978 resultados para BE-8
Resumo:
Angular distributions for the (9)Be((8)Li, (9)Be) (8)Li elastic-transfer reaction have been measured with a 27-MeV (8)Li radioactive nuclear beam. Spectroscopic factors for the <(9)Be vertical bar(8)Li + p > bound system were obtained from the comparison between the experimental differential cross sections and finite-range distorted-wave Born approximation calculations made with the code FRESCO. The spectroscopic factors so obtained are compared with shell-model calculations and other experimental values. Using the present value for the spectroscopic factors, cross sections and reaction rates for the (8)Li(p,gamma) (9)Be direct proton-capture reaction of astrophysical interest were calculated in the framework of the potential model.
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A new measurement of the B-11(p,alpha(0))Be-8 has been performed applying the Trojan horse method (THM) to the H-2(B-11,alpha Be-8(0))n quasi-free reaction induced at a laboratory energy of 27 MeV. The astrophysical S(E) factor has been extracted from similar to 600 keV down to zero energy by means of an improved data analysis technique and it has been compared with direct data available in the literature. The range investigated here overlaps with the energy region of the light element LiBeB stellar burning and with that of future aneutronic fusion power plants using the B-11+p fuel cycle. The new investigation described here confirms the preliminary results obtained in the recent TH works. The origin of the discrepancy between the direct estimate of the B-11(p,alpha(0))Be-8 S(E)-factor at zero energy and that from a previous THM investigation is quantitatively corroborated. The results obtained here support, within the experimental uncertainties, the low-energy S(E)-factor extrapolation and the value of the electron screening potential deduced from direct measurements.
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The elastic-scattering angular distribution for (8)Li on (12)C has been measured at E(LAB) = 23.9 MeV with (8)Li radioactive nuclear beam produced by the Radioactive Ion Beams in Brazil facility. This angular distribution was analyzed in terms of optical-model with Woods-Saxon and double-folding Sao Paulo potential. The roles of the breakup and inelastic channels were also investigated with cluster folding and deformed potentials, respectively, through coupled-channels calculations. The angular distribution for the proton-transfer (12)C((8)Li, (9)Be)(11)B reaction was also measured at the same energy. The spectroscopic factor for the <(9)Be|(8)Li + p > bound system was obtained and compared with shell-model calculations and with other experimental values. Total reaction cross sections for the present system were also extracted from the elastic-scattering analysis. A systematic of the reduced reaction cross sections obtained from the present and published data on (6,7,8)Li isotopes on (12)C was performed as a function of energy.
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We have analyzed a large set of alpha + alpha elastic scattering data for bombarding energies ranging from 0.6 to 29.5 MeV. Because of the complete lack of open reaction channels, the optical interaction at these energies must have a vanishing imaginary part. Thus, this system is particularly important because the corresponding elastic scattering cross sections are very sensitive to the real part of the interaction. The data were analyzed in the context of the velocity-dependent Sao Paulo potential, which is a successful theoretical model for the description of heavy-ion reactions from sub-barrier to intermediate energies. We have verified that, even in this low-energy region, the velocity dependence of the model is quite important for describing the data of the alpha + alpha system.
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Layer-by-layer (LBL) assembly was used to combine crystalline rod-like nanoparticles obtained from a vegetable source, cellulose nanowhiskers (CNWs), with collagen, the main component of skin and connective tissue found exclusively in animals. The film growth of the multilayered collagen/CNW was monitored by UV-Vis spectroscopy and ellipsometry measurements, whereas the film morphology and surface roughness were characterized by SEM and AFM. UV-Vis spectra showed the deposition of the same amount of collagen, 5 mg m(-2), in each dipping cycle. Ellipsometry data showed an increment in thickness with the number of layers, and the average thickness of each bilayer was found to be 8.6 nm. The multilayered bio-based nanocomposites were formed by single layers of densely packed CNWs adsorbed on top of each thin collagen layer where the hydrogen bonding between collagen amide groups and OH groups of the CNWs plays a mandatory role in the build-up of the thin films. The approach used in this work represents a potential strategy to mimic the characteristics of natural extracellular matrix (ECM) which can be used for applications in the biomedical field.
