Ultra-ductile and low friction epoxy matrix composites

We present the results of an effective reinforcement of epoxy resin matrix with fullerene carbon soot. The optimal carbon soot addition of 1 wt. % results in a toughness improvement of almost 20 times. The optimized soot-epoxy composites also show an increase in tensile elongation of more than 13 %, thus indicating a change of the failure mechanism in tension from brittle to ductile. Additionally, the coefficient of friction is reduced from its 0.91 value in plain epoxy resin to 0.15 in the optimized composite. In the optimized composite, the lateral forces during nanoscratching decrease as much as 80 % with enhancement of the elastic modulus and hardness by 43 % and 94%, respectively. The optimized epoxy resin fullerene soot composite can be a strong candidate for coating applications where toughness, low friction, ductility and light weight are important.Comment: 24 pages, 7 Figures, 1 Table in Polymer Testing (2015

Nutrición del oso negro (Ursus americanus eremicus) en las serranías del Carmen, Coahuila

RESUMEN Se determinaron los componentes de la dieta del oso negro (Ursus americanus eremicus) en las serranías Maderas del Carmen, Coahuila. También se cuantificó la disponibilidad de los alimentos y su contenido de energía metabolizable. Se calcularon las necesidades energéticas de los osos y se estimó la capacidad de carga para esta especie. Se establecieron seis patrones estacionales de la dieta y se identificaron 28 componentes alimenticios, 92% de materia vegetal y 8% de materia animal. La capacidad de carga estimada para la etapa de máximos requerimientos energéticos de los osos es de 136 ha/ oso o 0.73 osos/km2. ABSTRACT The black bear (Ursus americanus eremicus) diet composition was determined in Maderas del Carmen Coahuila. The availability of the food was determined, as well as its metabolizable energy concentration. Black bear metabolizable energy requirements and carrying capacity were estimated. Six seasonal diet patterns were established. 28 food components were identified. 92% of the diet was vegetation and 8% animal matter. The estimated carrying capacity for Sierra del Carmen, Coahuila during the maximum bear energetic requirement phase is 136 ha/bear or 0.73 bears/km2

Physical capacity in youth football players of a profesional club

Las características físicas del fútbol son muy diversas, aunque se reconocen como muy importantes la capacidad de realizar esfuerzos de alta intensidad y la de retrasar la fatiga en la mayor medida posible en esfuerzos intermitentes. Son diversos los trabajos que analizan dichas características en el fútbol profesional, aunque son menores los que analizan las categorías de formación. En el presente estudio se analiza la evolución por categorías de pruebas de salto, velocidad, agilidad y resistencia aeróbica específica, en jugadores de fútbol jóvenes de la cantera de un club profesional de la liga española. Se produjo un incremento de las marcas con la edad, aunque no se observaron diferencias significativas en grupos de edad cercanos, produciéndose una meseta en el rendimiento en la fuerza explosiva y velocidad de aceleración a partir de los 17 años y en la velocidad de desplazamiento y agilidad a los 15 añosPhysical characteristics of football are very different, but are recognized as very important the ability to perform high-intensity efforts and to delay fatigue as much as possible in intermittent efforts. There are several studies that analyze these characteristics in professional football but are less those who analyze the categories of training. In the present study analyzes the evolution of categories of jumping, speed, agility and specific endurance in young soccer players from a professional club of the Spanish league. There was an increase of the marks with age, although no significant differences in age groups encircle. Producing a plateau in performance in explosive strength and acceleration speed from 17 years and in speed and agility at age of 1

Fossil Groups Origins III. Characterization of the sample and observational properties of fossil systems

