912 resultados para LADDER POLYMERS
Resumo:
A series of acene-type conjugated molecules(1-5) containing 2-6 pyrazine units and up to 16 rectilinearly arranged fused aromatic rings were synthesized by condensation coupling of 1,2-diamines and 1,2-diketones. The energy gap of the molecules estimated from absorption edge decreases with an increase in molecular length, indicating the well-delocalized nature of the molecules. The cyclic voltarnmetry measurements suggest that the n-type properties of these ribbonlike pyrazine derivatives are dependent on the molecular length and the number of the pyrazine units.
Resumo:
Zusammenfassung: Im Rahmen der Arbeit wird über die Darstellung neuartiger, konjugierter Polyarylene mit Leiterstruktur berichtet. Über eine zweistufige Synthese wurde ein ethylenüberbrücktes Leiterpolymer (LPDP) hergestellt. Dabei wurde das Vorläuferpolymer mit Samarium(II)jodid unter milden Bedingungen zum Leiterpolymeren cyclisiert. Erste Untersuchungen zeigen, daß LPDP im Gegensatz zum 'gewinkelten Polyacen' eine sehr vielversprechende Elektrolumineszenz-Eigenschaft besitzt. Durch den Einbau chiraler Alkylsubstituenten in entsprechenden meta-Phenylen-Analoga der Leiterpolymere vom Polyacen-Typ wurde versucht, eine Vorzugsdrehrichtung der helikalen Leiterpolymere im Laufe der polymeranalogen Cyclisierung zu induzieren. Es zeigt sich, daß für eines der chiralen Derivate ein CD-Effekt im Bereich der Absorption der helikalen Polyacen-Hauptkette auch auf molekularer Ebene auftritt. Weiterhin wird die erfolgreiche Synthese eines neuen, heteroaromatischen Leiterpolymeren, LPPPT, beschrieben, welches alternierend aus 1,4-Phenylen- und 2,5-Thienylen-Einheiten aufgebaut ist. Eine LED in der Konfiguration ITO/LPPPT/Al zeigt eine orange Lichtemission. Die Quanteneffizienz der freien Ladungsträgerbildung für LPPPT wurde in Experimenten zur Ladungstraegergeneration im elektrischen Feld (Coronaentladung) zu ca. 1 % bei 10E7 V/m bestimmt. Letztlich wurde die Synthese eines neuen, heteroaromatischen Leiterpolymeren mit Carbazol-Einheiten, LPPPC, in der Hauptkette beschrieben, das alternierend aus 1,4-Phenylen- und Carbazol-3,6-diyl-Einheiten aufgebaut ist. Untersuchungen am LPPPC ergaben, daß das Polymer gute Lochleitereigenschaften besitzt, daneben weisen dünne Filme von LPPPC auch photovoltaische Eigenschaften auf.
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Im Rahmen dieser Arbeit wurden Darstellung und elektronische Anwendungsmöglichkeiten von neuartigen stickstoff- und damit elektronenreichen Poly(para-phenylenen) untersucht. Der Teilbereich „Polycarbazole“ befasst sich mit der Synthese von konjugierten (Stufen)leiterpolymeren auf der Basis von Carbazol. Dazu wurde ein neuer und effizienter Syntheseweg zur Gewinnung von 2,7-Dibromcarbazol entwickelt. Durch die weitere Funktionalisierung von 2,7-Dibromcarbazol gelang es, elektronenreiche Leiterpolymere zu gewinnen, die eine grüne Emissionsfarbe aufwiesen. Mit der Verwendung von R = 2-Decyltetradecyl als löslichkeitsfördernder Seitenkette in einem Poly(2,7-carbazol) konnte erstmals ein hochmolekulares Polycarbazol gewonnen werden. Dieses gut lösliche Poly(2,7-carbazol) erwies sich als ein exzellentes Donatormaterial in Solarzellen, welches in Kombination mit dem Farbstoff PDI eine effiziente Solarzelle ergab. Eine OLED mit einem neuartigen arylierten Polycarbazol als Emittermaterial zeigte eine sehr niedrige Turn-on-Spannung und eine intensive blaue EL-Emission. Das Kapitel über imidazolhaltige Poly(para-phenylene) und Discoten stellt die Darstellung von planarisierten Bisimidazolen vor, welche in hohen Ausbeuten durch eine intramolekulare Buchwald-Reaktion zwischen den Imidazolringen und der