar till att undersöka vilken utav bindningarna som är starkast och vilken som effektivast överför laddning. För att göra detta simulerades tre system kvantmekaniskt med hjälp av en superdator, ett system för varje sorts bindning. Den totala fria energin av systemen beräknades och jämfördes. Av de tre undersökta bindningarna hadehollow-site bindningen (pABA som binder till tre silveratomer) längst energi, vilket betyder att det är den starkaste av bindningarna. Utöver detta så visade det sig att bandgapet (energin som krävs för att överföra laddning) minskade för pABA när den var bunden till Ag-ytan. Hollow-site bundet pABA hade även minst bandgap, vilket betyder att den kräver minst energi för att överföra laddning och är därmed den mest effektiva bindningen för det fotokatalytiska systemet.

Colloidal semiconductor photocatalytic materials such as Ti02• α-Fe203 and Sn02 have been used in laboratory-scale pollution abatement systems, reducing I oxidising both organic and inorganic impurities / toxins to chemically useful and / or biologically harmless compounds. For Ti02 there are potentially two distinct photoinduced phenomena: the first is the photocatalytic redox phenomena described above. The second involves photolytically induced high wettability or superhydrophilicity. The longer the surface is illuminated with IN light, the smaller the contact angle formed between the air - water - TiO2 interfaces until, in some cases the angle approaches zero. We have studied Photo-induced SuperHydrophilicity (PISH) on mesoporous TiO2(M-Ti02) films produced from reverse micellar solutions of titanium isopropoxide. M-Ti02 films have been deposited on quartz by spin coating and shown to clearly exhibit phot(}-induced wettability when irradiated with ultra-band gap light. Using a new continuous contact angle measurement technique. the time dependence of the photo-induced wettability changes on the film have been evaluated through the spreading of a sessile water drop. Results obtained at 100% RH, 293 K showed that drops on M-Ti02 exhibited a photo-induced "stick-slip" behaviour. The thermodynamic driving force for this photo-induced stick-slip has been attributed to the departure of the system from capillary equilibrium as the equilibrium contact angle of the drop, θo, decreased with illumination time. Based on this model, a simple theoretical description of photo-induced stick-slip has been derived and used to calculate a value of the potential energy barrier opposing the onset of movement of the triple line, U = 6.26 X 10-6 J m-1. This is the first time that U has been quantified for a surface with photo-induced wenability. Micro gravimetric studies of M-Ti02 layers in humid atmospheres show that, especially at RH > 95%, illumination of the M-Ti02 surface leads to a photo-induced watcr adsorption I condensation at the semiconductor / gas interface. Studies of this photo-induced water condensation on M-Ti02 coated crystals as a function of crystal age / experiment run number indicates that there are two possible modes of condensation - in-pore / in-layer condensation and condensation over the outer surface of the layer.

There is current debate in literature as to the main source of photoinduced super-hydrophilic (PSH) nature on Ti02 films with groups segregated into two schools of thought: (i) those attributing the effect to UV induced modifications of the Ti02 surface; and (ii) those attributing the effect to the well-known photo-oxidation properties of Ti02 in removing hydrophobic organic layers from the Ti02 surface. This thesis presents acquisition of experimental goniometric data required to allow theoretical analysis of the super-hydrophilic nature on as prepared mesoporous-Ti02 (m-Ti02), in order to determine the source of PSH. Evidence to advocate that surface reconstruction does not occur instantaneously upon ultra-band gap illumination, the Ti02 surface is inherently wet with a contact angle, 8, being 4°, and the photo-induced super-hydrophilic nature is due to the latter effect, (ii), is also discussed. Experiments demonstrating the change in the Ti02 surface during UV band-gap illumination in the presence of organics using micro-gravimetric techniques, mainly the quartz crystal microbalance (QCM), are presented and exploration and applications of PSH-related phenomena in real world sensing devices are explored.

The solid-state mesoscopic solar cells (sMSCs) have been developed as a promising alternative technology to the conventional photovoltaics. However, the device performance suffers from the low hole-mobilities and the incomplete pore filling of the hole transport materials (HTMs) into the mesoporous electrodes. A variety of HTMs and different preparation methods have been studied to overcome these limitations. There are two types of sMSCs included in this doctoral thesis, namely solid-state dye-sensitized solar cells (sDSCs) and organometallic halide perovskite based solar cells. Two different types of HTMs, namely the small molecule organic HTM spiro-OMeTAD and the conjugated polymer HTM P3HT, were compared in sDSCs. The photo-induced absorption spectroscopy (PIA) spectra and spectroelectrochemical data suggested that the dye-dye hole conduction occurs in the absence of HTM and appears to be of significant importance to the contribution of hole transport. The PIA measurements and transient absorption spectroscopy (TAS) indicated that the oxidized dye was efficiently regenerated by a small molecule organic HTM TPAA due to its excellent pore filling. The conducting polymer P3HT was employed as a co-HTM to transfer the holes away from TPAA to prohibit the charge carrier recombination and to improve the hole transport. An alternative small molecule organic HTM, MeO-TPD, was found to outperform spiro-OMeTAD in sDSCs due to its more efficient pore filling and higher hole-mobility. Moreover, an initial light soaking treatment was observed to significantly improve the device performance due to a mechanism of Li+ ion migration towards the TiO2 surface. In order to overcome the infiltration difficulty of conducting polymer HTMs, a state-of-the-art method to perform in-situ photoelectrochemical polymerization (PEP) in an aqueous micellar solution of bis-EDOT monomer was developed as an environmental-friendly alternative pathway with scale-up potential for constructing efficient sDSCs with polymer HTMs. Three different types of HTMs, namely DEH, spiro-OMeTAD and P3HT, were used to investigate the influence of HTMs on the charge recombination in CH3NH3PbI3 perovskite based sMSCs. The photovoltage decay measurements indicate that the electron lifetime (τn) of these devices decreases by one order of magnitude in the sequence τspiro-OMeTAD > τP3HT > τDEH.