(Abridged) Fossil systems are group- or cluster-sized objects whose luminosity is dominated by a very massive central galaxy. In the current cold dark matter scenario, these objects formed hierarchically at an early epoch of the Universe and then slowly evolved until present day. That is the reason why they are called {\it fossils}. We started an extensive observational program to characterize a sample of 34 fossil group candidates spanning a broad range of physical properties. Deep $r-$band images were taken for each candidate and optical spectroscopic observations were obtained for $\sim$ 1200 galaxies. This new dataset was completed with SDSS DR7 archival data to obtain robust cluster membership and global properties of each fossil group candidate. For each system, we recomputed the magnitude gaps between the two brightest galaxies ($\Delta m_{12}$) and the first and fourth ranked galaxies ($\Delta m_{14}$) within 0.5 $R_{{\rm 200}}$. We consider fossil systems those with $\Delta m_{12} \ge 2$ mag or $\Delta m_{14} \ge 2.5$ mag within the errors. We find that 15 candidates turned out to be fossil systems. Their observational properties agree with those of non-fossil systems. Both follow the same correlations, but fossils are always extreme cases. In particular, they host the brightest central galaxies and the fraction of total galaxy light enclosed in the central galaxy is larger in fossil than in non-fossil systems. Finally, we confirm the existence of genuine fossil clusters. Combining our results with others in the literature, we favor the merging scenario in which fossil systems formed due to mergers of $L^\ast$ galaxies. The large magnitude gap is a consequence of the extreme merger ratio within fossil systems and therefore it is an evolutionary effect. Moreover, we suggest that at least one candidate in our sample could represent a transitional fossil stage.Comment: 14 pages, 11 figures, accepted for publication in A&

Trapping of three-dimensional electrons and transition to two-dimensional transport in the three-dimensional topological insulator Bi2Se3 under high pressure

