992 resultados para enhancement factor


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The present paper describes the use of sugar cane bagasse as solid phase extractor for cadmium determination after complexation of the analyte with ammonium diethyldithiophosphate (ADDP) and sorption of the Cd-DDP complexes on the solid support. The concomitants were separated using a flow injection analysis (FIA) system coupled to flame atomic absorption spectrometry (FAAS) for determination. The main parameters such as ADDP concentration, acid medium, flow rate, reaction coil length, and reaction time were investigated.The results obtained with HNO3 showed good accuracy and precision. The enhancement factor was 20.5 times for a 120-second preconcentration time, and the analytical frequency was 25 determinations per hour. The calibration curve was linear over the concentration range of 1-40 mu g L-1 Cd with a LOD of 0.697 mu g L-1 Cd and a relative standard deviation of 0.96% after 12 successive measurements of 30 mu g L-1 Cd.The proposed method was evaluated for the FIA-FAAS analysis of certified reference materials (tomato leaves, spinach leaves, and bovine liver) and Cd-spiked foods (shrimp, sardine, tuna, chicken liver and bovine liver). Good recoveries (80.0-97.1%) for the Cd-spiked samples and certified reference materials were obtained. The results of bagasse-packed minicolumns were compared with Si-C,8 packed minicolumns. The F-test was applied between Si-C-18/Bagasse minicolumns, Si-C-18/certified values, and bagasse/certified values. It was found that the results were in agreement with the certified values at a 95% confidence level.

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The vibrational spectra of palladium phthalocyanine (PdPc) evaporated thin solid films are reported, including the resonance Raman scattering, surface-enhanced resonance Raman scattering (SERRS) and SERRS mapping of the film surface using micro-Raman spectroscopy with 633 nm laser radiation. SERRS of PdPc was obtained by evaporating an overlayer of Ag nanoparticles on to the PdPc film on glass. The SERRS enhancement factor is estimated as similar to10(4) with reference to PdPc evaporated films on glass. The molecular organization of the PdPc evaporated films was probed using transmission and reflection-absorption infrared spectra. It was established that a random molecular distribution found in PdPc evaporated films is independent of temperature. No evidence of thermal degradation due to thermal annealing was found in the films. Electronic absorption and emission spectra are also discussed. Copyright (C) 2002 John Wiley Sons, Ltd.

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Time-of-flight photoemission spectromicroscopy was used to measure and compare the two-photon photoemission (2PPE) spectra of Cu and Ag nanoparticles with linear dimensions ranging between 40 nm and several 100 nm, with those of the corresponding homogeneous surfaces. 2PPE was induced employing femtosecond laser radiation from a frequency-doubled Ti:sapphire laser in the spectral range between 375 nm and 425 nm with a pulse width of 200 fs and a repetition rate of 80 MHz. The use of a pulsed radiation source allowed us to use a high-resolution photoemission electron microscope as imaging time-of-flight spectrometer, and thus to obtain spectroscopic information about the laterally resolved electron signal. Ag nanoparticle films have been deposited on Si(111) by electron-beam evaporation, a technique leading to hemispherically-shaped Ag clusters. Isolated Cu nanoparticles have been generated by prolonged heating of a polycrystalline Cu sample. If compared to the spectra of the corresponding homogeneous surfaces, the Cu and Ag nanoparticle spectra are characterized by a strongly enhanced total 2PPE yield (enhancement factor up to 70), by a shift (about 0.1 eV) of the Fermi level onset towards lower final state energies, by a reduction of the work function (typically by 0.2 eV) and by a much steeper increase of the 2PPE yield towards lower final state energies. The shift of the Fermi level onset in the nanoparticle spectra has been explained by a positive unit charge (localized photohole) residing on the particle during the time-scale relevant for the 2PPE process (few femtoseconds). The total 2PPE yield enhancement and the different overall shape of the spectra have been explained by considering that the laser frequency was close to the localized surface plasmon resonance of the Cu and Ag nanoparticles. The synchronous oscillations induced by the laser in the metal electrons enhance the near-zone (NZ) field, defined as the linear superposition of the laser field and the field produced in the vicinity of the particles by the forced charge oscillations. From the present measurements it is clear that the NZ field behavior is responsible for the 2PPE enhancement and affects the 2PPE spatial and energy distribution and its dynamics. In particular, its strong spatial dependence allows indirect transitions through real intermediate states to take place in the metal clusters. Such transitions are forbidden by momentum conservation arguments and are thus experimentally much less probable on homogeneous surfaces. Further, we investigated specially tailored moon-shaped small metal nanostructures, whose NZ field was theoretically predicted, and compared the calculation with the laterally resolved 2PPE signal. We could show that the 2PPE signal gives a clear fingerprint of the theoretically predicted spatial dependence of the NZ field. This potential of our method is highly attractive in the novel field of plasmonics.