Jádrem této disertační práce bylo studovat optické a elektrické charakteristiky tenkovrstvých elektroluminiscenčních součástek řízených střídavým proudem (ACTFEL) a zejména vliv procesu stárnutí luminiforů na jejich optické a elektrické vlastnosti. Cílem této studie měl být příspěvek ke zvýšení celkové účinnosti luminoforů, vyjádřené pomocí jasu, účinnosti a stability. Vzhledem k tomu, že současnou dominantní technologií plochých obrazovek je LCD, musí se další alternativní technologie plošných displejů porovnávat s LCD. Výhodou ACTFEL displejů proti LCD je lepší rozlišení, větší teplotní rozsah činnosti, větší čtecí úhel, či možnost čtení při mnohem vyšší intenzitě pozadí. Na druhou stranu je jejich nevýhodou vyšší energetická náročnost, problém s odpovídající barevností tří základních barev a podstatně vyšší napětí nutné pro činnost displeje. K dosažení tohoto cíle jsme provedli optická, elektrická a optoelektrická měření ACTFEL struktur a ZnS:Mn luminoforů. Navíc jsme studovali vliv dotování vrstvy pomocí KCl na chování mikrostruktury a na elektroluminiscenční vlastnosti (zejména na jas a světelnou účinnost) ZnS:Mn luminoforů. Provedli jsme i některá, ne zcela obvyklá, měření ACTFEL součástek. Vypočítali jsme i rozptylový poměr nabitých barevných center a simulovali transportní charakteristiky v ACTFEL součástkách. Studovali jsme vliv stárnutí dvou typů ZnS:Mn luminoforů (s vrstvou napařenou či získanou pomocí epitaxe atomových vrstev) monitorováním závislostí svítivost-napětí (L-V), velikost vnitřního náboje - elektrické pole luminoforu (Q-Fp) a kapacitance-napětí (C-V) ve zvolených časových intervalech v průběhu stárnutí. Provedli jsme krátkodobá i dlouhodobá měření a pokusili jsme se i o vizualizaci struktury luminoforu se subvlnovým rozlišením pomocí optického rastrovacího mikroskopu pracujícího v blízkém poli (SNOM). Na praktickém případu zeleného Zn2GeO4:Mn (2% Mn) ACTFEL displeje, pracujícího při 50 Hz, jsme také studovali stabilitu svítivosti pomocí měření závislosti svítivosti na napětí (L-V) a světelné účinnosti na napětí (eta-V). Přitom byl zhodnocen význam těchto charakteristik. Nezanedbatelnou a neoddělitelnou součástí této práce je i její pedagogický aspekt. Předložený text by mohl být využit i jako učebnice pro studenty na mé univerzitě v Lybii.

Le premier volet de cette thèse est consacré à la modélisation des phénomènes de transport dans le LN. Partant d'une analyse critique des modèles de bande usuels, nous montrons leur inadéquation dans le cas du LN et nous proposons un modèle de saut basé sur la théorie des petits polarons. Nous étudions d'abord par simulation Monte-Carlo la décroissance d'une population de polarons liés NbLi4+ relaxant vers des pièges profonds FeLi3+. Nous montrons que les pièges FeLi3+ ont des rayons effectifs particulièrement grands, rayons qui augmentent encore à température décroissante, et limitent considérablement les longueurs de diffusion des polarons. Les résultats de simulations sont ensuite confrontés aux résultats expérimentaux obtenus par différentes techniques ; Absorption photo-induite, Raman, Enregistrement holographique et Pompe-sonde. Le deuxième volet de cette thèse est consacré aux applications électro-optiques dans le LN périodiquement polarisé (PPLN). Sous l’effet d’une tension électrique, l’indice de réfraction du PPLN est périodiquement diminué et augmenté, formant ainsi un réseau d’indice activable électriquement. Un premier composant utilisant l’effet électro-optique dans du PPLN a été développé et démontré expérimentalement. Dans ce composant, la lumière est défléchie sous l’effet de la tension électrique par le réseau d’indice. Ce déflecteur de Bragg atteint une efficacité de diffraction proche de 100% avec une faible tension de commande de l’ordre de 5 V. Un deuxième composant a également été proposé, où la lumière se propage perpendiculairement aux parois de domaines du PPLN. Dans cette configuration un réflecteur de Bragg électro-optique peut être réalisé
The first part of this thesis is devoted to the modeling of transport phenomena in the LN. From a critical analysis of the usual band models, we show their inadequacy in the case of LN and we propose a hopping model based on the theory of small polarons. We first study by Monte-Carlo simulation the population decay of bound polarons NbLi4+ in deep traps FeLi3+. We show that the traps (FeLi3+) have particularly large effective radii, which increase further at decreasing temperature, and considerably limit the diffusion lengths of the polarons. The results of simulations are then compared with experimental results obtained by different techniques; Light-induced absorption, Raman, Holographic storage and Pump-Probe. The second part of this thesis is devoted to electro-optical applications in the periodically poled LN (PPLN). Under the effect of an electrical voltage, the refractive index of the PPLN is periodically decreased and increased, thus forming an electrically activatable index grating. A first component using the electro-optical effect in PPLN has been developed and demonstrated experimentally. In this component, the light is deflected under the effect of the electrical voltage by the index grating. This Bragg deflector achieves a diffraction efficiency of close to 100% with a low drive voltage of the order of 5 V. A second component has also been proposed, where light propagates perpendicularly to the domain walls of the PPLN. In this configuration an electro-optic Bragg reflector can be realized

In der vorliegenden Arbeit wird die neuartige Mikroskopiemethode der Ptychographie für die Untersuchung photorefraktiver Materialien genutzt. Photorefraktive Materialien zeichnen sich durch die Generation lichtinduzierter Brechungsindexänderungen aus. Die Ptychographie bietet die Möglichkeit, neben der generierten Brechungsindexänderung im photorefraktiven Material auch die für die Generation genutzte Intensitätsverteilung des Laserstrahls zu bestimmen. Es wird sowohl die Abhängigkeit der Brechungsindexänderung von der Zeit der Generation als auch die Abhängigkeit von der Polarisation des Lasers gemessen. Durch den Vergleich der gewonnenen Werte mit einer numerischen Simulation des photorefraktiven Effekts werden mikroskopische Parameter der lichtinduzierten Ladungswanderung ermittelt. Zudem wird aus der polarisationsabhängigen ptychographischen Messung das Raumladungsfeld und die korrespondierende Ladungsdichte im Material berechnet. Die Ptychographie liefert damit einen neuen Zugang zum quantitativen Verständnis der Photorefraktivität