[EN] This paper reports an experimental and theoretical investigation on the electronic structure of bismuth selenide (Bi2Se3) up to 9 GPa. The optical gap of Bi2Se3 increases from 0.17 eV at ambient pressure to 0.45 eV at 8 GPa. The quenching of the Burstein-Moss effect in degenerate samples and the shift of the free-carrier plasma frequency to lower energies reveal a quick decrease of the bulk three-dimensional (3D) electron concentration under pressure. On increasing pressure the behavior of Hall electron concentration and mobility depends on the sample thickness, consistently with a gradual transition from mainly 3D transport at ambient pressure to mainly two-dimensional (2D) transport at high pressure. Two-carrier transport equations confirm the trapping of high-mobility 3D electrons, an effect that can be related to a shallow-to-deep transformation of donor levels, associated with a change in the ordering of the conduction band minima. The high apparent areal density and low electron mobility of 2D electrons are not compatible with their expected properties in a Dirac cone. Measured transport parameters at high pressure are most probably affected by the presence of holes, either in an accumulation surface layer or as minority carriers in the bulk. ©2012 American Physical SocietyThis work has been done under financial support from Spanish MICINN under Grants No. MAT2008-06873-C02-02, No. MAT2007-66129, No. MAT2010-21270-C04-03/04, No. CSD2007-00045, and Prometeo No. GV2011/035. The supercomputer time has been provided by the Red Espanola de Supercomputacion (RES) and the MALTA cluster.Segura, A.; Panchal, V.; Sánchez-Royo, JF.; Marín-Borrás, V.; Muñoz-Sanjosé, V.; Rodríguez-Hernández, P.; Muñoz, A.... (2012). Trapping of three-dimensional electrons and transition to two-dimensional transport in the three-dimensional topological insulator Bi2Se3 under high pressure. Physical Review B. 85:195139-1-195139-9. https://doi.org/10.1103/PhysRevB.85.195139S195139-1195139-985Mishra, S. K., Satpathy, S., & Jepsen, O. (1997). Electronic structure and thermoelectric properties of bismuth telluride and bismuth selenide. Journal of Physics: Condensed Matter, 9(2), 461-470. doi:10.1088/0953-8984/9/2/014Hor, Y. S., Richardella, A., Roushan, P., Xia, Y., Checkelsky, J. G., Yazdani, A., … Cava, R. J. (2009). p-typeBi2Se3for topological insulator and low-temperature thermoelectric applications. Physical Review B, 79(19). doi:10.1103/physrevb.79.195208Zhang, H., Liu, C.-X., Qi, X.-L., Dai, X., Fang, Z., & Zhang, S.-C. (2009). Topological insulators in Bi2Se3, Bi2Te3 and Sb2Te3 with a single Dirac cone on the surface. Nature Physics, 5(6), 438-442. doi:10.1038/nphys1270Hasan, M. Z., & Kane, C. L. (2010). Colloquium: Topological insulators. Reviews of Modern Physics, 82(4), 3045-3067. doi:10.1103/revmodphys.82.3045Moore, J. E. (2010). The birth of topological insulators. Nature, 464(7286), 194-198. doi:10.1038/nature08916Xia, Y., Qian, D., Hsieh, D., Wray, L., Pal, A., Lin, H., … Hasan, M. Z. (2009). Observation of a large-gap topological-insulator class with a single Dirac cone on the surface. Nature Physics, 5(6), 398-402. doi:10.1038/nphys1274Chen, Y. L., Analytis, J. G., Chu, J.-H., Liu, Z. K., Mo, S.-K., Qi, X. L., … Shen, Z.-X. (2009). Experimental Realization of a Three-Dimensional Topological Insulator, Bi2Te3. Science, 325(5937), 178-181. doi:10.1126/science.1173034Hsieh, D., Xia, Y., Qian, D., Wray, L., Dil, J. H., Meier, F., … Hasan, M. Z. (2009). A tunable topological insulator in the spin helical Dirac transport regime. Nature, 460(7259), 1101-1105. doi:10.1038/nature08234Alpichshev, Z., Analytis, J. G., Chu, J.-H., Fisher, I. R., Chen, Y. L., Shen, Z. X., … Kapitulnik, A. (2010). STM Imaging of Electronic Waves on the Surface ofBi2Te3: Topologically Protected Surface States and Hexagonal Warping Effects. Physical Review Letters, 104(1). doi:10.1103/physrevlett.104.016401Roushan, P., Seo, J., Parker, C. V., Hor, Y. S., Hsieh, D., Qian, D., … Yazdani, A. (2009). Topological surface states protected from backscattering by chiral spin texture. Nature, 460(7259), 1106-1109. doi:10.1038/nature08308Butch, N. P., Kirshenbaum, K., Syers, P., Sushkov, A. B., Jenkins, G. S., Drew, H. D., & Paglione, J. (2010). Strong surface scattering in ultrahigh-mobilityBi2Se3topological insulator crystals. Physical Review B, 81(24). doi:10.1103/physrevb.81.241301Wang, Z., Lin, T., Wei, P., Liu, X., Dumas, R., Liu, K., & Shi, J. (2010). Tuning carrier type and density in Bi2Se3 by Ca-doping. Applied Physics Letters, 97(4), 042112. doi:10.1063/1.3473778Ren, Z., Taskin, A. A., Sasaki, S., Segawa, K., & Ando, Y. (2010). Large bulk resistivity and surface quantum oscillations in the topological insulatorBi2Te2Se. Physical Review B, 82(24). doi:10.1103/physrevb.82.241306Kulbachinskii, V. A., Miura, N., Nakagawa, H., Arimoto, H., Ikaida, T., Lostak, P., & Drasar, C. (1999). Conduction-band structure ofBi2−xSbxSe3mixed crystals by Shubnikov–de Haas and cyclotron resonance measurements in high magnetic fields. Physical Review B, 59(24), 15733-15739. doi:10.1103/physrevb.59.15733Analytis, J. G., McDonald, R. D., Riggs, S. C., Chu, J.-H., Boebinger, G. S., & Fisher, I. R. (2010). Two-dimensional surface state in the quantum limit of a topological insulator. Nature Physics, 6(12), 960-964. doi:10.1038/nphys1861Cho, S., Butch, N. P., Paglione, J., & Fuhrer, M. S. (2011). Insulating Behavior in Ultrathin Bismuth Selenide Field Effect Transistors. Nano Letters, 11(5), 1925-1927. doi:10.1021/nl200017fZhang, Y., He, K., Chang, C.-Z., Song, C.-L., Wang, L.-L., Chen, X., … Xue, Q.