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Diese Arbeit befasst sich mit den optischen Resonanzen metallischer Nanopartikel im Abstand weniger Nanometer von einer metallischen Grenzfläche. Die elektromagnetische Wechselwirkung dieser „Kugel-vor-Fläche“ Geometrie ruft interessante optische Phänomene hervor. Sie erzeugt eine spezielle elektromagnetische Eigenmode, auch Spaltmode genannt, die im Wesentlichen auf den Nanospalt zwi-schen Kugel und Oberfläche lokalisiert ist. In der quasistatischen Näherung hängt die Resonanzposition nur vom Material, der Umgebung, dem Film-Kugel Abstand und dem Kugelradius selbst ab. Theoretische Berechnungen sagen für diese Region unter Resonanzbedingungen eine große Verstärkung des elektro-magnetischen Feldes voraus. rnUm die optischen Eigenschaften dieser Systeme zu untersuchen, wurde ein effizienter plasmonenver-mittelnder Dunkelfeldmodus für die konfokale Rastermikroskopie durch dünne Metallfilme entwickelt, der die Verstärkung durch Oberflächenplasmonen sowohl im Anregungs- als auch Emissionsprozess ausnutzt. Dadurch sind hochwertige Dunkelfeldaufnahmen durch die Metallfilme der Kugel-vor-Fläche Systeme garantiert, und die Spektroskopie einzelner Resonatoren wird erleichtert. Die optischen Untersuchungen werden durch eine Kombination von Rasterkraft- und Rasterelektronenmikroskopie vervollständigt, so dass die Form und Größe der untersuchten Resonatoren in allen drei Dimensionen bestimmt und mit den optischen Resonanzen korreliert werden können. Die Leistungsfähigkeit des neu entwickelten Modus wird für ein Referenzsystem aus Polystyrol-Kugeln auf einem Goldfilm demonstriert. Hierbei zeigen Partikel gleicher Größe auch die erwartete identische Resonanz.rnFür ein aus Gold bestehendes Kugel-vor-Fläche System, bei dem der Spalt durch eine selbstorganisierte Monolage von 2-Aminoethanthiol erzeugt wird, werden die Resonanzen von Goldpartikeln, die durch Reduktion mit Chlorgoldsäure erzeugt wurden, mit denen von idealen Goldkugeln verglichen. Diese ent-stehen aus den herkömmlichen Goldpartikeln durch zusätzliche Bestrahlung mit einem Pikosekunden Nd:Yag Laser. Bei den unbestrahlten Partikeln mit ihrer Unzahl an verschiedenen Formen zeigen nur ein Drittel der untersuchten Resonatoren ein Verhalten, das von der Theorie vorhergesagt wird, ohne das dies mit ihrer Form oder Größe korrelieren würde. Im Fall der bestrahlten Goldkugeln tritt eine spürbare Verbesserung ein, bei dem alle Resonatoren mit den theoretischen Rechnungen übereinstimmen. Eine Änderung der Oberflächenrauheit des Films zeigt hingegen keinen Einfluß auf die Resonanzen. Obwohl durch die Kombination von Goldkugeln und sehr glatten Metallfilmen eine sehr definierte Probengeometrie geschaffen wurde, sind die experimentell bestimmten Linienbreiten der Resonanzen immer noch wesentlich größer als die berechneten. Die Streuung der Daten, selbst für diese Proben, deutet auf weitere Faktoren hin, die die Spaltmoden beeinflußen, wie z.B. die genaue Form des Spalts. rnDie mit den Nanospalten verbundenen hohen Feldverstärkungen werden untersucht, indem ein mit Farbstoff beladenes Polyphenylen-Dendrimer in den Spalt eines aus Silber bestehenden Kugel-vor-Fläche Systems gebracht wird. Das Dendrimer in der Schale besteht lediglich aus Phenyl-Phenyl Bindungen und garantiert durch die damit einhergende Starrheit des Moleküls eine überragende Formstabiliät, ohne gleichzeitig optisch aktiv zu sein. Die 16 Dithiolan Endgruppen sorgen gleichzeitig für die notwendige Affinität zum Silber. Dadurch kann der im Inneren befindliche Farbstoff mit einer Präzision von wenigen Nanometern im Spalt zwischen den Metallstrukturen platziert werden. Der gewählte Perylen Farbstoff zeichnet sich wiederum durch hohe Photostabilität und Fluoreszenz-Quantenausbeute aus. Für alle untersuchten Partikel wird ein starkes Fluoreszenzsignal gefunden, das mindestens 1000-mal stärker ist, als das des mit Farbstoff überzogenen Metallfilms. Das Profil des Fluoreszenz-Anregungsspektrums variiert zwischen den Partikeln und zeigt im Vergleich zum freien Farbstoff eine zusätzliche Emission bei höheren Frequenzen, was in der Literatur als „hot luminescence“ bezeichnet wird. Bei der Untersuchung des Streuverhaltens der Resonatoren können wieder zwei unterschiedliche Arten von Resonatoren un-terschieden werden. Es gibt zunächst die Fälle, die bis auf die beschriebene Linienverbreiterung mit einer idealen Kugel-vor-Fläche Geometrie übereinstimmen und dann andere, die davon stark abweichen. Die Veränderungen der Fluoreszenz-Anregungsspektren für den gebundenen Farbstoffs weisen auf physikalische Mechanismen hin, die bei diesen kleinen Metall/Farbstoff Abständen eine Rolle spielen und die über eine einfache wellenlängenabhängige Verstärkung hinausgehen.

