990 resultados para 7140-106


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Nanocomposite thin film transistors (TFTs) based on nonpercolating networks of single-walled carbon nanotubes (CNTs) and polythiophene semiconductor [poly [5, 5′ -bis(3-dodecyl-2-thienyl)- 2, 2′ -bithiophene] (PQT-12)] thin film hosts are demonstrated by ink-jet printing. A systematic study on the effect of CNT loading on the transistor performance and channel morphology is conducted. With an appropriate loading of CNTs into the active channel, ink-jet printed composite transistors show an effective hole mobility of 0.23 cm 2 V-1 s-1, which is an enhancement of more than a factor of 7 over ink-jet printed pristine PQT-12 TFTs. In addition, these devices display reasonable on/off current ratio of 105-10 6, low off currents of the order of 10 pA, and a sharp subthreshold slope (<0.8 V dec-1). The work presented here furthers our understanding of the interaction between polythiophene polymers and nonpercolating CNTs, where the CNT density in the bilayer structure substantially influences the morphology and transistor performance of polythiophene. Therefore, optimized loading of ink-jet printed CNTs is crucial to achieve device performance enhancement. High performance ink-jet printed nanocomposite TFTs can present a promising alternative to organic TFTs in printed electronic applications, including displays, sensors, radio-frequency identification (RFID) tags, and disposable electronics. © 2009 American Institute of Physics.

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This paper reports on the synthesis of zinc oxide (ZnO) nanostructures and examines the performance of nanocomposite thin-film transistors (TFTs) fabricated using ZnO dispersed in both n- and p-type polymer host matrices. The ZnO nanostructures considered here comprise nanowires and tetrapods and were synthesized using vapor phase deposition techniques involving the carbothermal reduction of solid-phase zinc-containing compounds. Measurement results of nanocomposite TFTs based on dispersion of ZnO nanorods in an n-type organic semiconductor ([6, 6]-phenyl-C61-butyric acid methyl ester) show electron field-effect mobilities in the range 0.3-0.6 cm2V-1 s-1. representing an approximate enhancement by as much as a factor of 40 from the pristine state. The on/off current ratio of the nanocomposite TFTs approach 106 at saturation with off-currents on the order of 10 pA. The results presented here, although preliminary, show a highly promising enhancement for realization of high-performance solution-processable n-type organic TFTs. © 2008 IEEE.

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Physical forces generated by cells drive morphologic changes during development and can feedback to regulate cellular phenotypes. Because these phenomena typically occur within a 3-dimensional (3D) matrix in vivo, we used microelectromechanical systems (MEMS) technology to generate arrays of microtissues consisting of cells encapsulated within 3D micropatterned matrices. Microcantilevers were used to simultaneously constrain the remodeling of a collagen gel and to report forces generated during this process. By concurrently measuring forces and observing matrix remodeling at cellular length scales, we report an initial correlation and later decoupling between cellular contractile forces and changes in tissue morphology. Independently varying the mechanical stiffness of the cantilevers and collagen matrix revealed that cellular forces increased with boundary or matrix rigidity whereas levels of cytoskeletal and extracellular matrix (ECM) proteins correlated with levels of mechanical stress. By mapping these relationships between cellular and matrix mechanics, cellular forces, and protein expression onto a bio-chemo-mechanical model of microtissue contractility, we demonstrate how intratissue gradients of mechanical stress can emerge from collective cellular contractility and finally, how such gradients can be used to engineer protein composition and organization within a 3D tissue. Together, these findings highlight a complex and dynamic relationship between cellular forces, ECM remodeling, and cellular phenotype and describe a system to study and apply this relationship within engineered 3D microtissues.

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To study electron affinity kinetics, a shock tube method was applied, in which the test gas was ionized by a reflected shock wave and subsequently quenched by a strong rarefaction wave. As the quenching speed of 106 K/s was reached, a nonequilibrium ionization-recombination process occurred, which was dominated by ion recombination with electrons. A Langmuir electrostatic probe was used to monitor variation in the ion number density at the reflection shock region. The working state of the probe was analyzed...