-K. (2010). Crossover of the three-dimensional topological insulator Bi2Se3 to the two-dimensional limit. Nature Physics, 6(8), 584-588. doi:10.1038/nphys1689Kong, D., Cha, J. J., Lai, K., Peng, H., Analytis, J. G., Meister, S., … Cui, Y. (2011). Rapid Surface Oxidation as a Source of Surface Degradation Factor for Bi2Se3. ACS Nano, 5(6), 4698-4703. doi:10.1021/nn200556hBenia, H. M., Lin, C., Kern, K., & Ast, C. R. (2011). Reactive Chemical Doping of theBi2Se3Topological Insulator. Physical Review Letters, 107(17). doi:10.1103/physrevlett.107.177602King, P. D. C., Hatch, R. C., Bianchi, M., Ovsyannikov, R., Lupulescu, C., Landolt, G., … Hofmann, P. (2011). Large Tunable Rashba Spin Splitting of a Two-Dimensional Electron Gas inBi2Se3. Physical Review Letters, 107(9). doi:10.1103/physrevlett.107.096802Hamlin, J. J., Jeffries, J. R., Butch, N. P., Syers, P., Zocco, D. A., Weir, S. T., … Maple, M. B. (2011). High pressure transport properties of the topological insulator Bi2Se3. Journal of Physics: Condensed Matter, 24(3), 035602. doi:10.1088/0953-8984/24/3/035602Köhler, H., & Hartmann, J. (1974). Burstein Shift of the Absorption Edge of nBi2Se3. physica status solidi (b), 63(1), 171-176. doi:10.1002/pssb.2220630116Panchal, V., Segura, A., & Pellicer-Porres, J. (2011). Low-cost set-up for Fourier-transform infrared spectroscopy in diamond anvil cell from 4000 to 400 cm−1. High Pressure Research, 31(3), 445-453. doi:10.1080/08957959.2011.594049Chervin, J. C., Canny, B., Besson, J. M., & Pruzan, P. (1995). A diamond anvil cell for IR microspectroscopy. Review of Scientific Instruments, 66(3), 2595-2598. doi:10.1063/1.1145594Piermarini, G. J., Block, S., Barnett, J. D., & Forman, R. A. (1975). Calibration of the pressure dependence of theR1ruby fluorescence line to 195 kbar. Journal of Applied Physics, 46(6), 2774-2780. doi:10.1063/1.321957Errandonea, D., Segura, A., Martínez-García, D., & Muñoz-San Jose, V. (2009). Hall-effect and resistivity measurements in CdTe and ZnTe at high pressure: Electronic structure of impurities in the zinc-blende phase and the semimetallic or metallic character of the high-pressure phases. Physical Review B, 79(12). doi:10.1103/physrevb.79.125203Errandonea, D., Martínez-García, D., Segura, A., Ruiz-Fuertes, J., Lacomba-Perales, R., Fages, V., … Mũnoz-San José, V. (2006). High-pressure electrical transport measurements on p-type GaSe and InSe. High Pressure Research, 26(4), 513-516. doi:10.1080/08957950601101787Hohenberg, P., & Kohn, W. (1964). Inhomogeneous Electron Gas. Physical Review, 136(3B), B864-B871. doi:10.1103/physrev.136.b864Kresse, G., & Hafner, J. (1993). Ab initiomolecular dynamics for liquid metals. Physical Review B, 47(1), 558-561. doi:10.1103/physrevb.47.558Kresse, G., & Hafner, J. (1994). Ab initiomolecular-dynamics simulation of the liquid-metal–amorphous-semiconductor transition in germanium. Physical Review B, 49(20), 14251-14269. doi:10.1103/physrevb.49.14251Kresse, G., & Furthmüller, J. (1996). Efficiency of ab-initio total energy calculations for metals and semiconductors using a plane-wave basis set. Computational Materials Science, 6(1), 15-50. doi:10.1016/0927-0256(96)00008-0Kresse, G., & Furthmüller, J. (1996). Efficient iterative schemes forab initiototal-energy calculations using a plane-wave basis set. Physical Review B, 54(16), 11169-11186. doi:10.1103/physrevb.54.11169Blöchl, P. E. (1994). Projector augmented-wave method. Physical Review B, 50(24), 17953-17979. doi:10.1103/physrevb.50.17953Kresse, G., & Joubert, D. (1999). From ultrasoft pseudopotentials to the projector augmented-wave method. Physical Review B, 59(3), 1758-1775. doi:10.1103/physrevb.59.1758Perdew, J. P., Ruzsinszky, A., Csonka, G. I., Vydrov, O. A., Scuseria, G. E., Constantin, L. A., … Burke, K. (2008). Restoring the Density-Gradient Expansion for Exchange in Solids and Surfaces. Physical Review Letters, 100(13). doi:10.1103/physrevlett.100.136406Mujica, A., Rubio, A., Muñoz, A., & Needs, R. J. (2003). High-pressure phases of group-IV, III–V, and II–VI compounds. Reviews of Modern Physics, 75(3), 863-912. doi:10.1103/revmodphys.75.863Köhler, H., & Becker, C. R. (1974). Optically Active Lattice Vibrations in Bi2Se3. physica status solidi (b), 61(2), 533-537. doi:10.1002/pssb.2220610218Vilaplana, R., Santamaría-Pérez, D., Gomis, O., Manjón, F. J., González, J., Segura, A., … Kucek, V. (2011). Structural and vibrational study of Bi2Se3under high pressure. Physical Review B, 84(18). doi:10.1103/physrevb.84.184110LaForge, A. D., Frenzel, A., Pursley, B. C., Lin, T., Liu, X., Shi, J., & Basov, D. N. (2010). Optical characterization ofBi2Se3in a magnetic field: Infrared evidence for magnetoelectric coupling in a topological insulator material. Physical Review B, 81(12). doi:10.1103/physrevb.81.125120Penn, D. R. (1962). Wave-Number-Dependent Dielectric Function of Semiconductors. Physical Review, 128(5), 2093-2097. doi:10.1103/physrev.128.2093PHILLIPS, J. C. (1970). Ionicity of the Chemical Bond in Crystals. Reviews of Modern Physics, 42(3), 317-356. doi:10.1103/revmodphys.42.317Van Vechten, J. A. (1969). Quantum Dielectric Theory of Electronegativity in Covalent Systems. I. Electronic Dielectric Constant. Physical Review, 182(3), 891-905. doi:10.1103/physrev.182.891Van Vechten, J. A. (1969). Quantum Dielectric Theory of Electronegativity in Covalent Systems. II. Ionization Potentials and Interband Transition Energies. Physical Review, 187(3), 1007-1020. doi:10.1103/physrev.187.1007Larson, P., Greanya, V. A., Tonjes, W. C., Liu, R., Mahanti, S. D., & Olson, C. G. (2002). Electronic structure ofBi2X3(X=S,Se,T)compounds:  Comparison of theoretical calculations with photoemission studies. Physical Review B, 65(8). doi:10.1103/physrevb.65.085108Chang, J., Jadaun, P., Register, L. F., Banerjee, S. K., & Sahu, B. (2011). Dielectric capping effects on binary and ternary topological insulator surface states. Physical Review B, 84(15). doi:10.1103/physrevb.84.155105Suski, T., Piotrzkowski, R., Wiśniewski, P., Litwin-Staszewska, E., & Dmowski, L. (1989). High pressure andDXcenters in heavily doped bulk GaAs. Physical Review B, 40(6), 4012-4021. doi:10.1103/physrevb.40.4012Errandonea, D., Segura, A., Sánchez-Royo, J. F., Mun-|Atoz, V., Grima, P., Chevy, A., & Ulrich, C. (1997). Investigation of conduction-band structure, electron-scattering mechanisms, and phase transitions in indium selenide by means of transport measurements under pressure. Physical Review B, 55(24), 16217-16225. doi:10.1103/physrevb.55.16217Analytis, J. G., Chu, J.-H., Chen, Y., Corredor, F., McDonald, R. D., Shen, Z. X., & Fisher, I. R. (2010). Bulk Fermi surface coexistence with Dirac surface state inBi2Se3: A comparison of photoemission and Shubnikov–de Haas measurements. Physical Review B, 81(20). doi:10.1103/physrevb.81.205407Köhler, H., & Fabbicius, A. (1975). Galvanomagnetic Properties of Bi2Se3with Free Carrier Densities below 5 × 1017 cm−3. physica status solidi (b), 71(2), 487-496. doi:10.1002/pssb.222071020