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We reported the first application of in situ shell-isolated nanoparticle enhanced Raman spectroscopy (SHINERS) to an interfacial redox reaction under electrochemical conditions. We construct gap-mode sandwich structures composed of a thiol-terminated HS-6V6H viologen adlayer immobilized on a single crystal Au(111)-(1x1) electrode and covered by Au(60 nm)@SlO(2) core shell nanoparticles acting as plasmonic antennas. We observed high-quality, potential-dependent Raman spectra of the three viologen species V(2+),V(+center dot) and V(0) on a well-defined Au(111) substrate surface and could map their potential-dependent evolution. Comparison with experiments on powder samples revealed an enhancement factor of the nonresonant Raman modes of similar to 3 x 10(5), and up to 9 x 10(7) for the resonance modes. The study illustrates the unique capability of SHINERS and its potential in the entire field of electrochemical surface science to explore structures and reaction pathways on well-defined substrate surfaces, such as single crystals, for molecular, (electro-)- catalytic, bioelectrochemical systems up to fundamental double layer studies at electrified solid/liquid interfaces.

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A new methodology based on combining active and passive remote sensing and simultaneous and collocated radiosounding data to study the aerosol hygroscopic growth effects on the particle optical and microphysical properties is presented. The identification of hygroscopic growth situations combines the analysis of multispectral aerosol particle backscatter coefficient and particle linear depolarization ratio with thermodynamic profiling of the atmospheric column. We analyzed the hygroscopic growth effects on aerosol properties, namely the aerosol particle backscatter coefficient and the volume concentration profiles, using data gathered at Granada EARLINET station. Two study cases, corresponding to different aerosol loads and different aerosol types, are used for illustrating the potential of this methodology. Values of the aerosol particle backscatter coefficient enhancement factors range from 2.1 ± 0.8 to 3.9 ± 1.5, in the ranges of relative humidity 60–90 and 40–83%, being similar to those previously reported in the literature. Differences in the enhancement factor are directly linked to the composition of the atmospheric aerosol. The largest value of the aerosol particle backscatter coefficient enhancement factor corresponds to the presence of sulphate and marine particles that are more affected by hygroscopic growth. On the contrary, the lowest value of the enhancement factor corresponds to an aerosol mixture containing sulphates and slight traces of mineral dust. The Hänel parameterization is applied to these case studies, obtaining results within the range of values reported in previous studies, with values of the γ exponent of 0.56 ± 0.01 (for anthropogenic particles slightly influenced by mineral dust) and 1.07 ± 0.01 (for the situation dominated by anthropogenic particles), showing the convenience of this remote sensing approach for the study of hygroscopic effects of the atmospheric aerosol under ambient unperturbed conditions. For the first time, the retrieval of the volume concentration profiles for these cases using the Lidar Radiometer Inversion Code (LIRIC) allows us to analyze the aerosol hygroscopic growth effects on aerosol volume concentration, observing a stronger increase of the fine mode volume concentration with increasing relative humidity.