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The high-field properties of polycrystalline superconducting TlBaCaCuO films fabricated by the incorporation of thallium vapour into air-atomised BaCaCuO precursors are described. Thick films with Tc values in the range 106-111 K have been prepared on polycrystalline yttria-stabilised zirconia substrates. The surface morphology, crystal structure and composition of the films are related to their high-field transport and magnetisation properties. Typical 10 mm × 9 mm films show Jc values > 1×104 A/cm2 at 77 K (0 T). The best film has a Jc=1.3×104 A/cm2 (Ic=3.6 A) at 77 K (0 T). Films prepared on 26 mm×9 mm substrates show typical large-area Jc values > 0.5×104 A/cm2 (77 K, 0 T). A square planar specimen of dimensions 4.3 mm ×4.3 mm exhibited magnetisation Jc values=1.2×105 A/cm2 at 4.2 K (0.1 T), 9.3×104 A/cm2 at 10 K (0.1 T), 3.3×104 A/ cm2 at 4 K (8 T), and 1.6×104 A/cm2 at 10 K (8 T). © 1994.

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El término “funciones ejecutivas” comienza a ser utilizado por Lezak en los 80’. No se trata de un concepto unitario, incluyendo varias funciones cognitivas y autodirigidas que contribuyen a la autorregulación del individuo. Existen varias controversias acerca del constructo “funciones ejecutivas”, entre ellas: la unidad vs diversidad de los procesos cognitivos que implican las funciones ejecutivas, y la naturaleza del control ejecutivo; el presente artículo se focaliza sobre esta última cuestión. Se presentarán dos aproximaciones de acuerdo a distintos modos de explicación de la memoria de trabajo y del control ejecutivo. Finalmente, se propone enfocar el estudio de las funciones ejecutivas desde una visión integrada de la mente, para su mejor comprensión.

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Resumen: La Antigone de Sófocles y el Corpus Hippocraticum delinean ya los rasgos propios del derecho natural. La ética de Aristóteles, luego, ofrece una primera noción explícita del derecho natural, que San Alberto Magno comenta en Super ethica. Sin embargo, en De inventione de Cicerón el teólogo alemán encuentra su definición de derecho natural: “lo que cierta fuerza innata introdujo”. En De bono V q. 1 San Alberto determina los alcances de esta definición y completa una presentación acabada de la noción de derecho natural. También advierte San Alberto que el hombre, con respecto a la ciencia del intelecto práctico, se encuentra doblemente en potencia. Primero, está en potencia de conocer los principios primeros de esta ciencia y, segundo, una vez conocidos éstos, se encuentra en potencia de inferir a partir de ellos las conclusiones de la ciencia práctica. Poseídas estas conclusiones, finalmente, el hombre está en potencia de aplicarlas en la acción práctica. Intrigado por el modo en que los primeros principios son conocidos, San Alberto advierte que el conocimiento de las nociones correspondientes a estos principios sólo accidentalmente debe ser atribuido al descubrimiento o determinación de los nombres con los que llamamos a estos principios. En verdad, es necesaria la intervención de la luz del intelecto agente para llevar al acto el conocimiento de los principios. En este punto el discurso de San Alberto retorna a la definición ciceroniana: aquella fuerza innata que introduce el derecho natural no es otra que la luz del intelecto agente.

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A single-crystal silicon resonant bulk acoustic mass sensor with a measured resolution of 125 pg cm2 is presented. The mass sensor comprises a micromachined silicon plate that is excited in the square-extensional bulk acoustic resonant mode at a frequency of 2.182 MHz, with a quality factor exceeding 106. The mass sensor has a measured mass to frequency shift sensitivity of 132 Hz cm2 μg. The resonator element is embedded in a feedback loop of an electronic amplifier to implement an oscillator with a short term frequency stability of better than 7 ppb at an operating pressure of 3.8 mTorr. © 2007 American Institute of Physics.

