905 resultados para soft lithography


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Nanocyrstalline LaGaO3 and Dy3+- and Eu3+-doped LaGaO3 were prepared through a Pechini-type sol-gel process. X-ray diffraction (XRD), field emission scanning electron microscopy (FE-SEM), photoluminescence, cathodoluminescence spectra, and lifetimes were utilized to characterize the samples. XRD reveals that the samples begin to crystallize at 900 degrees C and pure LaGaO3 phase can be obtained at 1000 degrees C. FE-SEM images indicate that the Dy3+- and Eu3+-doped LaGaO3 samples are both composed of aggregated spherical particles with sizes ranging from 40 to 80 nm. Under the excitation of ultraviolet light and low voltage electron beams (1-5 kV), the undoped LaGaO3 sample shows a strong blue emission peaking at 433 nm, and the Dy3+- and Eu3+-doped LaGaO3 samples show their characteristic emissions of Dy3+ (F-4(9/2)-H-6(15/2) and F-4(9/2)-H-6(13/2) transitions) and Eu3+ (D-5(0,1,2)-F-7(1,2,3,4) transitions), respectively. The relevant luminescence mechanisms are discussed.

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Nanocrystalline CaTiO3:Pr3+ phosphor layers were coated on nonaggregated, monodisperse, and spherical SiO2 particles by the sol-gel method, resulting in the formation of core-shell structured SiO2-CaTiO3:Pr3+ particles. X-ray diffraction, Fourier transform infrared spectroscopy, field emission scanning electron microscopy, transmission electron microscopy, photoluminescence, cathodoluminescence spectra, as well as lifetimes were utilized to characterize the core-shell structured SiO2-CaTiO3:Pr3+ phosphor particles. The obtained core-shell structured phosphors consist of well dispersed submicron spherical particles with a narrow size distribution. The thickness of the CaTiO3:Pr3+ shell could be easily controlled by changing the number of deposition cycles (about 70 nm for four deposition cycles). The core-shell SiO2-CaTiO3:Pr3+ particles show a strong red emission corresponding to D-1(2)-H-3(4) (612 nm) of Pr3+ under the excitation of ultraviolet (326 nm) and low voltage electron beams (1-5 kV). These particles may be used in field emission displays.

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A uniform nanolayer of europium-doped Gd2O3 was coated on the surface of preformed submicron silica spheres by a Pechini sol-gel process. The resulted SiO2@Gd2O3:Eu3+ core-shell structured phosphors were characterized by X-ray diffraction (XRD), Fourier transform infrared spectroscopy (FT-IR), field emission scanning electron microscopy (FESEM), transmission electron microscopy (TEM), photoluminescence (PL) spectra as well as kinetic decays. The XRD results show that the Gd2O3:Eu3+ layers start to crystallize on the SiO2 spheres after annealing at 400 degrees C and the crystallinity increases with raising the annealing temperature. The core-shell phosphors possess perfect spherical shape with narrow size distribution (average size: 640 nm) and non-agglomeration. The thickness of the Gd2O3:Eu3+ shells on the SiO2 cores can be adjusted by changing the deposition cycles (70 nm for three deposition cycles). Under short UV excitation, the obtained SiO2@Gd2O3:Eu3+ particles show a strong red emission with D-5(0)-F-7(2) (610 nm) of Eu3+ as the most prominent group.The PL intensity of Eu3+ increases with increasing the annealing temperature and the number of coating cycles.

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Micropatterning of functional polymer materials by micromolding in capillaries (MIMIC) with ice mold is reported in this paper. Ice mold was selected due to its thaw or sublimation. Thus, the mold can be easily removed. Furthermore, the polymer solution did not react with, swell, or adhere to the ice mold, so the method is suitable for many kinds of materials (such as P3HT, PMMA Alq(3)/PVK, PEDOT: PSS, PS, P2VP, etc.). Freestanding polymer microstructures, binary polymer pattern, and microchannels have been fabricated by the use of ice mold freely.