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En esta tesis se recoge el trabajo experimental realizado para la caracterización de las propiedades ópticas en diodos láser construidos con estructuras basadas en pozos cuánticos (QW) y puntos cuánticos (QD). Las propiedades que se han estudiado en estos dispositivos son los espectros de ganancia, ganancia diferencial, índice diferencial y factor de ensanchamiento de línea (LEF). La comprensión de estas propiedades es de especial importancia para el diseño de nuevos diodos láser destinados a ser utilizados en aplicaciones exigentes como son las comunicaciones ópticas o aplicaciones médicas. El estudio se ha llevado a cabo en muestras de diodos láser suministrados por diferentes fabricantes: Ferdinand Braun Institut für Hóchstfrequenztechnik, Thales Research and Technology y la Universidad de Würzburg. Debido a esto las muestras de los láseres se han suministrado en diferentes configuraciones, utilizándose tanto dispositivos con cavidades de área ancha como de tipo caballete (“ridge”). En los trabajos se ha realizado el diseño y la construcción de los montajes experimentales y la implementación de los métodos analíticos necesarios para el estudio de las diferentes muestras. En los montajes experimentales se han implementado procesos para el filtrado espacial de los modos laterales de la cavidad presentes en los láseres de área ancha. Los métodos analíticos implementados se han utilizado para reducir los errores existentes en los sistemas de medida, mejorar su precisión y para separar la variación de índice en debida al calentamiento y la variación de corriente cuando los láseres operan en continua. El estudio sistemático de las propiedades de ópticas de los diodos láser basados en QW y QD ha permitido concluir que propiedades como el factor de ensanchamiento de línea no tienen por qué ser necesariamente inferiores en estos últimos, ya que dependen de las condiciones de inyección. En los láseres de QW se ha observado experimentalmente una reducción del factor de ensanchamiento de línea al alcanzarse la segunda transición, debido al aumento de la ganancia diferencial. ABSTRACT This thesis includes the experimental work for the characterization of optical properties of quantum well (QW) and quantum dot (QD) laser diodes. The properties that have been studied in these devices are the gain, differential gain, differential index and the linewith enhancement factor (LEF). The understating of these properties is of special importance for the design of new laser diodes to be used in exigent applications such as optical communications or medical applications. The study has been carried out using laser samples supplied by different manufacturers: Ferdinand Braun Institut fu¨r H¨ochstfrequenztechnik, Thales Research and Technology and the University of Wu¨rzburg. Because of this the laser samples were supplied in various configurations, using both broad area and ridge devices. In the work it has been done the design and construction of the experimental setups and implementation of analytical methods required for the study of the different devices. In the experimental set-ups it has been implemented a spatial filtering process to remove the lateral modes present in broad area lasers. The implemented analytical methods has been used to reduce the experimental errors in the measurement systems, improve the accuracy and separate the index variation caused by heating and current variation when the lasers operated on continuous wave. The systematic study of the optical properties of the QW and QD laser diodes has allowed concluding that properties such the linewith enhancement factor does not have to be necessary to be lower in the QD devices, since it is dependent on the injections conditions. In this work it has been experimentally observed a reduction of the linewith enhancement factor where the second transition has been reached mainly due to in the increased of the differential gain which is observed in this situation.

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We show that the variation in dispersion managed soliton energy that occurs as the amplifier position varies within the dispersion map, for a fixed map strength, can be interpreted using the concept of effective average dispersion. Using this concept we physically explain why the location of the amplifier can produce a greater or lesser energy enhancement factor than the lossless model. © 2001 Elsevier Science B.V. All rights reserved.