In the present thesis the novel microscopy technique of ptychography is applied to the investigation of photorefractive materials. Photorefractive materials exhibit a change of the refractive index due to the exposure to light. The method of ptychography determines the refractive index change of the material together with the intensity distribution of the laser beam that was used for its generation. In one part of the experiment the time dependence of the refractive index change versus the generation time is investigated, in the other part of the experiment the dependence of the refractive index change to the polarisation of the laser beam is examined. Microscopic parameters of the photorefractive charge migration are determined with the utilisation of a numerical simulation of the photorefractive effect and its comparison with the measurement. Finally, the whole space charge field with the corresponding space charge density is calculated from a set of ptychographic measurements of one refractive index change with different polarisation directions of the laser. The presented experiments and their evaluation show, that the method of ptychography opens a new possibility for a quantitative understanding of the photorefractive effect

碩士
輔仁大學
化學系
98
The efficiency of charge transfer plays an important role in organic polymer solar cells. With the introduction of Bulk Heterojunction (BHJ) concept in 1994, the power conversion efficiency of organic solar cell has been improved tremendously. Unfortunately, the morphology is unstable because of the effect of molecular aggregation and de-mixing of the two materials. Both of these issues cause the blend to separate and phase separation occur. In this study, relationship between phase separation (the interface distance between donor and acceptor) and charge transfer of poly(3-hexyl thiophene) (P3HT) and 6,6-phenyl-C61-butyric acid methyl ester (PCBM) will be examined. Effect of parameters such as concentration, mixing ratio and annealing time will be studied by UV-visible spectroscopy, photoluminescence spectroscopy, and luminescence lifetime measurements. Aggregation that causes by thermal annealing will be analyzed by Scanning Electron Microscopy (SEM). In conclusion, we find there is no charge transfer occurred below a limited concentration in solution state. The efficiency of charge transfer develops when the mixing ratio of donor and acceptor increases. On the other hand, bilayer films of P3HT and PCBM shows a short-range ordered structure of PCBM after annealing treatment. The short-range ordered structure caused by aggregation affects the efficiency of charge transfer.

Photo-induced charge transfer which occurs between molecules or different parts of a large molecule is the pivotal process related to performances of organic electronics. In particular, injection of charge carriers into conjugated polymers and dissociation of photo-generated excitons at the heterojunction between a donor and acceptor system are of great importance in determining the luminescence efficiency of organic light emitting diodes (OLEDs) and solar energy conversion efficiency of organic solar cells, respectively. However, the complex nature of organic semiconductors as well as complicated primary processes involved in the functioning of these devices have prevented us from understanding unique characteristics of these processes and thereby engineering better materials for higher performances. In this dissertation, two different types of photo-induced (or -related) charge transfer processes occurring in organic semiconductors were investigated by using single molecule spectroscopy (SMS) techniques to unravel the complexities of these processes. The carefully designed functioning capacitor-like model devices similar to OLEDs and photovoltaic cells were fabricated where isolated single nanoparticles were introduced as an active medium to mitigate the complexities of these materials. We observed that injection of positively charged carriers (holes) into poly[2-methoxy-5-(2'-ethyl-hexyloxy)-1,4-phenylene vinylene] (MEH-PPV) single nanoparticles from the carbazole hole transport layer does not occur in the absence of light. We denoted the observed hole injection in aid of light as the light-induced hole transfer mechanism (LIHT). It was revealed that the charging dynamics are highly consistent with a cooperative charging effect. In addition, the LIHT was proposed as the possible source for the formation of deep trapped hole in organic devices. Local exciton dissociation yields across a nanostructured domain between poly(9,9-dioctylfluorene-alt-benzothiadiazole) (F8BT) single nanoparticles and either poly(9,9- dioctylfluorene - co - bis-N,N- (4 -butylphenyl)-bis-N,N-phenyl-1,4-phenylene diamine) (PFB) or poly(9,9-dioctylfluorene-co-N-(4-butylphenyl)diphenylamine) (TFB) film in model photovoltaic devices was also investigated. A wide distribution of exciton dissociation yields was observed from each nanodomain due to the device geometry. The observed hysteresis in fluorescence voltage curve was ascribed to accumulated charges following charge separations. The dynamics of charge separation under the applied electric field was described in more detail.
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The aim of the current work was to investigate the photo-induced charge transport at low temperatures, allowing more sensitive, detailed measurements of the first steps in the build-up of space charge fields, which modify the refractive index, leading to modern applications like volume holographic storage. We investigated the light-induced properties of SBN:Ce, KTO and KTN materials like origin of trapping centers which are involved in the charge transport process, characterization of trapping centers, like temperature dependence, illumination intensity dependence, evolution with time, spectral response, activation energies, the basic properties of the electronic excitations and photo-carriers localization based on results of absorption, light-induced absorption, photoluminescence, and photocurrent. The main contributions of this dissertation are summarized as follows: The experimental intensity dependence, temperature dependence, and decay process of the light-induced polaron (NIR) and VIS center absorption can be fitted with the help of a simplified charge transfer model (for SBN). The decay observed of the NIR polaron and the VIS centers is present due to the Fourier spectrometer light. The dissociation of the VIS centers into NIR centers under red light was observed. The model proposed for the VIS-centers in SBN is a triad structure related to the simultaneous bonding of two hole polarons and one electronic polaron.In KTN the emergence of the UV-light induced wide absorption bands in the NIR region with maxima at 0.69 0.8 eV at low temperatures is treated as a manifestation of the localization of photo-induced electrons and the formation of small electron polarons in close-neighbor Nb-Nb pair centers. Also, these properties in KTN can be fitted with the help of the simplified charge transfer model.