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Rare-earth ion (Eu3+, Tb3+, Ce3+)- doped LaPO4 nanocrystalline thin films and their patterning were fabricated by a Pechini sol-gel process combined with soft lithography on silicon and silica glass substrates. X-Ray diffraction (XRD), Fourier transform infrared spectroscopy (FT-IR), thermogravimetric and differential thermal analysis (TG-DTA), atomic force microscopy (AFM), scanning electron microcopy (SEM), optical microscopy, absorption and photoluminescence (PL) spectra as well as lifetimes were used to characterize the resulting films. The results of XRD indicate that the films begin to crystallize at 700 degreesC and the crystallinity increases with increasing annealing temperature. The morphology of the thin film depends on the annealing temperature and the number of coating layers. The 1000 degreesC annealed single layer film is transparent to the naked eye, uniform and crack-free with a thickness of about 200 nm and an average grain size of 100 nm. Patterned thin films with different strip widths ( 5 - 50 mm) were obtained by micromolding in capillaries ( soft lithography). The doped rare earth ions show their characteristic emission in the nanocrystalline LaPO4 films, i.e., Eu3+ D-5(0)-F-7(J) (J = 1, 2, 3, 4), Tb3+ D-5(3,4) - F-7(J) ( J = 6, 5, 4, 3, 2) and Ce3+ 5d-4f transition emissions, respectively. Both the lifetimes and the PL intensities of Eu3+ and Tb3+ increase with increasing annealing temperature, and the optimum concentrations for them were determined to be 5 mol% and 16 mol% of La3+ in LaPO4 thin films, respectively. An energy transfer phenomenon from Ce3+ to Tb3+ has been observed in LaPO4 nanocrystalline thin films, and the energy transfer efficiency depends on the doping concentration of Tb3+ if the concentration of Ce3+ is fixed.

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Ce3+ and/or Tb3+-doped LaPO4 nanocrystalline thin films and their patterning were fabricated by a sol-gel process combined with soft lithography on silicon and quartz glass substrates. The results of XRD indicated that the films began to crystallize at 700 degreesC. The 1000 degreesC annealed single layer films are transparent by eyes, uniform and crack-free with a thickness of about 200 nm and an average grain size of 100 nm. Patterned thin film with different band widths (5-50 mum) were obtained by micro-molding in capillaries technique. The luminescence and energy transfer properties of Ce3+ and Tb3+ were studied in LaPO4 films.

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The fabrication of multilayer microstructures, for example for organic field-effect transistors, using metal transfer printing (MTP) is demonstrated. The Figure shows a two-layer gold structure produced by MTP. Since MTP is a purely additive technique, in which mechanical adhesion acts as the patterning driving force, it is considered an attractive approach to reel-to-reel processing.

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The pattern evolution processes of thin polystyrene (PS) film on chemically patterned substrates during dewetting have been investigated experimentally. The substrates have patterns of self-assembly monolayers produced by microcontact printing with octadecyltrichlorosilane. Optical microscopy and atomic force microscopy images reveal that ordered micrometer scale pattern can be created by surface direct dewetting. Various pattern sizes and pattern complexities can be achieved by controlling the experimental parameters. The dewetting pattern has been transferred to form PDMS stamp for soft lithography.

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Microtransfer molding (muTM) is a kind of soft lithography for polymer micropatterning. In muTM, a liquid prepolymer(or concentrated polymer solution) is applied to the patterned surface of an elastomeric mold and then brought into the contact with a substrate. After prepolymer is cured thermally or by UV light, the elastomeric mold is peeled away. A pattern is left on the surface of the substrate. In this study, similar to300 nm lines and three-dimensional patterns of PMMA and epoxy on planar and/or non-planar substrates are realized.

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Polydimethylsiloxane (PDMS) is the elastomer of choice to create a variety of microfluidic devices by soft lithography techniques (eg., [1], [2], [3], [4]). Accurate and reliable design, manufacture, and operation of microfluidic devices made from PDMS, require a detailed characterization of the deformation and failure behavior of the material. This paper discusses progress in a recently-initiated research project towards this goal. We have conducted large-deformation tension and compression experiments on traditional macroscale specimens, as well as microscale tension experiments on thin-film (≈ 50µm thickness) specimens of PDMS with varying ratios of monomer:curing agent (5:1, 10:1, 20:1). We find that the stress-stretch response of these materials shows significant variability, even for nominally identically prepared specimens. A non-linear, large-deformation rubber-elasticity model [5], [6] is applied to represent the behavior of PDMS. The constitutive model has been implemented in a finite-element program [7] to aid the design of microfluidic devices made from this material. As a first attempt towards the goal of estimating the non-linear material parameters for PDMS from indentation experiments, we have conducted micro-indentation experiments using a spherical indenter-tip, and carried out corresponding numerical simulations to verify how well the numerically-predicted P(load-h(depth of indentation) curves compare with the corresponding experimental measurements. The results are encouraging, and show the possibility of estimating the material parameters for PDMS from relatively simple micro-indentation experiments, and corresponding numerical simulations.

