796 resultados para 14C measurement


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In this paper, we report the in-plane and cross-plane measurements of the thermal diffusivity of double epitaxial layers of n-type GaAs doped with various concentrations of Si and a p-type Be-doped GaAs layer grown on a GaAs substrate by the molecular beam epitaxial method, using the laser-induced nondestructive photothermal deflection technique. The thermal diffusivity value is evaluated from the slope of the graph of the phase of the photothermal deflection signal as a function of pump-probe offset. Analysis of the data shows that the cross-plane thermal diffusivity is less than that of the in-plane thermal diffusivity. It is also seen that the doping concentration has a great influence on the thermal diffusivity value. Measurement of p-type Be-doped samples shows that the nature of the dopant also influences the effective thermal diffusivity value. The results are interpreted in terms of a phonon-assisted heat transfer mechanism and the various scattering process involved in the propagation of phonons

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In this paper, we report the in-plane and cross-plane measurements of the thermal diffusivity of double epitaxial layers of n-type GaAs doped with various concentrations of Si and a p-type Be-doped GaAs layer grown on a GaAs substrate by the molecular beam epitaxial method, using the laser-induced nondestructive photothermal deflection technique. The thermal diffusivity value is evaluated from the slope of the graph of the phase of the photothermal deflection signal as a function of pump-probe offset. Analysis of the data shows that the cross-plane thermal diffusivity is less than that of the in-plane thermal diffusivity. It is also seen that the doping concentration has a great influence on the thermal diffusivity value. Measurement of p-type Be-doped samples shows that the nature of the dopant also influences the effective thermal diffusivity value. The results are interpreted in terms of a phonon-assisted heat transfer mechanism and the various scattering process involved in the propagation of phonons

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Certain organic crystals are found to possess high non- linear optical coefficients,often one to two orders of magnitude higher than those of the well known inorganic non-linear optical materials.Benzoyl glycine is one such crystal whose optical second-harmonic generation efficiency is much higher than that of potassium dihydrogen phosphate. Single crystals of benzoyl glycine are grown by solvent evaporation technique using N,N-dimethyl formamide as the solvent.All the nine second-order elastic stiffness constants of this orthorhombic crystal are determined from ultrasonic wave velocity measurements employing the pulse echo overlap technique.The anisotropy of elastic wave propagation in this crystal is demonstrated by plotting the phase velocity, slowness,Young's modulus and linear compressibility surfaces along symmetry planes.The volume compressibility, bulk modulus and relevant Poisson's ratios are also determined. Variation of the diagonal elastic stiffness constants with temperature over a limited range are measured and reported.

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The dual-beam thermal lens technique has been found to be very effective for the measurement of fluorescence quantum yields of dye solutions. The concentration-dependence of the quantum yield of rhodamine B in methanol is studied here using this technique. The observed results are in line with the conclusion that the reduction in the quantum yield in the quenching region is essentially due to the non-radiative relaxation of the absorbed energy. The thermal lens has been found to become abberated above 40 mW of pump laser power. This low value for the upper limit of pump power is due to the fact that the medium is a resonantly absorbing one.

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Laser‐induced damage and ablation thresholds of bulk superconducting samples of Bi2(SrCa)xCu3Oy(x=2, 2.2, 2.6, 2.8, 3) and Bi1.6 (Pb)xSr2Ca2Cu3 Oy (x=0, 0.1, 0.2, 0.3, 0.4) for irradiation with a 1.06 μm beam from a Nd‐YAG laser have been determined as a function of x by the pulsed photothermal deflection technique. The threshold values of power density for ablation as well as damage are found to increase with increasing values of x in both systems while in the Pb‐doped system the threshold values decrease above a specific value of x, coinciding with the point at which the Tc also begins to fall.  

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The photoacoustic technique under heat transmission configuration is used to determine the effect of doping on both the thermal and transport properties of p- and n-type GaAs epitaxial layers grown on GaAs substrate by the molecular beam epitaxial method. Analysis of the data is made on the basis of the theoretical model of Rosencwaig and Gersho. Thermal and transport properties of the epitaxial layers are found by fitting the phase of the experimentally obtained photoacoustic signal with that of the theoretical model. It is observed that both the thermal and transport properties, i.e. thermal diffusivity, diffusion coefficient, surface recombination velocity and nonradiative recombination time, depend on the type of doping in the epitaxial layer. The results clearly show that the photoacoustic technique using heat transmission configuration is an excellent tool to study the thermal and transport properties of epitaxial layers under different doping conditions.

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In this paper we show that the orthorhombic phase of FeSi2 (stable at room temperature) displays a sizable anisotropy in the infrared spectra, with minor effects in the Raman data too. This fact is not trivial at all, since the crystal structure corresponds to a moderate distortion of the fluorite symmetry. Our analysis is carried out on small single crystals grown by flux transport, through polarization-resolved far-infrared reflectivity and Raman measurements. Their interpretation has been obtained by means of the simulated spectra with tight-binding molecular dynamics.

