Event-triggered sampling using signal extrema for instantaneous amplitude and instantaneous frequency estimation

Event-triggered sampling (ETS) is a new approach towards efficient signal analysis. The goal of ETS need not be only signal reconstruction, but also direct estimation of desired information in the signal by skillful design of event. We show a promise of ETS approach towards better analysis of oscillatory non-stationary signals modeled by a time-varying sinusoid, when compared to existing uniform Nyquist-rate sampling based signal processing. We examine samples drawn using ETS, with events as zero-crossing (ZC), level-crossing (LC), and extrema, for additive in-band noise and jitter in detection instant. We find that extrema samples are robust, and also facilitate instantaneous amplitude (IA), and instantaneous frequency (IF) estimation in a time-varying sinusoid. The estimation is proposed solely using extrema samples, and a local polynomial regression based least-squares fitting approach. The proposed approach shows improvement, for noisy signals, over widely used analytic signal, energy separation, and ZC based approaches (which are based on uniform Nyquist-rate sampling based data-acquisition and processing). Further, extrema based ETS in general gives a sub-sampled representation (relative to Nyquistrate) of a time-varying sinusoid. For the same data-set size captured with extrema based ETS, and uniform sampling, the former gives much better IA and IF estimation. (C) 2015 Elsevier B.V. All rights reserved.

Electric field induced short range to long range structural ordering and its influence on the Eu+3 photoluminescence in the lead-free ferroelectric Na1/2Bi1/2TiO3

Eu+3 was incorporated into the lattice of a lead-free ferroelectric Na1/2Bi1/2TiO3 (NBT) as per the nominal formula Na0.5Bi0.5-xEuxTiO3. This system was investigated with regard to the Eu+3 photoluminescence (PL) and structural behaviour as a function of composition and electric field. Electric field was found to irreversibly change the features in the PL spectra and also in the x-ray diffraction patterns below the critical composition x = 0.025. Detailed analysis revealed that below the critical composition, electric field irreversibly suppresses the structural heterogeneity inherent of the host matrix NBT and brings about a long range ferroelectric state with rhombohedral (R3c) distortion. It is shown that the structural disorder on the nano-scale opens a new channel for radiative transition which manifests as a new emission line branching off from the main D-5(0)-> F-7(0) line along with a concomitant change in the relative intensity of the other crystal field induced Stark lines with different J values. The study suggests that Eu+3 luminescence can be used to probe the relative degree of field induced structural ordering in relaxor ferroelectrics and also in high performance piezoelectric alloys where electric field couples very strongly with the lattice and structural degrees of freedom. (C) 2015 AIP Publishing LLC.

Quark and gluon distribution functions in a viscous quark-gluon plasma medium and dilepton production via q(q)over-bar annihilation

Viscous modifications to the thermal distributions of quark-antiquarks and gluons have been studied in a quasiparticle description of the quark-gluon-plasma medium created in relativistic heavy-ion collision experiments. The model is described in terms of quasipartons that encode the hot QCD medium effects in their respective effective fugacities. Both shear and bulk viscosities have been taken in to account in the analysis, and the modifications to thermal distributions have been obtained by modifying the energy-momentum tensor in view of the nontrivial dispersion relations for the gluons and quarks. The interactions encoded in the equation of state induce significant modifications to the thermal distributions. As an implication, the dilepton production rate in the q (q) over bar annihilation process has been investigated. The equation of state is found to have a significant impact on the dilepton production rate along with the viscosities.

Quick measurement of H-1-F-19 scalar couplings from the complex NMR spectra by real-time spin edition

Most often the measurement of VHF from the conventional 1D H-1 NMR spectrum is severely hindered consequent to similar magnitudes of JHF and JHH couplings and the spectral multiplicity pattern. The present study reports a new 1D NMR technique based on real time spin edition, which removes all JHF and JHH while retaining only VHF of a chosen fluorine. The obtained spectrum is significantly simplified and permits straightforward determination of all possible VHF values of a chosen fluorine. Due to one dimensional nature, the method is much faster compared to 2D GET-SERF by 1-2 orders of magnitude. (C) 2015 Elsevier B.V. All rights reserved.