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CoB, CO(2)B, CoSi, Co(2)Si and CO(5)Si(2)B phases can be formed during heat-treatment of amorphous co-Si-B soft magnetic materials. Thus, it is important to determine their magnetic behavior as a function of applied field and temperature. In this study, polycrystalline single-phase samples of the above phases were produced via arc melting and heat-treatment under argon. The single-phase nature of the samples was confirmed via X-ray diffraction experiments. AC and DC magnetization measurements showed that Co(2)Si and CO(5)Si(2)B phases are paramagnetic. Minor amounts of either Co(2)Si or CoSi(2) in the CoSi-phase sample suggested a paramagnetic behavior of the CoSi-phase, however, it should be diamagnetic as shown in the literature. The diamagnetic behavior of the CoB phase was also confirmed. The paramagnetic behavior of CO(5)Si(2)B is for the first time reported. The magnetization results of the phase CO(2)B have a ferromagnetic signature already verified on previous NMR studies. A detailed set of magnetization measurements of this phase showed a change of the easy magnetization axis starting at 70K, with a temperature interval of about 13K at a very small field of 1 mT. As the strength of the field is increased the temperature interval is enlarged. The strength of field at which the magnetization saturates increases almost linearly as the temperature is increased above 70K. The room temperature total magnetostriction of the CO(2)B phase was determined to be 8 ppm at a field of 1T. (C) 2010 Elsevier B.V. All rights reserved.
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Objectives: (1) To establish test performance measures for Transient Evoked Otoacoustic Emission testing of 6-year-old children in a school setting; (2) To investigate whether Transient Evoked Otoacoustic Emission testing provides a more accurate and effective alternative to a pure tone screening plus tympanometry protocol. Methods: Pure tone screening, tympanometry and transient evoked otoacoustic emission data were collected from 940 subjects (1880 ears), with a mean age of 6.2 years. Subjects were tested in non-sound-treated rooms within 22 schools. Receiver operating characteristics curves along with specificity, sensitivity, accuracy and efficiency values were determined for a variety of transient evoked otoacoustic emission/pure tone screening/tympanometry comparisons. Results: The Transient Evoked Otoacoustic Emission failure rate for the group was 20.3%. The failure rate for pure tone screening was found to be 8.9%, whilst 18.6% of subjects failed a protocol consisting of combined pure tone screening and tympanometry results. In essence, findings from the comparison of overall Transient Evoked Otoacoustic Emission pass/fail with overall pure tone screening pass/fail suggested that use of a modified Rhode Island Hearing Assessment Project criterion would result in a very high probability that a child with a pass result has normal hearing (true negative). However, the hit rate was only moderate. Selection of a signal-to-noise ratio (SNR) criterion set at greater than or equal to 1 dB appeared to provide the best test performance measures for the range of SNR values investigated. Test performance measures generally declined when tympanometry results were included, with the exception of lower false alarm rates and higher positive predictive values. The exclusion of low frequency data from the Transient Evoked Otoacoustic Emission SNR versus pure tone screening analysis resulted in improved performance measures. Conclusions: The present study poses several implications for the clinical implementation of Transient Evoked Otoacoustic Emission screening for entry level school children. Transient Evoked Otoacoustic Emission pass/fail criteria will require revision. The findings of the current investigation offer support to the possible replacement of pure tone screening with Transient Evoked Otoacoustic Emission testing for 6-year-old children. However, they do not suggest the replacement of the pure tone screening plus tympanometry battery. (C) 2001 Elsevier Science Ireland Ltd. All rights reserved.