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The non-Newtonian flow of dilute aqueous polyethylene oxide (PEO) solutions through microfabricated planar abrupt contraction-expansions is investigated. The contraction geometries are fabricated from a high-resolution chrome mask and cross-linked PDMS gels using the tools of soft-lithography. The small length scales and high deformation rates in the contraction throat lead to significant extensional flow effects even with dilute polymer solutions having time constants on the order of milliseconds. The dimensionless extra pressure drop across the contraction increases by more than 200% and is accompanied by significant upstream vortex growth. Streak photography and videomicroscopy using epifluorescent particles shows that the flow ultimately becomes unstable and three-dimensional. The moderate Reynolds numbers (0.03 ≤ Re ≤ 44) associated with these high Deborah number (0 ≤ De ≤ 600) microfluidic flows results in the exploration of new regions of the Re-De parameter space in which the effects of both elasticity and inertia can be observed. Understanding such interactions will be increasingly important in microfluidic applications involving complex fluids and can best be interpreted in terms of the elasticity number, El = De/Re, which is independent of the flow kinematics and depends only on the fluid rheology and the characteristic size of the device.

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The aim of my dissertation is to provide new knowledge and applications of microfluidics in a variety of problems, from materials science, devices, and biomedicine, where the control on the fluid dynamics and the local concentration of the solutions containing the relevant molecules (either materials, precursors, or biomolecules) is crucial. The control of interfacial phenomena occurring in solutions at dierent length scales is compelling in nanotechnology for devising new sensors, molecular electronics devices, memories. Microfluidic devices were fabricated and integrated with organic electronics devices. The transduction involves the species in the solution which infills the transistor channel and confined by the microfluidic device. This device measures what happens on the surface, at few nanometers from the semiconductor channel. Soft-lithography was adopted to fabricate platinum electrodes, starting from platinum carbonyl precursor. I proposed a simple method to assemble these nanostructures in periodic arrays of microstripes, and form conductive electrodes with characteristic dimension of 600 nm. The conductivity of these sub-microwires is compared with the values reported in literature and bulk platinum. The process is suitable for fabricating thin conductive patterns for electronic devices or electrochemical cells, where the periodicity of the conductive pattern is comparable with the diusion length of the molecules in solution. The ordering induced among artificial nanostructures is of particular interest in science. I show that large building blocks, like carbon nanotubes or core-shell nanoparticles, can be ordered and self-organised on a surface in patterns due to capillary forces. The eective probability of inducing order with microfluidic flow is modeled with finite element calculation on the real geometry of the microcapillaries, in soft-lithographic process. The oligomerization of A40 peptide in microconfined environment represents a new investigation of the extensively studied peptide aggregation. The added value of the approach I devised is the precise control on the local concentration of peptides together with the possibility to mimick cellular crowding. Four populations of oligomers where distinguished, with diameters ranging from 15 to 200 nm. These aggregates could not be addresses separately in fluorescence. The statistical analysis on the atomic force microscopy images together with a model of growth reveal new insights on the kinetics of amyloidogenesis as well as allows me to identify the minimum stable nucleus size. This is an important result owing to its implications in the understanding and early diagnosis and therapy of the Alzheimer’s disease

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Die vorliegende Arbeit beschreibt unter anderem die Realisierung eines Assays aus mikrostrukturierten und selektiv funktionalisierten künstlichen Membransegmenten auf einem Chip. Die Strukturierungsmethode kombiniert die softlithographische Technik des Mikroformens in Kapillaren mit der Vesikelspreittechnik und bietet ein elegantes Verfahren, einzeln adressierbare Lipidsegmente im Mikrometer Regime zu erzeugen. Unter Berücksichtigung des hydrodynamischen Fließverhaltens und der Stabilitätskriterien für PDMS-Elastomere wurden außerdem neue Strukturen entwi-ckelt, die für den kombinierten Einsatz von Rasterkraftmikroskopie und Fluoreszenz-mikroskopie optimiert sind. Die Anwendbarkeit des Lab-On-A-Chip-Devices als Bio-sensor wurde durch zwei prominente Protein-Rezeptor-Bindungsstudien fluores-zenzmikroskopisch und rasterkraftmikroskopisch belegt. Im zweiten Teil der Arbeit sind die mechanischen und adhäsiven Eigenschaften aus-gewählter Lipidsysteme mit einer neuen Charakterisierungstechnik untersucht wor-den, die die Kontaktmechanik von Rastersonden und Lipidmembranen auf Basis der Digitalisierung von Hochgeschwindigkeitskraftkurven und einer automatisierten Multi-parameteranalyse quantitativ erfasst. Dabei konnte die Korrelation zwischen der Ad-häsion und den materialspezifischen Durchbruchlängen und Durchbruchkräften, die charakteristische Stabilitätsparameter der Lipidmembran darstellen, auf Systemen mit variierenden Kopfgruppen und Kettenlängen analysiert werden. Das Verfahren erlaubte zudem die simultane Quantifizierung der elastischen Eigenschaften der Li-piddoppelschichten. Zu den Kraftkurven wurden Simulationen der Systemantwort durchgeführt, die ein tieferes Verständnis der Kontrastentstehung ermöglichen.