Efficient and practical synthesis of modular chiral beta-organochalcogeno amines, ArYCH2CH(R)NH2, and single crystal structures of (S) - MsOCH2CH(Bz)NH3+ center dot Cl- and (R)-MsOCH2CH(Ph)NH3+ center dot Cl-

Modular chiral I3-organochalcogeno amines, ArYCH2CH(R)NH2 (4a-4g) where R = Me, Bz, Ph; and ArY = PhS, BzSe and 4-MeOC6H4Te respectively have been synthesized and characterized. Compounds 4a-4g were synthesized (Method II) from chiral aminoalkyl 13-methanesulfonate hydrochlorides, MsOCH2CH(R)NH3+ center dot Cl- (2a-2c) through nucleophilic displacement of MsO- with organochalcogenolate (ArY-). In another attempt (Method I) chiral beta-organotelluro amines (4a-4c) were prepared by deprotection of chiral N-boc I3-organotelluro amides, 4-MeOC6H4TeCH2CH(R)NH-Boc (3a-3c), which in turn, 13,-,1 were made from chiral N-boc 13-methanesulfonate amides (la-lc) and ArTeNa. 1H, and FTIR spectra of all the compounds (3a-3c and 4a-4g) were characteristic. The composition of 3a-3c was determined by elemental analysis. The a]TD values of 3b-3c and 4a-4g were determined. The single crystal structures of (S)-2b and (R)-2c were determined by X-Ray diffraction studies. Both (S)-2b and (R)2c were crystallized in orthorhombic system and the Flack parameter x was found 0.08(12) and 0.00(2) respectively. The crystal of (S)-2b contain two asymmetric units with gauche (A) and staggered (B) conformations. There are NH Cl-, NH-O and CH-O intra and intermolecular secondary interactions in (S)-2b and (R)-2c resulting in supramolecular structures. (C) 2015 Elsevier By. All rights reserved.

Lifshitz transition and modulation of electronic and transport properties of bilayer graphene by sliding and applied normal compressive strain

Using density functional theory (DFT) we investigate the changes in electronic and transport properties of graphene bilayer caused by sliding one of the layers. Change in stacking pattern breaks the lattice symmetry, which results in Lifshitz transition together with the modulation of the electronic structure. Going from AA to AB stacking by sliding along armchair direction leads to a drastic transition in electronic structure from linear to parabolic dispersion. Our transport calculations show a significant change in the overall transmission value for large sliding distances along zigzag direction. The increase in interlayer coupling with normal compressive strain increases the overlapping of conduction and valence band, which leads to further shift in the Dirac points and an enhancement in the Lifshitz transition. The ability to tune the topology of band structure by sliding and/or applying normal compressive strain will open doors for controlled tuning of many physical phenomenon such as Landau levels and quantum Hall effect in graphene. (C) 2015 Elsevier Ltd. All rights reserved.

Thermoelectric Properties of In-Doped Cu2ZnGeSe4

Recently, much research has been focused on finding new thermoelectric materials. Cu-based quaternary chalcogenides that belong to A(2)BCD(4) (A = Cu; B = Zn, Cd; C = Sn, Ge; D = S, Se, Te) are wide band gap materials and one of the potential thermoelectric materials due to their complex crystal structures. In this study, In-doped quaternary compounds Cu2ZnGe1-xInxSe4 (x = 0, 0.025, 0.05, 0.075, 0.1) were prepared by a solid state synthesis method. Powder x-ray diffraction patterns of all the samples showed a tetragonal crystal structure (space group I-42m) of the main phase with a trace amount of impurity phases, which was further confirmed by Rietveld analysis. The elemental composition of all the samples showed a slight deviation from the nominal composition with the presence of secondary phases. All the transport properties were measured in the temperature range 373-673 K. The electrical resistivity of all the samples initially decreased up to similar to 470 K and then increased with increase in temperature upto 673 K, indicating the transition from semiconducting to metallic behavior. Positive Seebeck coefficients for all the samples revealed that holes are the majority carriers in the entire temperature range. The substitution of In3+ on Ge4+ introduces holes and results in the decrease of resistivity as well as the Seebeck coefficient, thereby leading to the optimization of the power factor. The lattice thermal conductivity of all the samples decreased with increasing temperature, indicating the presence of phonon-phonon scattering. As a result, the thermoelectric figure of merit (zT) of the doped sample showed an increase as compared to the undoped compound.