zentralen Terphenyleinheit durchgeführte wurde. Die dreistufige Darstellung der Discoten aus einem Terephthalaldehyd-Derivat und einem Benzil erlaubt eine einfache sowie variable Einführung von löslichkeitsfördernden Alkylsubstituenten. Auf diese Weise ist der Zugang zu einer völlig neuartigen Klasse an discotischen Materialien möglich, die eine Kombination aus Discoten auf der Basis von Benzolringen (wie z.B. HBC) mit Heteroaromaten darstellen. Die gewonnenen scheibenförmigen Bisimidazole wiesen dementsprechend auf Selbstanordnung zurückzuführende kolumnare Anordnungen und hexagonale Überstrukturen auf. Im dritten Themengebiet wird der Einbau eines Phthalimidchromophors direkt in das Rückgrad von Polyanilin vorgestellt. Da jegliche Veränderung des Oxidationsgrades zu einer unterschiedlichen Donatorfähigkeit des Polyanilinhauptkette führt, variiert in Abhängigkeit davon das Absorptionsverhalten des eingebauten Farbstoffes. Durch die Einführung des Phthalimidchromophores war es zudem möglich, ein leitfähiges Polymer zu erhalten, das im Gegensatz zum nicht-fluoreszierenden Polyanilin eine intensive gelbe Fluoreszenz (lmax = 547 nm) aufweist.
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Ion implantation can be used to confer electrical conductivity upon conventional insulating polymers such as polyetheretherketone (PEEK). We have implanted PEEK films using three different types of ion implantation: conventional inert gas and metal ion implantation, and ion beam mixing. We have applied a number of analytical techniques to compare the chemical, structural and electrical properties of these films. The most effective means of increasing electrical conductivity appears to be via ion beam mixing of metals into the polymer, followed by metal ion implantation and finally, inert gas ion implantation. Our results suggest that in all cases, the conducting region corresponds to the implanted layer in the near surface to a depth of similar to750 Angstrom (ion beam mixed) to similar to5000 Angstrom (metal ion). This latter value is significantly higher than would be expected from a purely ballistic standpoint, and can only be attributed to thermal inter-diffusion. Our data also indicates that graphitic carbon is formed within the implant region by chain scission and subsequent cross-linking. All ion implanted samples retained their bulk mechanical properties, i.e. they remained flexible. The implant layers showed no signs of de-lamination. We believe this to be the first comparative study between different implantation techniques, and our results support the proposition that soft electronic circuitry and devices can be created by conductivity engineering with ion beams. (C) 2004 Elsevier B.V. All rights reserved.
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Two new cadmium (II) complexes [Cd(hmt)(dca)(2)] (n) (1) and [Cd-3(hmt)(2)(SeCN)(6)(H2O)(2)] (n) (2) (hmt=hexamethylenetetramine, dca=dicyanamide) have been synthesized and characterized by X-ray single-crystal analysis. The complex 1 is a 2D rectangular grid of octahedral cadmium (II) with CdN6 chromophore where cadmium centers are doubly bridged by dicyanamide and hmt along a-axis, which are interlinked by dicyanamide running along c-axis. Whereas, complex 2 is a 1D chain of octahedral cadmium (II) with a three-leg ladder topology running along a-axis. The Cd(II) centers are doubly bridged through SeCN (infinite rail) along a-axis and singly bridged by hmt (two-step rung) along c-axis, having cadmium centers with CdSe2N3O and CdSe2N4 chromophores. The adjacent chains through H-bonding between coordinated water and hmt, and (SeSe)-Se-... interaction are extended to 2D supramolecular architecture.