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Measurement is the act or the result of a quantitative comparison between a given quantity and a quantity of the same kind chosen as a unit. It is generally agreed that all measurements contain errors. In a measuring system where both a measuring instrument and a human being taking the measurement using a preset process, the measurement error could be due to the instrument, the process or the human being involved. The first part of the study is devoted to understanding the human errors in measurement. For that, selected person related and selected work related factors that could affect measurement errors have been identified. Though these are well known, the exact extent of the error and the extent of effect of different factors on human errors in measurement are less reported. Characterization of human errors in measurement is done by conducting an experimental study using different subjects, where the factors were changed one at a time and the measurements made by them recorded. From the pre‐experiment survey research studies, it is observed that the respondents could not give the correct answers to questions related to the correct values [extent] of human related measurement errors. This confirmed the fears expressed regarding lack of knowledge about the extent of human related measurement errors among professionals associated with quality. But in postexperiment phase of survey study, it is observed that the answers regarding the extent of human related measurement errors has improved significantly since the answer choices were provided based on the experimental study. It is hoped that this work will help users of measurement in practice to better understand and manage the phenomena of human related errors in measurement.

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The problem of using information available from one variable X to make inferenceabout another Y is classical in many physical and social sciences. In statistics this isoften done via regression analysis where mean response is used to model the data. Onestipulates the model Y = µ(X) +ɛ. Here µ(X) is the mean response at the predictor variable value X = x, and ɛ = Y - µ(X) is the error. In classical regression analysis, both (X; Y ) are observable and one then proceeds to make inference about the mean response function µ(X). In practice there are numerous examples where X is not available, but a variable Z is observed which provides an estimate of X. As an example, consider the herbicidestudy of Rudemo, et al. [3] in which a nominal measured amount Z of herbicide was applied to a plant but the actual amount absorbed by the plant X is unobservable. As another example, from Wang [5], an epidemiologist studies the severity of a lung disease, Y , among the residents in a city in relation to the amount of certain air pollutants. The amount of the air pollutants Z can be measured at certain observation stations in the city, but the actual exposure of the residents to the pollutants, X, is unobservable and may vary randomly from the Z-values. In both cases X = Z+error: This is the so called Berkson measurement error model.In more classical measurement error model one observes an unbiased estimator W of X and stipulates the relation W = X + error: An example of this model occurs when assessing effect of nutrition X on a disease. Measuring nutrition intake precisely within 24 hours is almost impossible. There are many similar examples in agricultural or medical studies, see e.g., Carroll, Ruppert and Stefanski [1] and Fuller [2], , among others. In this talk we shall address the question of fitting a parametric model to the re-gression function µ(X) in the Berkson measurement error model: Y = µ(X) + ɛ; X = Z + η; where η and ɛ are random errors with E(ɛ) = 0, X and η are d-dimensional, and Z is the observable d-dimensional r.v.