Thermoelectric properties of indium doped Cu2CdSnSe4

Recently, research in copper-based quaternary chalcogenide materials has been found to be interesting for the study of thermoelectric properties because of their low thermal conductivity due to complex crystal structures. In the present work, stoichiometric quaternary chalcogenide compounds Cu2CdSn1-xInxSe4(x = 0, 0.025, 0.05, 0.1) were prepared by solid state synthesis. The powder X-ray diffraction patterns of all the samples showed a tetragonal crystal structure with the space group I (4) over bar 2m of the main phase. In addition to this phase, a small amount of impurity phase CdSe was present in all the samples, as confirmed by Rietveld analysis. The elemental composition of all the samples characterized by an Electron Probe Micro Analyzer showed a slight deviation from the nominal composition. The transport properties were measured in the temperature range of 350 K-723 K. The positive Seebeck coefficient of all the compounds indicate that the majority carriers are holes. The Seebeck coefficient and electrical resistivity did not follow the trend in the expected manner with In doping, which could be influenced by the presence of the impurity phases. The total thermal conductivity of all the samples was dominated by the lattice thermal conductivity, while the electronic contribution was very small due to the low carrier contribution. A lattice thermal conductivity decrease with an increase of temperature indicates the dominance of phonon-phonon scattering at higher temperatures. The maximum figure of merit zT = 0.30 at 723 K was obtained for the compound Cu2CdSn0.9In0.1Se4. (C) 2016 Elsevier Ltd. All rights reserved.

Structural, Optical, and Piezoelectric Response of Lead-Free Ba0.95Mg0.05Zr0.1Ti0.9O3 Nanocrystalline Powder

Nanocrystalline powders of Ba1-xMgxZr0.1Ti0.9O3 (x = 0.025-0.1) were synthesized via citrate assisted sol-gel method. Interestingly, the one with x = 0.05 in the system Ba1-xMgxZr0.1Ti0.9O3 exhibited fairly good piezoelectric response aside from the other physical properties. The phase and structural confirmation of synthesized powder was established by X-ray powder diffraction (XRD) and Raman Spectroscopic techniques. Two distinct Raman bands i.e., 303 and 723 cm(-1) characteristic of tetragonal phase were observed. Thermogravimetric analysis (TGA) was performed to evaluate the phase decomposition of the as-synthesized Ba0.95Mg0.05Zr0.1Ti0.9O3 sample as a function of temperature. The average crystallite size associated with Ba0.95Mg0.05Zr0.1Ti0.9O3 was calculated using Scherrer formula based on the XRD data and was found to be 25 nm. However, Scanning and Transmission Electron Microscopy studies revealed the average crystallite size to be in the range of 30-40 nm, respectively. Kubelka-Munk function was employed to determine the optical band gap of these nanocrystallites. A piezoelectric response of 26 pm/V was observed for Ba0.95Mg0.05Zr0.1Ti0.9O3 nanocrystal by Piezoresponse Force Microscopy (PFM) technique. Photoluminescence (PL) study carried out on these nanocrystals exhibited a blue emission (470 nm) at room temperature.

Long-period modulated structure and electric-field-induced structural transformation in Na0.5Bi0.5TiO3-based lead-free piezoelectrics

Na0.5Bi0.5TiO3- based lead-free piezoelectrics exhibiting giant piezostrain are technologically interesting materials for actuator applications. The lack of clarity with regard to the structure of the nonpolar phase of this system has hindered the understanding of the structural mechanism associated with the giant piezostrain and other related phenomena. In this paper, we have investigated the structure and field-induced phase transformation behavior of a model system (0.94 - x) Na0.5Bi0.5TiO3-0.06BaTiO(3)-xK(0.5)Na(0.5)NbO(3) (0.0 <= x <= 0.025). A detailed structural analysis using neutron powder diffraction revealed that the nonpolar phase is neither cubic nor a mixture of rhombohedral (R3c) and tetragonal (P4bm) phases as commonly reported in literature but exhibits a long-period modulated structure, which is most probably of the type root 2 x root 2 x n with n = 16. Our results suggest that the giant piezoelectric strain is associated with a field-induced phase transformation of the long-period modulated structure to rhombohedral R3c structure above a critical field. We also demonstrate that the giant piezostrain is lost if the system retains a fraction of the field-induced R3c phase. A possible correlation among depolarization temperature, giant piezostrain, and its electrical fatigue behavior has also been indicated.