碩士
國立中山大學
光電工程研究所
96
In this thesis , we studied the photo-chemistry between the green emitter (C545T) and the photo-acid generator (PAG) . When the sample of C545T and PAG in solutions and thin films were exposured to UV-light , we found that a new product was produced due to protonation of C545T with the acid generated by PAG . Therefore , we measured absorption and fluorescence spectra of the samples in solutions (THF) and in polymer (PMMA) thin films . The different concentrations of C545T dopanted photo-acid generator in the solvent (THF) could increase the photo-acid generator at higher concentrations of PAG , the energy could be transferred from unprotonated to protonated . Therefore , we can easily observe the absorption and fluorescence spectra have been changed and the phenomenon of stock’s shift has been found accordingly . At higher concentrations of C545T in solutions , also called concentrations quenching effect was observed because C545T molecules could collide each other easily that causes intensity to decrease in the solvent (THF) . In order to get rid of the collision effect , we use the samples of polymer thin films instead of solutions . The different of the change of spectra between solutions and thin films were observed and compared were also studied .

碩士
國立中山大學
光電工程研究所
96
In this thesis , we studied a green emitter (C545T) dopanted SU8. C545T is an organic dye. [10-(2-benzothiazolyl)-1,1,7,7-tetramethyl-2,3,6,7-tetrahydro-1H,5H,11Hbenzo[l]-pyrano[6,7,8-ij]quinolizin-11one(C545T)] . When the sample of C545T and SU8 with thin films were exposured to UV-light. We found that the thin film between with UV exposure (L1-Red) and without UV exposure (L2-Green) will show the different chemistry properties.We can achieve proper CIE coordinates and color by adjusting .The different concentrations of C545T dopanted in SU8 thin films.The L1 and L2 were close-kint blue back-light in order to achieve a tunable emission module . If we crafted meticulously optimization , we can find a exclusive white light. This is a optic thin film attach to Color-change materials

The rapidly increasing power conversion efficiencies (PCEs) of organic solar cells (OSCs) above 10% were made possible by concerted international research activities in the last few years, aiming to understand the processes that lead to the generation of free charge carriers following photon absorption. Despite these efforts, many details are still unknown, especially how these processes can be improved already at the drawing board of molecular design. To unveil this information, dicyanovinyl end-capped oligothiophene derivatives (DCVnTs) are used as a model system in this thesis, allowing to investigate the impact of small structural changes on the molecular properties and the final solar cells. On thin films of a methylated DCV4T derivative, the influence of the measurement temperature on the charge carrier generation process is investigated. The observed temperature activation in photoinduced absorption (PIA) measurements is attributed to an increased charge carrier mobility, increasing the distance between the charges at the donor/acceptor (D/A) interface and, thus, facilitating their final dissociation. The correlation between the activation energy and the mobility is confirmed using a DCV6T derivative with lower mobility , exhibiting a higher activation energy for charge carrier generation. Another parameter to influence the charge carrier generation process is the molecular structure. Here, alkyl side chains with varying length are introduced and their influence on the intramolecular energy levels as well as the absorption and emission properties in pristine and blend films with the acceptor C60 are examined. The observed differences in intermolecular order (higher order for shorter side chains) and phase separation in blend layers (larger phase separation for shorter side chains) are confirmed in PIA measurements upon comparing the temperature dependence of the triplet exciton lifetimes. A proposed correlation between the side chain length and the coupling between D and A, which is crucial for efficient charge transfer, is not confirmed. The presented flat heterojunction solar cells underline this conclusion, giving similar photocurrent densities for all compounds. Differences in PCE are related to shifts of the energy levels and the morphology of the blend layer in bulk heterojunction devices. Furthermore, the impact of the electric field on the charge carrier generation yield is investigated in a proof-of-principle study, introducing PIA measurements in transmission geometry realized using semitransparent solar cells. The recombination analysis of the photogenerated charge carriers reveals two recombination components. Trapped charge carriers or bound charge pairs at the D/A interface are proposed as an explanation for this result. The miscibility of D and A, which can be influenced by heating the substrate during layer deposition, is of crucial importance to obtain high PCEs. In this work, the unusual negative influence of the substrate temperature on DCV4T:C60 blend layers in solar cells is investigated. By using optical measurements and structure determination tools, a rearrangement of the DCV4T crystallites is found to be responsible for the reduced