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The crustal and lithospheric mantle structure at the south segment of the west Iberian margin was investigated along a 370 km long seismic transect. The transect goes from unthinned continental crust onshore to oceanic crust, crossing the ocean-continent transition (OCT) zone. The wide-angle data set includes recordings from 6 OBSs and 2 inland seismic stations. Kinematic and dynamic modeling provided a 2D velocity model that proved to be consistent with the modeled free-air anomaly data. The interpretation of coincident multi-channel near-vertical and wide-angle reflection data sets allowed the identification of four main crustal domains: (i) continental (east of 9.4 degrees W); (ii) continental thinning (9.4 degrees W-9.7 degrees W): (iii) transitional (9.7 degrees W-similar to 10.5 degrees W); and (iv) oceanic (west of similar to 10.5 degrees W). In the continental domain the complete crustal section of slightly thinned continental crust is present. The upper (UCC, 5.1-6.0 km/s) and the lower continental crust (LCC, 6.9-7.2 km/s) are seismically reflective and have intermediate to low P-wave velocity gradients. The middle continental crust (MCC, 6.35-6.45 km/s) is generally unreflective with low velocity gradient. The main thinning of the continental crust occurs in the thinning domain by attenuation of the UCC and the LCC. Major thinning of the MCC starts to the west of the LCC pinchout point, where it rests directly upon the mantle. In the thinning domain the Moho slope is at least 13 degrees and the continental crust thickness decreases seaward from 22 to 11 km over a similar to 35 km distance, stretched by a factor of 1.5 to 3. In the oceanic domain a two-layer high-gradient igneous crust (5.3-6.0 km/s; 6.5-7.4 km/s) was modeled. The intra-crustal interface correlates with prominent mid-basement, 10-15 km long reflections in the multi-channel seismic profile. Strong secondary reflected PmP phases require a first order discontinuity at the Moho. The sedimentary cover can be as thick as 5 km and the igneous crustal thickness varies from 4 to 11 km in the west, where the profile reaches the Madeira-Tore Rise. In the transitional domain the crust has a complex structure that varies both horizontally and vertically. Beneath the continental slope it includes exhumed continental crust (6.15-6.45 km/s). Strong diffractions were modeled to originate at the lower interface of this layer. The western segment of this transitional domain is highly reflective at all levels, probably due to dykes and sills, according to the high apparent susceptibility and density modeled at this location. Sub-Moho mantle velocity is found to be 8.0 km/s, but velocities smaller than 8.0 km/s confined to short segments are not excluded by the data. Strong P-wave wide-angle reflections are modeled to originate at depth of 20 km within the lithospheric mantle, under the eastern segment of the oceanic domain, or even deeper at the transitional domain, suggesting a layered structure for the lithospheric mantle. Both interface depths and velocities of the continental section are in good agreement to the conjugate Newfoundland margin. A similar to 40 km wide OCT having a geophysical signature distinct from the OCT to the north favors a two pulse continental breakup.
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The exponential coefficient in the first-passage-time problem for a bistable potential with highly colored noise is predicted to be (8/27 by all existing theories. On the other hand, we show herein that all existing numerical evidence seems to indicate that the coefficient is actually larger by about (4/3, i.e., that the numerical factor in the exponent is approximately (32/81. Existing data cover values of ¿V0/D up to ~20, where V0 is the barrier height, ¿ the correlation time of the noise, and D the noise intensity. We provide an explanation for the modified coefficinet, the explanation also being based on existing numerical simulations. Whether the value (8/27 predicted by all large-¿ theories is achieved for even larger values of ¿V0/D is unknown but appears questionable (except perhaps for enormously large, experimentally inaccessible values of this factor) in view of currently available results.
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Este trabalho teve como objetivo avaliar e selecionar híbridos de cacaueiro, quanto a rendimento e qualidade de sementes, nas condições ecológicas do Município de Ouro Preto do Oeste, Rondônia. A seleção foi feita comparando-se, pelo teste de Duncan, as médias das medidas dos componentes de rendimento avaliados em um ensaio conduzido entre 1986 e 1991. O delineamento experimental usado foi o de blocos completos casualizados. Os melhores desempenhos, quanto aos caracteres avaliados, foram obtidos em cruzamentos que incluíram os clones POUND 7 e BE 10 (número total de frutos coletados), SCA 6 e PA 150 (número total de frutos sadios), PA 150 (peso total de sementes úmidas), IMC 67 e POUND 7 (peso médio de sementes úmidas por fruto). Na análise simultânea dos caracteres, os híbridos SCA 6 x ICS 1, PA 150 x SIC 328 e IMC 67 x BE 8 sobressaíram-se, em relação aos demais.
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Les lesions per cremades comporten conseqüències a nivell físic, psicològic i social. Les intervencions psicosocials per aquests pacients estan valorades de forma positiva però manquen estudis fets a l’Estat Espanyol. Les intervencions de pacient expert estan donant resultats positius en moltes patologies cròniques però no n’existeix cap per aquest tipus de lesions cròniques. L’objectiu d’aquest estudi és comprendre la utilitat d’una intervenció de pacient expert a pacients d’entre 18 i 30 anys que han patit lesions per cremades recentment. Es realitzaran 9 sessions de pacient expert des de la perspectiva bio-psicosocial. El grup focal serà un grup de 8-10 pacients de 18 a 30 anys amb un mínim del 15% de superfície corporal cremada de grau 2n profund o 3r, residents a Barcelona o rodalies. Les dades s’analitzaran per mètode mixt amb enfocament dominant qualitatiu. La recollida de dades s’obtindrà d’entrevistes, testos i anotacions realitzades prèvia a la primera sessió, al finalitzar les 9 sessions i als 6 mesos de la última sessió. Les limitacions de l’estudi són: el risc de pèrdua dels membres del grup focal a causa del retorn a la vida laboral i l’heterogeneïtat del grup en la fase d’acceptació, principis i valors personals que podrien desviar els resultats.