Efecto de diferentes distancias de siembra sobre la producción de biomasa del frijol terciopelo, (Stizolobium deeringianum) en el departamento de Masaya

El presente trabajo tuvo como objetivo, evaluar en términos biológicos y económicos el efecto de diferentes distancias de siembra sobre la producción de biomasa en base verde y seca del frijol terciopelo (Stizolobium deeringianum) El estudio se llevó a cabo en el Departamento de Masaya, en la finca "La Antena" ubicada al oeste de la ciudad de Masaya, para el estudio se utilizó un diseño de bloques completos al azar (BCA). Los resultados evidencian que las diferentes distancias de siembra, tuvieron efecto estadísticamente significativo sobre la producción de biomasa de frijol terciopelo en base verde y seca. Los mayores valores en cuanto a producción de biomasa corresponden a aquellos tratamientos cuya distancias entre planta son iguales a 0.25 m y 0.50 m, obteniendose 15.3 ton/ha y 12.3 ton/ha en base verde respectivamente y 2.43 ton/ha y 2.025 ton/ha en base seca respectivamente. En lo que respecta a la capacidad de rebrote se demostró que a una altura de corte inferior a 10 cm el frijol terciopelo no es eficiente, ya que en ninguno de los diferentes tratamientos una vez realizado el primer corte se encontraron plantas en estado de rebrote. De todos los tratamientos evaluados, el que resulta más económico en cuanto a costos de producción es el tratamiento cuya distancia entre planta es igual a 1.0 m, ya que en este se utiliza menos semilla en la siembra; pero aplicando el metodo de presupuestos parciales en base a la producción de biomasa obtenida y los posibles beneficios que se pueden obtener resultó que los tratamientos más rentables económicamente son aquellos en los cuales las distancias entre planta oscilan entre 0.25 m y 0.50 m. ya que con estos se obtiene un mayor beneficio económico.

Volúmenes y calidad de la cerdaza producida en porquerizas industriales y su aprovechamiento en la alimentación de bovinos

El presente estudio se realizó en cuatro granjas porcinas industriales del país con el objetivo de conocer y valorar la producción de cenlaza y su aprovechamiento en la alimentación de ganado bovino. Se realizaron encuestas estructuradas para obtener infonnaci6n necesaria sobre la cantidad y calidad de la cerdaza. El volumen total aproximado de cerdaza fresca en las granjas estudiadas es de 8.48 ton/día. De los análisis bromatológicos de la cerdaza se obtuvieron valores del 23.96% al 28.81% de MS y del 20.81% al 27.93% de PB. Del análisis sanitario se encontró la bacteria Klebsielta so. con flora normal. No se encontró ningún tipo de parásito. Se realizó una prueba de aceptabilidad de la cerdaza con diez bovinos, con peso promedio de 237.27 Kg; determinándose un periodo de aceptaci6n de 18 días, un consumo promedio de alimento de 15.10 Kg/animal/día, con diferentes niveles de inclusión de cerdaza (15, 30, 45 y 60%) en la ración y una ganancia diaria de 0.262 Kg/animal. Una vez estabilizado el consumo de cerdaza (60%) en la ración se encontró un consumo de cerdaza de 15.58 Kg/animal/día y una ganancia diaria de 0.535 Kg/animal, en un periodo de 11 días. Se determinó un costo de la cerdaza de C$ 0.025/Kg.

Evaluación de inductores florales y dosis en el cultivo de la piña (Ananas comosus (L) Merr) en la zona Ticuantepe