absorption and, therefore, photocurrent at higher substrate temperature. The proposed blend morphology at a substrate temperature of 90° C is characterized by a nearly complete demixing of the D and A phases. This investigation is of particular relevance, because it shows the microscopic origins of a behavior that is contrary to the increase of the PCE upon substrate heating usually reported in literature. Finally, the optimization steps to achieve a record PCE of 7.7% using a DCV5T derivative as donor material are presented, including the optimization of the substrate temperature, the active layer thickness, and the transport layers.:Abstract - Kurzfassung Publications Contents 1 Introduction 2 Elementary Processes in Organic Semiconductors 2.1 Introduction 2.2 Optical Excitations in Organic Materials 2.2.1 Introduction 2.2.2 Radiative Processes: Absorption and Emission 2.2.3 Non-radiative Relaxation Processes 2.2.4 Triplet Excitons and Intersystem Crossing 2.3 Polarization Effects and Disorder 2.4 Transport Processes in Disordered Organic Materials 2.4.1 Charge Transport 2.4.1.1 The Bässler Model 2.4.1.2 Marcus Theory for Electron Transfer 2.4.1.3 Small Polaron Model 2.4.1.4 Functional Dependencies of the Charge Carrier Mobility 2.4.2 Diffusive Motion 2.4.3 Exciton Transfer Mechanisms 2.4.4 Characteristics of Exciton Diffusion 2.5 Charge Photogeneration in Pristine Materials 3 Organic Photovoltaics 3.1 General Introduction to Solar Cell Physics 3.2 Introduction to the Donor/Acceptor Heterojunction Concept 3.3 The Open-Circuit Voltage in Organic Solar Cells 3.4 Doping of Organic Semiconductors 3.5 Introduction to the p-i-n Concept 3.6 Charge Transfer Excitons in Donor/Acceptor Heterojunction Systems 3.6.1 Introduction 3.6.2 Verification of Charge Transfer Excitons in Donor/Acceptor Systems 3.7 The Process Cascade for Free Charge Carrier Generation in Donor/Acceptor Heterojunction Systems 3.7.1 The Initial Charge Transfer Step 3.7.2 The Binding Energy of the Charge Transfer Exciton 3.7.3 \"Hot\" Charge Transfer Exciton Dissociation 3.7.4 \"Cold\" Charge Transfer Exciton Dissociation 3.7.5 Supposed Influence Factors on Charge Transfer Exciton Dissociation 3.7.6 Recombination Pathways for Charge Transfer Excitons 3.7.7 Free Charge Carrier Formation and Recombination 4 Experimental Methods 4.1 Sample Preparation 4.2 Material Characterization Methods 4.2.1 Optical Characterization 4.2.2 Cyclic Voltammetry 4.2.3 Ultraviolet Photoelectron Spectroscopy 4.2.4 Atomic Force Microscopy 4.2.5 Grazing Incidence X-Ray Diffraction 4.2.6 Organic Field-Effect Transistor 4.3 Photoinduced Absorption Spectroscopy 4.3.1 Introduction 4.3.2 Derivation of the PIA Signal 4.3.3 Recombination Dynamics 4.3.4 Intensity Dependence of the PIA Signal 4.4 Solar Cell Characterization 4.4.1 External Quantum Efficiency 4.4.2 Spectral Mismatch Correction 4.4.3 Current-Voltage Characteristics 4.4.4 Optical Device Simulations 4.4.5 Optical Device Transmission Measurements 5 The Oligothiophene Material System 5.1 Introduction 5.2 Thermal Stability 5.3 Energy Levels 5.4 Optical Properties of the Pristine Materials 5.5 The Donor/Acceptor Couple: DCVnT and C60 5.6 Solar Cell Devices 5.7 Summary 6 Temperature Dependence of Charge Carrier Generation 6.1 Introduction 6.2 Principal Introduction to the PIA Measurements 6.2.1 Interpretation of the Spectra 6.2.2 Interpretation of the Frequency Scans 6.3 Temperature Dependence of the Spectra 6.4 Discussion of the Temperature Dependent Processes in the Blend Layer 6.5 Temperature Activated Free Charge Carrier Generation 6.5.1 Evaluation of the Activation Energy for the DCV4T-Me:C60 Blend 6.5.2 Comparison to a Sexithiophene Derivative (DCV6T-Me) 6.6 Summary 7 Side Chain Investigation on Quaterthiophene Derivatives 7.1 Energy Levels 7.2 Optical Properties 7.2.1 Solution and Pristine Films 7.2.2 Mixed Films with C60 7.3 Influence of the Side Chain Length on the Intermolecular Coupling 7.3.1 PIA Spectra of Pristine and Blend Layers at 10K 7.3.2 Recombination Analysis for Pristine and Blend Films at 10K 7.4 The Influence of the Side Chain Length on the Offset Charge Carrier Generation Rate at Low Temperature 7.5 In the High-Temperature Limit: Implications for Solar Cell Devices 7.5.1 PIA Spectra in Pristine and Blend Films at 200K 7.5.2 Recombination Analysis: Triplet Excitons and Free Charge Carriers 7.6 Solar Cells 7.6.1 Flat Heterojunction Devices 7.6.2 Bulk Heterojunction Devices 7.7 Summary 8 Electric-Field Dependent PIA Measurements on Complete Solar Cell Devices 8.1 Introduction 8.2 Semitransparent Organic Solar Cells 8.3 Photoinduced Absorption Measurements 8.4 Summary and Outlook 9 The Effect of Substrate Heating During Layer Deposition on the Performance of DCV4T:C60 BHJ Solar Cells 9.1 Introduction 9.2 The Importance of Morphology Control for BHJ Solar Cells 9.3 The Impact of Substrate Heating on DCV4T:C60 BHJ Solar Cells 9.4 Absorption and Photoluminescence 9.5 Topographical Investigations (AFM) 9.6 X-ray Investigations 9.6.1 1D GIXRD Measurements 9.6.2 2D GIXRD Measurements 9.7 Proposed Morphological Picture and Confirmation Measurements 9.7.1 Morphology Sketch of the DCV4T:C60 Blend Layer 9.7.2 Confirmation Measurements 9.8 The Equivalence of Temperature and Time 9.9 Summary 10 Record Solar Cells Using DCV5T-Me33 as Donor Material 10.1 Introduction 10.2 The Influence of the Substrate Temperature 10.3 Determination of the Optical Constants 10.4 Stack Optimization 10.5 Summary and Outlook 11 Conclusions and Outlook 11.1 Summary of the Photophysical Investigations 11.2 Summary of Device Investigations 11.3 Future Challenges Appendix A Detailed Description of the Experimental Setup for PIA Spectroscopy Appendix B Determination of the Triplet Level by Differential PL Measurements Appendix C Additional Tables and Figures Appendix D Reproducibility of the Solar Cell Results (Statistics) Appendix E Lists Bibliography Acknowledgments