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En el mes de Enero del 2003, se estableció el experimento en la finca del Campus agropecuario de la UNAN-León, localizada a 1 km de la carretera de circunvalación by pass departamento de León, con el objetivo de: evaluar la incidencia y comportamiento de la Sigatoka negra (Mycosphaerella fijiensis m.) en el período de verano e invierno en el cultivo del plátano variedad cuerno gigante (AAB). El área donde se estableció el estudio fue de 1.42 hectárea, la parcela útil tenia 2500 metros cuadrados en la que se tomaron planta a evaluar, las variables en estudio fueron; período de incubación en la que se estudiaron 120 plantas, intensidad de la infección con 120 plantas estudiadas, período de latencia, Estado de evolución con 130 plantas muestreadas, severidad de la enfermedad en la que se evaluaron 240 plantas. Para el análisis de la información con la evaluación del período de incubación, intensidad de la infección, período de latencia, estado de evolución de la enfermedad, severidad, se construyeron curvas de progreso de la enfermedad en el tiempo en relación con los factores climáticos. En el análisis estadístico de la información se aplico correlación y regresión lineal simple y métodos gráficos, utilizando un criterio de decisión de significancia de P= 0.05 para establecer el peso de cada factor climático en el desarrollo de la enfermedad y su importancia relativa en el modelo de preaviso biológico de la misma. Los resultados obtenidos indican que los factores que permitieron un mayor desarrollo de la Sigatoka negra fueron las altas precipitaciones, las horas de humedad relativa mayor al 90% y las temperaturas bajas menores de los 25ºc. En los meses de verano (enero– abril) con humedad relativa de 40% a 70% la severidad de la enfermedad fue relativamente baja, en relación con la severidad y comportamiento que esta presentó en el invierno. El período de incubación fue de 99 días, con síntomas en estado de pizca, y para llegar al estado de mancha en el período de latencia duró 106, para un período total del ciclo del patógeno de 205 días. De mayo a octubre, época de invierno, con precipitaciones de 429 mm a 636mm, humedad relativa en el ambiente de 95% a 100% la severidad de la Sigatoka negra fue mayor, en donde los síntomas en estado de estrías para el período de incubación llego a durar de 23 a 25 días y los síntomas en estado de mancha en la variable período de latencia llegó a durar como mínimo 8 días y como máximo 94 días. A lo largo del año el mes que menos severa fue la enfermedad fue febrero, y más severa se presento en agosto. El estado de evolución de la enfermedad fue de 585 estría en el período de verano, de enero a abril, y de 800 estría en el período de invierno de mayo a octubre, lo que indica que el estado de evolución del patógeno es relativamente bajo en período seco, debido a que no se le presentaron las condiciones optimas necesarias de humedad relativa alta, precipitaciones y temperatura baja, las que juegan un papel importante en la reproducción y liberación del inoculo del patógeno. En junio que se establecen las precipitacion es el estado de evolución asciende a 890 estrías, para un 20% de daño en toda la plantación, siendo este relativamente bajo en comparación con el estado de evolución que se presento en el mes de octubre el cual fue de 2,402 estrías. Es muy importante mencionar que los síntomas de la enfermedad en las variables de intensidad de la infección, severidad de la enfermedad y el estado de evolución, no se presentaron en el mismo momento que se le presentan las condiciones favorable al patógeno, estas se vienen manifestando después de 15 días, lo que consideramos normal dentro del ciclo reproductivo del hongo.