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The behavior of a semiconductor optical amplifier (SOA)-based nonlinear loop mirror with feedback has been investigated as a potential device for all-optical signal processing. In the feedback device, input signal pulses (ones) are injected into the loop, and amplified reflected pulses are fed back into the loop as switching pulses. The feedback device has two stable modes of operation - block mode, where alternating blocks of ones and zeros are observed, and spontaneous clock division mode, where halving of the input repetition rate is achieved. Improved models of the feedback device have been developed to study its performance in different operating conditions. The feedback device could be optimized to give a choice of either of the two stable modes by shifting the arrival time of the switching pulses at the SOA. Theoretically, it was found possible to operate the device at only tens of fJ switching pulse energies if the SOA is biased to produce very high gain in the presence of internal loss. The clock division regime arises from the combination of incomplete SOA gain recovery and memory of the startup sequence that is provided by the feedback. Clock division requires a sufficiently high differential phase shift per unit differential gain, which is related to the SOA linewidth enhancement factor.

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We examine the response of a pulse pumped quantum dot laser both experimentally and numerically. As the maximum of the pump pulse comes closer to the excited-state threshold, the output pulse shape becomes unstable and leads to dropouts. We conjecture that these instabilities result from an increase of the linewidth enhancement factor α as the pump parameter comes close to the excitated state threshold. In order to analyze the dynamical mechanism of the dropout, we consider two cases for which the laser exhibits either a jump to a different single mode or a jump to fast intensity oscillations. The origin of these two instabilities is clarified by a combined analytical and numerical bifurcation diagram of the steady state intensity modes.

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In the current age of fast-depleting conventional energy sources, top priority is given to exploring non-conventional energy sources, designing highly efficient energy storage systems and converting existing machines/instruments/devices into energy-efficient ones. ‘Energy efficiency’ is one of the important challenges for today’s scientific and research community, worldwide. In line with this demand, the current research was focused on developing two highly energy-efficient devices – field emitters and Li-ion batteries, using beneficial properties of carbon nanotubes (CNT). Interface-engineered, directly grown CNTs were used as cathode in field emitters, while similar structure was applied as anode in Li-ion batteries. Interface engineering was found to offer minimum resistance to electron flow and strong bonding with the substrate. Both field emitters and Li-ion battery anodes were benefitted from these advantages, demonstrating high energy efficiency. Field emitter, developed during this research, could be characterized by low turn-on field, high emission current, very high field enhancement factor and extremely good stability during long-run. Further, application of 3-dimensional design to these field emitters resulted in achieving one of the highest emission current densities reported so far. The 3-D field emitter registered 27 times increase in current density, as compared to their 2-D counterparts. These achievements were further followed by adding new functionalities, transparency and flexibility, to field emitters, keeping in view of current demand for flexible displays. A CNT-graphene hybrid structure showed appreciable emission, along with very good transparency and flexibility. Li-ion battery anodes, prepared using the interface-engineered CNTs, have offered 140% increment in capacity, as compared to conventional graphite anodes. Further, it has shown very good rate capability and an exceptional ‘zero capacity degradation’ during long cycle operation. Enhanced safety and charge transfer mechanism of this novel anode structure could be explained from structural characterization. In an attempt to progress further, CNTs were coated with ultrathin alumina by atomic layer deposition technique. These alumina-coated CNT anodes offered much higher capacity and an exceptional rate capability, with very low capacity degradation in higher current densities. These highly energy efficient CNT based anodes are expected to enhance capacities of future Li-ion batteries.