Der rasante Anstieg des Wirkungsgrads von organischen Solarzellen über die Marke von 10% war nur durch länderübergreifende Forschungsaktivitäten während der letzten Jahre möglich. Trotz der gemeinsamen Anstrengungen, die Prozesse, die zwischen der Absorption der Photonen und der Ladungsträgererzeugung liegen, genauer zu verstehen, sind einige Fragen jedoch immer noch ungelöst, z.B. wie diese Prozesse schon auf dem Reißbrett durch die gezielte Änderung bestimmter Molekülstrukturen optimiert werden können. Um dieses Ziel zu erreichen, werden in dieser Arbeit Dicyanovinyl-substituierte Oligothiophene (DCVnTs) verwendet. Diese Materialien bieten die Möglichkeit, kleine strukturelle Änderungen vorzunehmen, deren Einfluss auf die molekularen und auf die Solarzelleneigenschaften untersucht werden soll. Der Einfluss der Messtemperatur auf den Prozess der Ladungsträgertrennung wird hier an einer methylierten DCV4T-Verbindung in einer dünnen Schicht untersucht. Die bei photoinduzierter Absorptionsspektroskopie (PIA) beobachtete Aktivierung dieses Prozesses mit zunehmender Temperatur wird auf eine erhöhte Ladungsträgerbeweglichkeit zurückgeführt. Der dadurch erhöhte effektive Abstand der Ladungen an der Grenzfläche zwischen Donator (D) und Akzeptor (A) erleichtert die endgültige Trennung der Ladungsträger. Durch den Vergleich mit einer DCV6T-Verbindung wird der Zusammenhang zwischen der Aktivierungsenergie und der Beweglichkeit bekräftigt. Die kleinere Beweglichkeit äußert sich dabei in einer größeren Aktivierungsenergie. Darüber hinaus kann der Ladungsträgergenerationsprozess auch von der Molekülstruktur abhängen. In dieser Arbeit wird untersucht, wie sich die Länge von Alkylseitenketten auf die Energieniveaus der Moleküle, aber auch auf die Absorptions- und Lumineszenzeigenschaften der Materialien in reinen und in Mischschichten mit dem Akzeptor C60 äußert. Die ermittelten Unterschiede bezüglich der Molekülordnung (geordneter für kürzere Seitenketten) und der Phasengrößen in Mischschichten (größere Phasen bei kürzerer Kettenlänge) werden in der Untersuchung der Temperaturabhängigkeit der Lebensdauer von Triplettexzitonen mittels PIA-Messungen bestätigt. Für Solarzellen ist von Bedeutung, ob sich die Seitenkettenlänge auf die Wechselwirkung zwischen D und A auswirkt. Der vermutete Zusammenhang wird hier nicht bestätigt. Ein ähnlicher Photostrom für alle untersuchten Verbindungen in Solarzellen mit planaren Heteroübergängen unterstreicht diese Schlussfolgerung. Unterschiede im Wirkungsgrad werden auf Änderungen der Energieniveaus und die Morphologie in Mischschichtsolarzellen zurückgeführt. Des Weiteren wird in einer Machbarkeitsstudie der Einfluss des elektrischen Felds auf die Generationsausbeute freier Ladungsträger untersucht. Dafür werden halbtransparente Solarzellen verwendet, die es ermöglichen, PIA-Messungen in Transmissionsgeometrie durchzuführen. Als mögliche Erklärung für das Auftreten zweier Rekombinationskomponenten in der Analyse des Rekombinationsverhaltens der durch Licht erzeugten Ladungsträger werden eingefangene Ladungsträger und gebundene Ladungsträgerpaare an der D/A-Grenzfläche genannt. Das Mischverhalten von D und A kann durch ein Heizen des Substrates während des Verdampfungsprozesses eingestellt werden, was von entscheidender Bedeutung für eine weitere Steigerung des Wirkungsgrades ist. Für DCV4T:C60-Mischschichtsolarzellen wird jedoch eine Verschlechterung des Wirkungsgrads zu höheren Substrattemperaturen beobachtet. Durch optische Messungen und Methoden zur Schichtstrukturbestimmung wird dieser Effekt auf eine Umordnung der DCV4T-Kristallite für hohe Substrattemperaturen und die damit verbundene Verringerung der Absorption und damit auch des Photostroms zurückgeführt. Bei einer Substrattemperatur von 90° C sind die D- und A-Komponenten fast vollständig entmischt. Dieses Beispiel ist von besonderer Bedeutung, weil hier die Ursachen für ein Verhalten aufgezeigt werden, das entgegen den Beispielen aus der Literatur eine Abnahme des Wirkungsgrads beim Aufdampfen der aktiven Schicht auf ein geheiztes Substrat zeigt. Schließlich werden die Optimierungsschritte dargelegt, mit denen Solarzellen mit einer DCV5T-Verbindung als Donatormaterial auf einen Rekordwirkungsgrad von 7,7% gebracht werden. Dabei wird die Substrattemperatur, die Dicke der aktiven Schicht und die Transportschichten angepasst.:Abstract - Kurzfassung Publications Contents 1 Introduction 2 Elementary Processes in Organic Semiconductors 2.1 Introduction 2.2 Optical Excitations in Organic Materials 2.2.1 Introduction 2.2.2 Radiative Processes: Absorption and Emission 2.2.3 Non-radiative Relaxation Processes 2.2.4 Triplet Excitons and Intersystem Crossing 