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(1) Neuropeptid Y (NPY), einer der häufigsten peptidergen Neurotransmitter im zentralen und peripheren Nervensystem der Säuger, ist an der Steuerung zahlreicher physiologischer Prozesse beteiligt. Auch Amphibien weisen eine verstärkte NPY-Immunreaktivität im Zentralnervensystem auf. Im Hinblick auf bereits gewonnene Erkenntnisse sollte in der vorliegenden Arbeit eine Modulierbarkeit retino-tectaler Aktivität durch Neuropeptid Y an der chinesischen Rotbauchunke (Bombina orientalis) überprüft und erstmals mit Hilfe der 14[C]-2-Desoxiglukose-Methode (14C-2DG) (Sokoloff et al. 1977) quantitativ analysiert werden. Als Vergleichstier diente die Agakröte (Bufo marinus). Zur Darstellung eines möglichen Effektes auf das Tectum opticum wurde NPY lokal auf die tectale Oberfläche visuell stimulierter Rotbauchunken appliziert. Mit Hilfe der 14C-2DG-Methode und den daraus autoradiographisch ermittelten Daten konnten die zerebralen Aktivitäten visualisiert, quantitativ ausgewertet und miteinander verglichen werden. In einer weiteren Versuchsreihe wurde hinterfragt, welche inhibitorische Wirkung NPY entwickeln kann, wenn zuvor der retinale Input pharmakologisch durch systemische Gabe von Apomorphin (APO) signifikant erhöht wurde. (2) Die 14C-2DG-Methode erlaubt einen Blick in die funktionale Aktivität des Gehirns und ermöglicht es, regional ablaufende physiologische und biochemische Energiestoffwechselprozesse innerhalb des Gehirns quantitativ zu erfassen. Mit Hilfe der 14C-2DG-Methode werden die neuromodulatorischen Wirkungen von NPY kartiert und analysiert. (3) Versuchstiergruppe 1 – Bombina orientalis – unbehandelt Zur Beurteilung pharmakologischer Effekte durch NPY bzw. APO auf den Hirnmetabolismus war es zunächst erforderlich, die Gehirnaktivitäten pharmakologisch unbeeinflusster Tiere nach visueller Reizgabe zu untersuchen. Im Bereich des medialen Mesencephalon wurden die tectalen 14C-2DG-Konzentrationen über zehn Messreihen pro Einzeltier sowohl an der rechten als auch an der linken tectalen Hälfte auf Höhe des ventrolateralen Tectum opticum ermittelt. Beim rechts-links Vergleich zeigen sich gleich verteilte Strahlungsintensitäten. Basierend auf dieser Aussage konnte NPY unilateral auf die tectale Oberfläche aufgebracht und auf seine Wirkung geprüft werden. (4) Versuchstiergruppe 2 – Bombina orientalis – NPY-Applikation Der unilaterale Einsatz von NPY auf die tectale Oberfläche des Versuchstieres bewirkt, dass die unter dem Einfluss von NPY stehende tectale Hälfte, im Gegensatz zur unbehandelten tectalen Hälfte, einen deutlich niedrigeren 14C-2DG-Gebrauch aufweist. Besonders in den oberen Schichten des Tectum opticum (Layer 9) zeigt die 14C-2DG-Methode qualitativ und quantitativ auswertbare Aktivitätsminderungen an. (5) Verhalten unter NPY: Durchschnittlich nach 10 min Versuchsdauer zeigt Bombina orientalis eine deutliche Abnahme in der Beutefangaktivität, die sich gegen Ende der Versuchszeit noch weiter reduziert. (6) Versuchstiergruppe 3 – Bombina orientalis – APO-Applikation Systemisch verabreichtes APO führt bei Bombina orientalis zu einer Verstärkung des retinalen Ausganges in die retino-tectalen Projektionsfelder. Die neuronalen Aktivitäten im Tectum opticum erhöhen sich unter dem Einfluss von APO im Durchschnitt um 40% im Vergleich zu APO-unbehandelten Tieren. (7) Verhalten unter APO: Bombina orientalis zeigt nach systemischer Applikation von APO keine verstärkten stereotypen Schnappreaktionen. Die Tiere reagieren ausschließlich mit Akinese, d.h. einem Ausfall gerichteter Lokomotionen und Orientierungsbewegungen. (8) Versuchstiergruppe 4 – Bombina orientalis – APO/NPY-Applikation Die durch systemisch verabreichtes APO erhöhten retino-tectalen Aktivitäten im Tectum opticum werden unter dem unilateralen Einsatz von NPY deutlich abgeschwächt. Eindeutig niedrigere 14C-2DG-Aufnahmen sind in den oberen Schichten des Tectum opticum messbar, was die starke Wirkung von NPY quantitativ belegt. (9) Versuchstiergruppe 2 – Bufo marinus – NPY-Applikation Der unilaterale Einsatz von NPY auf die tectale Oberfläche von Bufo marinus zeigt ebenfalls, dass die unter dem Einfluss von NPY stehende tectale Hälfte, im Gegensatz zur unbehandelten tectalen Hälfte, einen deutlich niedrigeren 14C-2DG-Gebrauch aufweist. Bufo marinus zeigt aber aufgrund erweiterter Versuchsbedingungen (On-Off-Beleuchtungswechsel) anders verteilte Strahlungsintensitäten über dem Tectum-Querschnitt als Bombina orientalis. Stärkere [14C]-Akkumulationen zeigen sich in den tieferen zentralen Schichten des Tectum opticum. (10) Versuchstiergruppe 4 – Bufo marinus – APO/NPY-Applikation Auch die durch systemisch verabreichtes APO erhöhten retino-tectalen Aktivitäten im Tectum opticum von Bufo marinus werden unter dem unilateralen Einsatz von NPY deutlich abgeschwächt. (11) Die Ergebnisse der vorliegenden Arbeit leisten einen Beitrag zum Einfluss von NPY auf den retino-tectalen Informationstransfer bei Anuren im Sinne einer praetecto-tectalen inhibitorischen Modulation. Im Einklang mit früheren neuroanatomischen, immuncytochemischen und elektro-physiologischen Befunden liefern diese Ergebnisse erstmals ein biochemisches Korrelat auf der Basis des tectalen Energiestoffwechsels. (12) Es ist hervorzuheben, dass NPY-vermittelte inhibitorische Modulationen visuellen Informationstransfers in der vorliegenden Arbeit an Bombina orientalis nachgewiesen wurden, die phylogenetisch zu den ältesten Anuren (Anamnioten) gehört. Vergleichbares ist an verschiedenen Amnioten – einschließlich Primaten – beschrieben worden, was darauf hinweist, dass solche NPY-vermittelten Prozesse sich innerhalb der Tetrapoden relativ früh herausgebildet haben und in der Evolution konserviert worden sind.

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In the accounting literature, interaction or moderating effects are usually assessed by means of OLS regression and summated rating scales are constructed to reduce measurement error bias. Structural equation models and two-stage least squares regression could be used to completely eliminate this bias, but large samples are needed. Partial Least Squares are appropriate for small samples but do not correct measurement error bias. In this article, disattenuated regression is discussed as a small sample alternative and is illustrated on data of Bisbe and Otley (in press) that examine the interaction effect of innovation and style of use of budgets on performance. Sizeable differences emerge between OLS and disattenuated regression