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Currently pi-conjugated polymers are considered as technologically interesting materials to be used as functional building elements for the development of the new generation of optoelectronic devices. More specifically during the last few years, poly-p-phenylene materials have attracted considerable attention for their blue photoluminescence properties. This Thesis deals with the optical properties of the most representative blue light poly-p-phenylene emitters such as poly(fluorene), oligo(fluorene), poly(indenofluorene) and ladder-type penta(phenylene) derivatives. In the present work, laser induced photoluminescence spectroscopy is used as a major tool for the study of the interdependence between the dynamics of the probed photoluminescence, the molecular structures of the prepared polymeric films and the presence of chemical defects. Complementary results obtained by two-dimensional wide-angle X-ray diffraction are reported. These findings show that the different optical properties observed are influenced by the intermolecular solid-state interactions that in turn are controlled by the pendant groups of the polymer backbone. A significant feedback is delivered regarding the positive impact of a new synthetic route for the preparation of a poly(indenofluorene) derivative on the spectral purity of the compound. The energy transfer mechanisms that operate in the studied systems are addressed by doping experiments. After the evaluation of the structure/property interdependence, a new optical excitation pathway is presented. An efficient photon low-energy up-conversion that sensitises the blue emission of poly(fluorene) is demonstrated. The observed phenomenon takes place in poly(fluorene) derivatives hosts doped with metallated octaethyl porphyrins, after quasi-CW photoexcitation of intensities in the order of kW/cm2. The up-conversion process is parameterised in terms of temperature, wavelength excitation and central metal cation in the porphyrin ring. Additionally the observation of the up-conversion is extended in a broad range of poly-p-phenylene blue light emitting hosts. The dependence of the detected up-conversion intensity on the excitation intensity and doping concentration is reported. Furthermore the dynamics of the up-conversion intensity are monitored as a function of the doping concentration. These experimental results strongly suggest the existence of triplet-triplet annihilation events into the porphyrin molecules that are subsequently followed by energy transfer to the host. After confirming the occurrence of the up-conversion in solutions, cyclic voltammetry is used in order to show that the up-conversion efficiency is partially determined from the energetic alignment between the HOMO levels of the host and the dopant.
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Films of piezoelectric PVDF and P(VDF-TrFE) were exposed to vacuum UV (115-300 nm VUV) and -radiation to investigate how these two forms of radiation affect the chemical, morphological, and piezoelectric properties of the polymers. The extent of crosslinking was almost identical in both polymers after -irradiation, but surprisingly, was significantly higher for the TrFE copolymer after VUV-irradiation. Changes in the melting behavior were also more significant in the TrFE copolymer after VUV-irradiation due to both surface and bulk crosslinking, compared with only surface crosslinking for the PVDF films. The piezoelectric properties (measured using d33 piezoelectric coefficients and D-E hysteresis loops) were unchanged in the PVDF homopolymer, while the TrFE copolymer exhibited more narrow D-E loops after exposure to either - or VUV-radiation. The more severe damage to the TrFE copolymer in comparison with the PVDF homopolymer after VUV-irradiation is explained by different energy deposition characteristics. The short wavelength, highly energetic photons are undoubtedly absorbed in the surface layers of both polymers, and we propose that while the longer wavelength components of the VUV-radiation are absorbed by the bulk of the TrFE copolymer causing crosslinking, they are transmitted harmlessly in the PVDF homopolymer.
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Poly(vinylidene fluoride) and copolymers of vinylidene fluoride with hexafluoropropylene, trifluoroethylene and chlorotrifluoroethylene have been exposed to gamma irradiation in vacuum, up to doses of 1MGy under identical conditions, to obtain a ranking of radiation sensitivities. Changes in the tensile properties, crystalline melting points,heats of fusion, gel contents and solvent uptake factors were used as the defining parameters. The initial degree of crystallinity and film processing had the greatest influence on relative radiation damage, although the cross-linked network features were almost identical in their solvent swelling characteristics, regardless of the comonomer composition or content.