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This paper reports the design and electrical characterization of a micromechanical disk resonator fabricated in single crystal silicon using a foundry SOI micromachining process. The microresonator has been selectively excited in the radial extensional and the wine glass modes by reversing the polarity of the DC bias voltage applied on selected drive electrodes around the resonant structure. The quality factor of the resonator vibrating in the radial contour mode was 8000 at a resonant frequency of 6.34 MHz at pressure below 10 mTorr vacuum. The highest measured quality factor of the resonator in the wine glass resonant mode was 1.9 × 106 using a DC bias voltage of 20 V at about the same pressure in vacuum; the resonant frequency was 5.43 MHz and the lowest motional resistance measured was approximately 17 kΩ using a DC bias voltage of 60 V applied across 2.7 μm actuation gaps. This corresponds to a resonant frequency-quality factor (f-Q) product of 1.02 × 1013, among the highest reported for single crystal silicon microresonators, and on par with the best quartz crystal resonators. The quality factor for the wine glass mode in air was approximately 10,000. © 2009 Elsevier B.V. All rights reserved.

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We present a technique for independently exciting two resonant modes of vibration in a single-crystal silicon bulk mode microresonator using the same electrode configuration through control of the polarity of the DC actuation voltage. Applications of this technique may include built-in temperature compensation by the simultaneous selective excitation of two closely spaced modes that may have different temperature coefficients of resonant frequency. The technique is simple and requires minimum circuit overhead for implementation. The technique is implemented on square plate resonators with quality factors as high as 3.06 × 106. Copyright © 2008 by ASME.

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This paper reports on the design and electrical characterization of a single crystal silicon micromechanical square-plate resonator. The microresonator has been excited in the anti-symmetrical wine glass mode at a resonant frequency of 5.166 MHz and exhibits an impressive quality factor (Q) of 3.7 × 106 at a pressure of 33 mtorr. The device has been fabricated in a commercial foundry process. An associated motional resistance of approximately 50 kΩ using a dc bias voltage of 60 V is measured for a transduction gap of 2 νm due to the ultra-high Q of the resonator. This result corresponds to a frequency-Q product of 1.9 × 1013, the highest reported for a fundamental mode single-crystal silicon resonator and on par with some of the best quartz crystal resonators. The results are indicative of the superior performance of silicon as a mechanical material, and show that the wine glass resonant mode is beneficial for achieving high quality factors allowed by the material limit. © 2009 IOP Publishing Ltd.

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We report on the experimental characterization of a single crystal silicon square-plate microresonator. The resonator is excited in the square wine glass (SWG) mode at a mechanical resonance frequency of 2.065 MHz. The resonator displays quality factor of 9660 in air and an ultra-high quality factor of Q = 4.05 × 106 in 12 mtorr vacuum. The SWG mode may be described as a square plate that contracts along one axis in the fabrication plane, while simultaneously extending along an orthogonal axis in the same plane. The resonant structure is addressed in a 2-terminal configuration by utilizing equal and opposite drive polarities on surrounding capacitor electrodes, thereby decreasing the motional resistance of the resonator. The resonant micromechanical device has been fabricated in a commercial silicon-on-insulator process through the MEMSCAP foundry utilising a minimum electrostatic gap of 2 μm. © 2008 IEEE.

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We report on the fabrication and field emission of carbon nanotube lateral field emitters. Due to its high aspect ratio and mechanical strength, we use vertically aligned multi-wall carbon nanotubes prepared by plasma-enhanced chemical vapour deposition as cathodes, which makes the fabrication of cantilever type lateral field emitters possible. The emission characteristics show that the field emission initiates at 11-17 V. The device has high geometrical enhancement factors (9.3 × 106 cm-1) compared to standard Spindt tips, which may be due to increased field concentration at the nanotube tip and the close proximity of the anode (<1 μm). The relative ease of fabrication compared to vertical field emitters and enhanced field emission characteristics observed makes the carbon nanotube lateral field emitter a good candidate for future integrated nano-electronic devices.

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We report weaknesses in two algebraic constructions of low-density parity-check codes based on expander graphs. The Margulis construction gives a code with near-codewords, which cause problems for the sum-product decoder; The Ramanujan-Margulis construction gives a code with low-weight codewords, which produce an error-floor. © 2004 Elsevier B.V.