2.3 Polarization Effects and Disorder 2.4 Transport Processes in Disordered Organic Materials 2.4.1 Charge Transport 2.4.1.1 The Bässler Model 2.4.1.2 Marcus Theory for Electron Transfer 2.4.1.3 Small Polaron Model 2.4.1.4 Functional Dependencies of the Charge Carrier Mobility 2.4.2 Diffusive Motion 2.4.3 Exciton Transfer Mechanisms 2.4.4 Characteristics of Exciton Diffusion 2.5 Charge Photogeneration in Pristine Materials 3 Organic Photovoltaics 3.1 General Introduction to Solar Cell Physics 3.2 Introduction to the Donor/Acceptor Heterojunction Concept 3.3 The Open-Circuit Voltage in Organic Solar Cells 3.4 Doping of Organic Semiconductors 3.5 Introduction to the p-i-n Concept 3.6 Charge Transfer Excitons in Donor/Acceptor Heterojunction Systems 3.6.1 Introduction 3.6.2 Verification of Charge Transfer Excitons in Donor/Acceptor Systems 3.7 The Process Cascade for Free Charge Carrier Generation in Donor/Acceptor Heterojunction Systems 3.7.1 The Initial Charge Transfer Step 3.7.2 The Binding Energy of the Charge Transfer Exciton 3.7.3 \"Hot\" Charge Transfer Exciton Dissociation 3.7.4 \"Cold\" Charge Transfer Exciton Dissociation 3.7.5 Supposed Influence Factors on Charge Transfer Exciton Dissociation 3.7.6 Recombination Pathways for Charge Transfer Excitons 3.7.7 Free Charge Carrier Formation and Recombination 4 Experimental Methods 4.1 Sample Preparation 4.2 Material Characterization Methods 4.2.1 Optical Characterization 4.2.2 Cyclic Voltammetry 4.2.3 Ultraviolet Photoelectron Spectroscopy 4.2.4 Atomic Force Microscopy 4.2.5 Grazing Incidence X-Ray Diffraction 4.2.6 Organic Field-Effect Transistor 4.3 Photoinduced Absorption Spectroscopy 4.3.1 Introduction 4.3.2 Derivation of the PIA Signal 4.3.3 Recombination Dynamics 4.3.4 Intensity Dependence of the PIA Signal 4.4 Solar Cell Characterization 4.4.1 External Quantum Efficiency 4.4.2 Spectral Mismatch Correction 4.4.3 Current-Voltage Characteristics 4.4.4 Optical Device Simulations 4.4.5 Optical Device Transmission Measurements 5 The Oligothiophene Material System 5.1 Introduction 5.2 Thermal Stability 5.3 Energy Levels 5.4 Optical Properties of the Pristine Materials 5.5 The Donor/Acceptor Couple: DCVnT and C60 5.6 Solar Cell Devices 5.7 Summary 6 Temperature Dependence of Charge Carrier Generation 6.1 Introduction 6.2 Principal Introduction to the PIA Measurements 6.2.1 Interpretation of the Spectra 6.2.2 Interpretation of the Frequency Scans 6.3 Temperature Dependence of the Spectra 6.4 Discussion of the Temperature Dependent Processes in the Blend Layer 6.5 Temperature Activated Free Charge Carrier Generation 6.5.1 Evaluation of the Activation Energy for the DCV4T-Me:C60 Blend 6.5.2 Comparison to a Sexithiophene Derivative (DCV6T-Me) 6.6 Summary 7 Side Chain Investigation on Quaterthiophene Derivatives 7.1 Energy Levels 7.2 Optical Properties 7.2.1 Solution and Pristine Films 7.2.2 Mixed Films with C60 7.3 Influence of the Side Chain Length on the Intermolecular Coupling 7.3.1 PIA Spectra of Pristine and Blend Layers at 10K 7.3.2 Recombination Analysis for Pristine and Blend Films at 10K 7.4 The Influence of the Side Chain Length on the Offset Charge Carrier Generation Rate at Low Temperature 7.5 In the High-Temperature Limit: Implications for Solar Cell Devices 7.5.1 PIA Spectra in Pristine and Blend Films at 200K 7.5.2 Recombination Analysis: Triplet Excitons and Free Charge Carriers 7.6 Solar Cells 7.6.1 Flat Heterojunction Devices 7.6.2 Bulk Heterojunction Devices 7.7 Summary 8 Electric-Field Dependent PIA Measurements on Complete Solar Cell Devices 8.1 Introduction 8.2 Semitransparent Organic Solar Cells 8.3 Photoinduced Absorption Measurements 8.4 Summary and Outlook 9 The Effect of Substrate Heating During Layer Deposition on the Performance of DCV4T:C60 BHJ Solar Cells 9.1 Introduction 9.2 The Importance of Morphology Control for BHJ Solar Cells 9.3 The Impact of Substrate Heating on DCV4T:C60 BHJ Solar Cells 9.4 Absorption and Photoluminescence 9.5 Topographical Investigations (AFM) 9.6 X-ray Investigations 9.6.1 1D GIXRD Measurements 9.6.2 2D GIXRD Measurements 9.7 Proposed Morphological Picture and Confirmation Measurements 9.7.1 Morphology Sketch of the DCV4T:C60 Blend Layer 9.7.2 Confirmation Measurements 9.8 The Equivalence of Temperature and Time 9.9 Summary 10 Record Solar Cells Using DCV5T-Me33 as Donor Material 10.1 Introduction 10.2 The Influence of the Substrate Temperature 10.3 Determination of the Optical Constants 10.4 Stack Optimization 10.5 Summary and Outlook 11 Conclusions and Outlook 11.1 Summary of the Photophysical Investigations 11.2 Summary of Device Investigations 11.3 Future Challenges Appendix A Detailed Description of the Experimental Setup for PIA Spectroscopy Appendix B Determination of the Triplet Level by Differential PL Measurements Appendix C Additional Tables and Figures Appendix D Reproducibility of the Solar Cell Results (Statistics) Appendix E Lists Bibliography Acknowledgments

Thin coatings of photoresponsive, pyrimidine-terminated molecules, attached to gold or quartz substrates in contact with water, undego photodimerisation and wettability changes when irradiated with UV light at 280 and 240mm. Spin-casting and chemisorption techniques were used to prepare the thin films.
Thesis (PhDApSc)--University of South Australia, 2000.