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Components of daily energy expenditure were measured serially by whole-body calorimetry in Gambian women before pregnancy and at 6, 12, 18, 24, 30, and 36 wk gestation. Weight gain was (mean +/- SD) 6.8 +/- 2.8 kg, fat deposition was 2.0 +/- 2.5 kg and lean tissue deposition was 5.0 +/- 2.5 kg. Basal metabolic rate (BMR) was depressed during the first 18 wk of gestation, causing total cumulative maintenance costs by week 36 to be 8.4 MJ. Individual responses to pregnancy correlated with changes in body mass (36 wk: delta BMR vs delta weight; r = 0.60, P < 0.01 delta BMR vs delta LBM; r = 0.62, P < 0.01). There was no significant increase in the cost of treadmill exercise (0% slope: F = 0.71, P = 0.64; 5% slope: F = 1.97, P = 0.10), 24-h energy expenditure (F = 0.72, P = 0.64), activity or diet-induced thermogenesis (F = 1.02, P = 0.43), during pregnancy in spite of body weight gain. Total metabolic costs over 36 wk were 144 MJ (fetus 43 MJ, fat deposition 92 MJ, cumulative maintenance costs 8.4 MJ). These were far lower than reported for well-nourished Western populations.
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La scoliose idiopathique de l’adolescence (SIA) est une déformation tridimensionnelle complexe du rachis affectant majoritairement les filles. L’atteinte progressive est surtout esthétique avec, notamment, une déformation de la cage thoracique résultante. L’asymétrie mammaire est une préoccupation fréquente chez ces jeunes filles. Se définissant comme une différence de forme, de position ou de volume des seins ou des complexes aréolo-mamelonnaires, l’asymétrie mammaire est courante chez les femmes, mais habituellement mineure et non visible. Il demeure incertain dans la littérature si l’asymétrie mammaire est plus fréquente chez les scoliotiques. De plus, très peu d’études ont évalué la relation entre la scoliose et l’asymétrie mammaire. De façon instinctive, on serait porté à croire que ce ne sont pas les seins qui sont asymétriques, mais plutôt la déformation du thorax en rotation qui donne cette impression. Les seins représentent un des organes les plus difficiles à mesurer étant donné leur grande variabilité. Plusieurs méthodes de mesure ont été décrites. L’imagerie par résonance magnétique (IRM) est considérée l’outil le plus précis pour définir la glande mammaire et plus particulièrement, sa délimitation sur la cage thoracique. Ce projet consiste à quantifier l’asymétrie mammaire, représentée par une différence de volume entre les deux seins, chez une cohorte de jeunes filles présentant une SIA significative, en utilisant l’IRM comme outil de mesure. Ensuite, une méthode de mesure automatisée, à partir de la topographie surfacique 3D, est proposée. Les résultats obtenus avec cette méthode sont confrontés à ceux de l’IRM. L’influence de la posture sur le volume mammaire est également étudiée à partir de ces deux modalités différentes. Pour réaliser ces objectifs, une cohorte de 30 patientes scoliotiques a été recrutée sur la base de leur courbure thoracique et de leur maturité osseuse et mammaire. Deux imageries de tronc ont été effectuées : la topographie surfacique 3D et la résonance magnétique. Dans un premier temps, la sommation des images segmentées acquises par IRM nous a permis de mesurer de façon très précise le volume mammaire. Notre cohorte présente une asymétrie mammaire moyenne statistiquement significative de 8.32%. 66.6% des patientes présentent une asymétrie ≥ 5%. Par ailleurs, le sein gauche est plus volumineux chez 65.5% des patientes. Une faible corrélation non-significative existe entre les volumes mammaires et l’angle de Cobb ainsi que la gibbosité thoracique. Par la suite, une méthode de mesure automatisée, développée à partir de l’environnement mathématique Matlab, est appliquée directement sur les reconstructions 3D. En bref, elle consiste à identifier les contours des seins pour les exciser afin d’exposer la cage thoracique puis, à soustraire le thorax complet du thorax sans seins pour déterminer les volumes mammaires. Les volumes mammaires acquis par la méthode automatisée sont, de manière attendue, de plus petites tailles que ceux obtenus à l’IRM. Une forte corrélation est établie entre les volumes mammaires obtenus par les deux différentes techniques de mesure. Bien que statistiquement significatives, les asymétries mammaires (r= 0.614, p< .001) ne sont pas aussi fortement corrélées entre elles que les volumes. Le sein droit (r=0.805) présente une corrélation plus élevée que le sein gauche (r=0.747). Finalement, l’influence de la posture est étudiée à partir des maillages 