La floración de la piña [Ananas comosus (L) Merr.] ocurre naturalmente influenciado por factores climáticos (fotoperíodo, temperatura, radiación solar, etc.) y artificialmente mediante el uso de sustancias químicas (reguladores de crecimiento de la planta o inductores de la floración). El objetivo de este trabajo es evaluar dos inductores de floración: Carburo de Calcio (CaC2) y el Ácido 2-Cloroetilfosfónico (Ethephón), y una combinación de estos, de cada uno se compararon tres diferentes concentraciones. El experimento se realizó en noviembre del 2000, en la finca “El Piñal”, localizada en el municipio de Ticuantepe, departamento de Managua, sobre piña cv “cayena lisa’ de 10 meses de edad y en un promedio de 35-40 hojas. El diseño experimental utilizado en el estudio fue de parcela dividida, con tres repeticiones. Los tratamientos o parcelas principales fueron: Carburo de Calcio al 0.57%, 0.43% y 0.28%; Ethephón o ácido 2-cloroétil fosfórico al 0.075%, 0.050% y 0.025% y la combinación de Carburo de Calcio al 0.57% más Ethephón en tres concentraciones 0.025%, 0.020% y 0.015%. Las subparcelas fueron constituidas por cinco (5) intervalos de recuento de floración tomados como días después de la inducción (ddi), estos fueron: 40, 45, 50, 55 y 60 ddi. Se realizó la prueba de Duncan a 95% de confianza para las comparaciones de medias de los tratamientos y sus interacciones. Los tratamientos que presentaron los mejores resultados en cuanto a porcentaje de floración, fueron: los inductores de Carburo de Calcio al 0.57% y 0.43%, que completaron el 100% de plantas florecidas a 50 días después de la inducción y las combinaciones de Carburo de Calcio al 0.57% más Ethephón al 0.025% y al 0.020%. los cuales obtuvieron el 100% de plantas florecidas a los 55 días después de la inducción. Los tratamientos Ethephón al 0.075%, 0.025% y 0.050% con 71.67%, 81.67% y 93.33% respectivamente, presentaron los mas bajos porcentajes de floración a los 60 días después de la inducción. En relación a la rapidez de la aparición de la inflorescencia los mejores resultados se obtuvieron en los tratamientos Carburo de Calcio al 0.57% y al 0.43% que tan solo a 50 días después de la inducción completaron el 100% de plantas florecidas. En cuanto al análisis económico de los tratamientos en estudio, el de mejor rentabilidad resultó ser Carburo de Calcio al 0.28%, dado que es el de menor costo de aplicación, además en este tratamiento se obtuvo uno de los mayores resultados de porcentaje de floración y en menor tiempo.

Experimental Investigation On The Slip Between Oil And Water In Horizontal Pipes

This work is devoted to study of the slip phenomenon between phases in water-oil two-phase flow in horizontal pipes. The emphasis is placed on the effects of input fluids flow rates, pipe diameter and viscosities of oil phase on the slip. Experiments were conducted to measure the holdup in two horizontal pipes with 0.05 m diameter and 0.025 m diameter, respectively, using two different viscosities of white oil and tap water as liquid phases. Results showed that the ratios of in situ oil to water velocity at the pipe of small diameter are higher than those at the pipe of big diameter when having same input flow rates. At low input water flow rate, there is a large deviation on the holdup between two flow systems with different oil viscosities and the deviation becomes gradually smaller with further increased input water flow rate. (C) 2008 Elsevier Inc. All rights reserved.

Estudio de la factibilidad de aplicación, a escala planta piloto, del catalizador Cr2O3 soportado en alúmina en la reducción de emisión de SO2 a la atmósfera, proveniente de fuentes fijas : avances 2012

Resumen: Se realizaron las experiencias planificadas con el objeto de analizar el comportamiento del catalizador en la columna metálica, para simular condiciones de planta piloto. Se modificaron las masas de catalizador y se realizaron ciclos de adsorción, desorción y readsorción sucesivos sobre una misma muestra, con lo que se determinaron variaciones en la eficiencia del mismo. En otra fase se desarrolló el estudio teórico de la adsorción de O2 y CO2 sobre el mismo sustrato, y el estudio de la cinética de la reacción entre CH4, SO2 y el O2 por medio del programa VASP (Vienna Ab-initio Simulation Package). Se verificó, a través de los datos experimentales y teóricos y en colaboración con el Dr. V. A. Ranea y el Prof. E. E. Mola (INIFTA, UNLP), la presencia de especies sulfito y sulfato sobre la superficie del soporte. Experimentalmente, se observa que la eficiencia de adsorción del catalizador respecto al SO2 es cercana al 100%. Se observa un pico de termodesorción a 1120 K. Luego, se estudió la oxidación de CH4 con SO2. Se observa que hay producción de CO2 desde temperatura inicial, seguida de un aumento en la formación de CO2 hasta 330-340 K. Luego, la producción de CO2 se mantiene aproximadamente constante. Mediante el empleo de la ecuación de Arrhenius y resultados experimentales, se obtuvo la energía de activación de la reacción global, de 7 Kcal/mol. También se observó que el incremento del flujo de SO2 a valores superiores a 200 ml/min no incrementa la cantidad de SO2 retenida en el rango de 923-1023K. Para un incremento de masa de sustrato catalítico de 0,025 a 0,050 g, la masa retenida de SO2 se incrementa un 70,61%. Mediante estudios teóricos, se determinó que la energía de quimisorción del SO2 sobre el Cr2O3 es de -3.09 eV para la configuración más estable.