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Grundlage für die hier gezeigte Arbeit stellt die Eigenschaft von amphiphilen Blockcopolymeren dar immer den Block mit der niedrigsten Grenzflächenenergie zum angrenzenden Medium an die Oberfläche zu bringen. Durch einen Austausch des Mediums an der Grenzfläche zum Blockcopolymer kann eine Reorientierung erzwungen werden, wenn die Grenzflächenenergie des anderen Blocks nun die niedrigere Grenzflächenenergie besitzt. Dieses Verhalten von dünnen amphiphilen Blockcopolymerfilmen wurde zur Strukturierung von Oberflächen ausgenutzt und in nachfolgenden Synthesen weiter verstärkt. Um dies zu erreichen wurde das zur Strukturierung erforderliche Poly(4-Octylstyrol)block(4-hydroxystyrol) durch kontrollierte radikalische Polymerisationsmethode mit dem Tempo Unimer (2,2,6,6-Tetramethyl-1-1(1-phenyl-ethoxy)-piperidin) synthetisiert. Für die geplanten Reorientierungen und Modifizierungen von Oberflächen wurden dünne Filme durch Schleuderbeschichtung auf verschiedenen Substraten (Siliziumwafern, Glassubstraten und Goldoberflächen) hergestellt. Das Verhalten der Oberflächen von diesen Filmen wurde durch Kontaktwinkelmessungen untersucht. Auf diese Weise konnte gezeigt werden, dass die Oberfläche von Polymerfilmen nach der Präparation aus dem hydrophoben Block des Polymers gebildet wird. Durch Kontakt des Polymerfilms mit Wasser kann dieser zur Reorientierung gebracht werden, so dass der hydrophile Block des Polymers an der Oberfläche erscheint. Dieses Verhalten wurde zur Strukturierung mit softlithographischen Techniken genutzt. Dazu wurden hydrophil/hydrophob strukturierte Oberflächen durch Aufsetzen von hydrophoben PDMS-Stempeln, die Teile der Oberfläche selektiv abdeckten, und Einbringen von Wasser in die dabei entstehenden Kapillaren hergestellt. Dies ermöglichte es die Oberfläche selektiv im Größenbereich von 500nm bis zu 50µm zu strukturieren und an den reaktiven Bereichen Materialien, wie z.B. Kupfer, Titandioxid, Polyelektrolyte, photonische Kristalle und angegraftete Polymere, mit verschiedenen Methoden selektiv auf die Oberfläche aufzubringen. Um den Reorganisationsprozess der Oberfläche genauer zu studieren, wurde ein für diese Aufgabe besser geeignetes Polymer (Poly(Styrol)-block-poly(essigsäure-2-(2-(4-vinyl-phenoxy)-ethoxy)ethylester)) synthetisiert. Aus diesem Blockcopolymer wurden wieder dünne Filme durch Spincoaten hergestellt. Die Reorientierung dieses Polymers in 70°C warmen Wasser konnte durch Kontaktwinkelmessungen und NEXAFS Spektroskopie nachgewiesen werden. Mit Hilfe der NEXAFS Spektroskopie konnte festgestellt werden, dass die Geschwindigkeit der Reorientierung durch eine exponentielle Funktion beschrieben werden kann. Eine Auswertung der Geschwindigkeitskonstante für die Reorientierung einer hydrophilen zu einer hydrophoben Oberfläche des Polymers bei 60°C führt zu =75min. Aufgrund des exponentiellen Charakters der Reorientierung macht es den Anschein, dass die Reorientierung bei verschiedenen Reorientierungstemperaturen bis zu einem gewissen Grad erfolgt und dann stoppt. Eine weitere Reorientierung scheint erst wieder bei einer Temperaturerhöhung zu beginnen. Aus AFM Messungen ist ein Beginnen der Reorientierung durch Bildung kleiner Löcher in der Polymeroberfläche zu erkennen, die sich zu runden Erhöhungen und Vertiefungen vergrößern, um letztendlich in ein spinodales Entmischungsmuster über zu gehen. Dieses heilt dann im Laufe der Zeit langsam durch Verschwinden der hydrophilen Bereiche langsam aus. Der Beginn des zuvor beschriebenen Reorientierungsprozesses einer hydrophilen Oberfläche in eine hydrophobe konnte sowohl in den AFM, als auch in den NEXAFS-Messungen zu ca. 50°C bestimmt werden.