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The effects of atomic oxygen (AO) and vacuum UV radiation simulating low Earth orbit conditions on two commercially available piezoelectric polymer films, poly(vinylidene fluoride) (PVDF) and poly(vinylidene fluoride-trifluoroethylene) P(VDF-TrFE), have been studied. Surface erosion and pattern development are significant for both polymers. Erosion yields were determined as 2.8 � 10�24 cm3/atom for PVDF and 2.5 � 10�24 cm3/atom for P(VDF-TrFE). The piezoelectric properties of the residual material of both polymers were largely unchanged after exposure, although a slight shift in the Curie transition of the P(VDF-TrFE) was observed. A lightly cross-linked network was formed in the copolymer presumably because of penetrating vacuum ultraviolet (VUV) radiation, while the homopolymer remained uncross-linked. These differences were attributed to varying degrees of crystallinity and potentially greater absorption, and hence damage, of VUV radiation in P(VDFTrFE) compared with PVDF.
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Smart materials, such as thin-film piezoelectric polymers, are interesting for potential applications on Gossamer spacecraft. This investigation aims to predict the performance and long-term stability of the piezoelectric properties of poly(vinylidene fluoride) (PVDF) and its copolymers under conditions simulating the low-Earthorbit environment. To examine the effects of temperature on the piezoelectric properties of PVDF, poly(vinylidenefluoride-co-trifluoroethylene), and poly(vinylidenefluoride-cohexafluoropropylene), the d33 piezoelectric coefficients were measured up to 160 8C, and the electric displacement/electric field (D–E) hysteresis loops were measured from �80 to þ110 8C. The room-temperature d33 coefficient of PVDF homopolymer films, annealed at 50, 80, and 125 8C, dropped rapidly within a few days of thermal exposure and then remained unchanged. In contrast, the TrFE copolymer exhibited greater thermal stability than the homopolymer, with d33 remaining almost unchanged up to 125 8C. The HFP copolymer exhibited poor retention of d33 at temperatures above 80 8C. In situ D–E loop measurements from �80 to þ110 8C showed that the remanent polarization of the TrFE copolymer was more stable than that of the PVDF homopolymer. D–E hysteresis loop and d33 results were also compared with the deflection of the PVDF homopolymer and TrFE copolymer bimorphs tested over a wide temperature range.
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Various piezoelectric polymers based on polyvinylidene fluoride (PVDF) are of interest for large aperture space-based telescopes. Dimensional adjustments of adaptive polymer films depend on charge deposition and require a detailed understanding of the piezoelectric material responses which are expected to deteriorate owing to strong vacuum UV, � -, X-ray, energetic particles and atomic oxygen exposure. We have investigated the degradation of PVDF and its copolymers under various stress environments detrimental to reliable operation in space. Initial radiation aging studies have shown complex material changes with lowered Curie temperatures, complex material changes with lowered melting points, morphological transformations and significant crosslinking, but little influence on piezoelectric d33 constants. Complex aging processes have also been observed in accelerated temperature environments inducing annealing phenomena and cyclic stresses. The results suggest that poling and chain orientation are negatively affected by radiation and temperature exposure. A framework for dealing with these complex material qualification issues and overall system survivability predictions in low earth orbit conditions has been established. It allows for improved material selection, feedback for manufacturing and processing, material optimization/stabilization strategies and provides guidance on any alternative materials.
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Piezoelectric polymers based on polyvinylidene flouride (PVDF) are of interest as adaptive materials for large aperture space-based telescopes. In this study, two piezoelectric polymers, PVDF and P(VDF-TrFE), were exposed to conditions simulating the thermal, radiative and atomic oxygen conditions of low Earth orbit. The degradation pathways were governed by a combination of chemical and physical degradation processes with the molecular changes primarily induced via radiative damage, and physical damage from temperature and atomic oxygen exposure, as evident from depoling, loss of orientation and surface erosion. The piezoelectric responsiveness of each polymer was strongly dependent on exposure temperature. Radiation and atomic oxygen exposure caused physical and chemical degradation, which would ultimately cause terminal damage of thin films, but did not adversely affect the piezoelectric properties.