3D de l’IRM (décubitus ventral) et de la topographie surfacique 3D (position debout). D’excellentes corrélations sont confirmées entre les volumes mammaires ; r= 0.896 et r= 0.939, respectivement pour les volumes mammaires gauches et droits. Ce projet a permis de démontrer, pour la première fois, qu’il est possible de calculer le volume mammaire de façon objective et précise avec l’IRM, chez une cohorte scoliotique. Grâce à la précision des repères anatomiques, l’IRM nous a permis de revisiter une croyance populaire dans la communauté de la scoliose. Celle soutenant que l’asymétrie mammaire ressentie par les patientes n’est qu’une perception. Ces nouvelles données nous permettrons de conseiller les jeunes filles avec la SIA, concernant leurs préoccupations sur l’asymétrie de leurs seins. Nous avons confirmé que la méthode de mesure automatisée est réalisable cliniquement et pourrait être utilisée pour prédire les volumes obtenus à l’IRM. Par ailleurs, c’est le premier outil de mesure de volumétrie mammaire complètement automatisé à notre connaissance. Les volumes mammaires obtenus debout et en décubitus ventral sont comparables.
Resumo:
Study Design Cross-sectional descriptive study. Objectives To characterize breast asymmetry (BA), as defined by breast volume difference, in girls with significant adolescent idiopathic scoliosis (AIS), using magnetic resonance imaging (MRI). Summary and Background BA is a frequent concern among girls with AIS. It is commonly believed that this results from chest wall deformity. Although many women exhibit physiological BA, the prevalence is not known in adolescents and it remains unclear if it is more frequent in AIS. Breasts vary in shape and size and many ways of measuring them have been explored. MRI shows the highest precision at defining breast tissue. Methods Thirty patients were enrolled on the basis of their thoracic curvature, skeletal and breast maturity, without regard to their perception on their BA. MRI acquisitions were performed in prone with a 1.5-Tesla system using a 16-channel breast coil. Segmentation was achieved using the ITK-SNAP 2.4.0 software and subsequently manually refined. Results The mean left breast volume (528.32 ± 205.96 cc) was greater compared with the mean right breast volume (495.18 ± 170.16 cc) with a significant difference between them. The mean BA was found to be 8.32% ± 6.43% (p < .0001). A weak positive correlation was observed between BA and thoracic Cobb angle (0.177, p = .349) as well as thoracic gibbosity angle (0.289, p = .122). The left breast was consistently larger in 65.5% of the patients. Twenty patients (66.7%) displayed BA ≥5%. Conclusions We have described BA in patients with significant AIS using MRI. This method is feasible, objective, and very precise. The majority of patients had a larger left breast, which could compound the apparent BA secondary to trunk rotation. In many cases, BA is present independently of thoracic deformity. This knowledge will assist in counseling AIS patients in regards to their concerns with BA.
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Este trabajo se centra en el análisis de las actividades desarrolladas en torno a los servicios de procesos de impresión que ofrece la organización DATAPOINT de Colombia SAS para identificar los puntos críticos en la gestión de los residuos de impresión y las decisiones tomadas por parte de los involucrados durante todo el proceso (proveedores, clientes y la empresa), con el fin de revisar medidas y estrategias que permitan fortalecer la gestión integral de residuos de impresión a partir de una revisión y comparación de las mejores prácticas planteadas por los actores del sector. También se efectuaron recomendaciones con acciones de mejora que se podrían desarrollar con el fin de mitigar el impacto ambiental generado por estos residuos. Con la finalidad de cumplir con lo planteado se realizó inicialmente un estudio sobre la organización, sus clientes y proveedores para entender de manera integral la cadena de valor en torno a los tóner y su gestión inversa, (explicar) al igual que el entorno normativo tanto de manera nacional como internacional. Posteriormente, se identificaron los puntos de mejora comparando lo planteado por el proveedor versus lo ejecutado por los involucrados en el proceso, labor se realizó en campo con los clientes para entender la situación actual, sus necesidades y en que basan la toma de decisiones relacionada con el manejo de los residuos de impresión. Finalmente se listaran una serie de acciones de mejora y recomendaciones las cuales pueden ser incorporadas a los procesos críticos de DATAPOINT.