In der vorliegenden Arbeit wird die neuartige Mikroskopiemethode der Ptychographie für die Untersuchung photorefraktiver Materialien genutzt. Photorefraktive Materialien zeichnen sich durch die Generation lichtinduzierter Brechungsindexänderungen aus. Die Ptychographie bietet die Möglichkeit, neben der generierten Brechungsindexänderung im photorefraktiven Material auch die für die Generation genutzte Intensitätsverteilung des Laserstrahls zu bestimmen. Es wird sowohl die Abhängigkeit der Brechungsindexänderung von der Zeit der Generation als auch die Abhängigkeit von der Polarisation des Lasers gemessen. Durch den Vergleich der gewonnenen Werte mit einer numerischen Simulation des photorefraktiven Effekts werden mikroskopische Parameter der lichtinduzierten Ladungswanderung ermittelt. Zudem wird aus der polarisationsabhängigen ptychographischen Messung das Raumladungsfeld und die korrespondierende Ladungsdichte im Material berechnet. Die Ptychographie liefert damit einen neuen Zugang zum quantitativen Verständnis der Photorefraktivität.:1 Einleitung 2 Theoretische Vorbetrachtungen 2.1 Ptychographie 2.1.1 Messung 2.1.2 Modell und Rekonstruktion 2.1.3 Ortsauflösung 2.2 Photorefraktiver Efekt 2.2.1 Lithiumniobat - Musterbeispiel für die Photorefraktivität 2.2.2 Ein-Zentrum-Modell 2.2.3 Brechungsindexänderung 2.2.4 Hohe Intensitäten 2.3 Raumladungsfeld 2.3.1 Ableitung des Feldes aus den Messgrößen 2.3.2 Raumladungsverteilung 2.3.3 Oberflächendeformation 2.3.4 Dynamik der Ladungen und des Feldes 3 Messungen 3.1 Proben 3.1.1 Ptychographische Teststruktur 3.1.2 LiNbO3:Fe 3.2 Versuchsanordnung 3.2.1 Experimenteller Aufbau 3.2.2 Grenze der Ortsauflösung 3.2.3 Charakterisierung des Laserstrahls 3.2.4 Experimentelle Überprüfung der Näherungen 3.3 Dynamik der Brechungsindexänderung 3.4 Polarisationsabhängigkeit der Brechungsindexänderung 4 Auswertung 4.1 Dynamik des Raumladungsfeldes und der Ladungen 4.1.1 Simulation 4.1.2 Vergleich zwischen Messung und Simulation 4.1.3 Dynamik der Ladungsverteilung 4.1.4 Fazit 4.2 Berechnung des Raumladungsfeldes 4.2.1 Raumladungsfeld und Ladungsverteilung 4.2.2 Simulation 4.2.3 Asymmetrie der Ladungsverteilung 4.2.4 Fazit 5 Zusammenfassung Appendizes A Physikalische Konstanten B Tensoren für LiNbO3 C Ungenäherte Herleitung der Brechungsindexänderung D Implementierung eines iterativen Verfahrens zur Bestimmung der Dynamik des Ein-Zentrum-Modells E Quelltext der Implementierung des iterativen Verfahrens Literaturverzeichnis
In the present thesis the novel microscopy technique of ptychography is applied to the investigation of photorefractive materials. Photorefractive materials exhibit a change of the refractive index due to the exposure to light. The method of ptychography determines the refractive index change of the material together with the intensity distribution of the laser beam that was used for its generation. In one part of the experiment the time dependence of the refractive index change versus the generation time is investigated, in the other part of the experiment the dependence of the refractive index change to the polarisation of the laser beam is examined. Microscopic parameters of the photorefractive charge migration are determined with the utilisation of a numerical simulation of the photorefractive effect and its comparison with the measurement. Finally, the whole space charge field with the corresponding space charge density is calculated from a set of ptychographic measurements of one refractive index change with different polarisation directions of the laser. The presented experiments and their evaluation show, that the method of ptychography opens a new possibility for a quantitative understanding of the photorefractive effect.:1 Einleitung 2 Theoretische Vorbetrachtungen 2.1 Ptychographie 2.1.1 Messung 2.1.2 Modell und Rekonstruktion 2.1.3 Ortsauflösung 2.2 Photorefraktiver Efekt 2.2.1 Lithiumniobat - Musterbeispiel für die Photorefraktivität 2.2.2 Ein-Zentrum-Modell 2.2.3 Brechungsindexänderung 2.2.4 Hohe Intensitäten 2.3 Raumladungsfeld 2.3.1 Ableitung des Feldes aus den Messgrößen 2.3.2 Raumladungsverteilung 2.3.3 Oberflächendeformation 2.3.4 Dynamik der Ladungen und des Feldes 3 Messungen 3.1 Proben 3.1.1 Ptychographische Teststruktur 3.1.2 LiNbO3:Fe 3.2 Versuchsanordnung 3.2.1 Experimenteller Aufbau 3.2.2 Grenze der Ortsauflösung 3.2.3 Charakterisierung des Laserstrahls 3.2.4 Experimentelle Überprüfung der Näherungen 3.3 Dynamik der Brechungsindexänderung 3.4 Polarisationsabhängigkeit der Brechungsindexänderung 4 Auswertung 4.1 Dynamik des Raumladungsfeldes und der Ladungen 4.1.1 Simulation 4.1.2 Vergleich zwischen Messung und Simulation 4.1.3 Dynamik der Ladungsverteilung 4.1.4 Fazit 4.2 Berechnung des Raumladungsfeldes 4.2.1 Raumladungsfeld und Ladungsverteilung 4.2.2 Simulation 4.2.3 Asymmetrie der Ladungsverteilung 4.2.4 Fazit 5 Zusammenfassung Appendizes A Physikalische Konstanten B Tensoren für LiNbO3 C Ungenäherte Herleitung der Brechungsindexänderung D Implementierung eines iterativen Verfahrens zur Bestimmung der Dynamik des Ein-Zentrum-Modells E Quelltext der Implementierung des iterativen Verfahrens Literaturverzeichnis