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Carbon nanotubes (CNTs) have become one of the most interesting allotropes of carbon due to their intriguing mechanical, electrical, thermal and optical properties. The synthesis and electron emission properties of CNT arrays have been investigated in this work. Vertically aligned CNTs of different densities were synthesized on copper substrate with catalyst dots patterned by nanosphere lithography. The CNTs synthesized with catalyst dots patterned by spheres of 500 nm diameter exhibited the best electron emission properties with the lowest turn-on/threshold electric fields and the highest field enhancement factor. Furthermore, CNTs were treated with NH3 plasma for various durations and the optimum enhancement was obtained for a plasma treatment of 1.0 min. CNT point emitters were also synthesized on a flat-tip or a sharp-tip to understand the effect of emitter geometry on the electron emission. The experimental results show that electron emission can be enhanced by decreasing the screening effect of the electric field by neighboring CNTs. In another part of the dissertation, vertically aligned CNTs were synthesized on stainless steel (SS) substrates with and without chemical etching or catalyst deposition. The density and length of CNTs were determined by synthesis time. For a prolonged growth time, the catalyst activity terminated and the plasma started etching CNTs destructively. CNTs with uniform diameter and length were synthesized on SS substrates subjected to chemical etching for a period of 40 minutes before the growth. The direct contact of CNTs with stainless steel allowed for the better field emission performance of CNTs synthesized on pristine SS as compared to the CNTs synthesized on Ni/Cr coated SS. Finally, fabrication of large arrays of free-standing vertically aligned CNT/SnO2 core-shell structures was explored by using a simple wet-chemical route. The structure of the SnO2 nanoparticles was studied by X-ray diffraction and electron microscopy. Transmission electron microscopy reveals that a uniform layer of SnO2 is conformally coated on every tapered CNT. The strong adhesion of CNTs with SS guaranteed the formation of the core-shell structures of CNTs with SnO2 or other metal oxides, which are expected to have applications in chemical sensors and lithium ion batteries.

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We compare the pore size distribution of a well-characterized activated carbon derived from model-dependent, adsorption integral equation (AIE) methods with those from model-independent, immersion calorimetry and isosteric heat analyses. The AIE approach applied to nitrogen gave a mean pore width of 0.57 nm; the CO2 distribution exhibited wider dispersion. Spherical model application to CO2 and diffusion limitations for nitrogen and argon were proposed as primary reasons for inconsistency. Immersion enthalpy revealed a sharp decrease in available area equivalent to a cut-off due to molecular exclusion when the accessible surface was assessed against probe kinetic diameter. Mean pore width was identified as 0.58 ± 0.02 nm, endorsing the underlying assumptions for the nitrogen-based AIE approach. A comparison of the zero-coverage isosteric heat of adsorption for various non-polar adsorptives by the porous test sample was compared with the same adsorptives in contact with a non-porous reference adsorbent, leading to an energy ratio or adsorption enhancement factor. A linear relationship between the energy ratio and probe kinetic diameter indicated a primary pore size at 0.59 nm. The advantage of this enthalpy, model-independent methods over AIE were due to no assumptions regarding probe molecular shape, and no assumptions for pore shape and/or connectivity.

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Serum-free aggregating cell cultures of fetal rat telencephalon grown in the presence of 3 ng/ml (5 X 10(-10) M) epidermal growth factor (EGF) until day 12 showed 2- to 3-fold increased activities in the two glial enzymes, glutamine synthetase (GLU-S) and 2',3'-cyclic nucleotide 3'-phosphohydrolase (CNPase). This effect was concentration-dependent, with maximal stimulation in cultures treated daily with 3 ng/ml EGF. Addition of EGF during the first 10 culture days was sufficient to produce a maximal stimulation of both GLU-S and CNPase on day 19, whereas treatments starting on day 12 were ineffective. The stimulation of GLU-S preceded that of CNPase. The EGF-induced increase in GLU-S activity was not directly dependent on the presence of insulin, triiodothyronine, or hydrocortisone in the medium, whereas insulin was required for the stimulation of CNPase. A single dose of 5 ng/ml EGF on day 2 caused a slight but significant decrease in DNA synthesis after day 6. The present results indicate that in serum-free aggregating cell cultures of fetal rat telencephalon EGF partially inhibits DNA synthesis, and stimulates an early step in glial differentiation.

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We investigated near-infrared-to-blue upconversion from thulium (Tm 3+) doped in tellurite glasses upon continuous wave excitation near 800 nm. We observed an enhancement of over two orders of magnitude of the upconverted emission at ∼480nm when neodymium (Nd 3+) ions were codoped with Tm 3+ ions. For comparison, using a Tm 3+:Nd 3+ codoped fluorozirconate glass as a reference material we observed a 40-fold enhancement of the blue emission. Analysis of the blue emission for samples with different doping levels of Nd 3+ ions showed that energy transfer between Nd 3+ and Tm 3+ is the mechanism responsible for the enhancement in upconversion. © 2002 American Institute of Physics. © 2002 American Institute of Physics.