Effectiveness of mobile telemonitoring applications in heart failure patients: systematic review of literature and meta-analysis

Q2Q1Pacientes con Insuficiencia cardiacaClose and frequent follow-up of heart failure (HF) patients improves clinical outcomes. Mobile telemonitoring applications are advantageous alternatives due to their wide availability, portability, low cost, computing power, and interconnectivity. This study aims to evaluate the impact of telemonitoring apps on mortality, hospitalization, and quality of life (QoL) in HF patients. We conducted a registered (PROSPERO CRD42022299516) systematic review of randomized clinical trials (RCTs) evaluating mobile-based telemonitoring strategies in patients with HF, published between January 2000 and December 2021 in 4 databases (PubMed, EMBASE, BVSalud/LILACS, Cochrane Reviews). We assessed the risk of bias using the RoB2 tool. The outcome of interest was the effect on mortality, hospitalization risk, and/or QoL. We performed meta-analysis when appropriate; heterogeneity and risk of publication bias were evaluated. Otherwise, descriptive analyses are offered. We screened 900 references and 19 RCTs were included for review. The risk of bias for mortality and hospitalization was mostly low, whereas for QoL was high. We observed a reduced risk of hospitalization due to HF with the use of mobile-based telemonitoring strategies (RR 0.77 [0.67; 0.89]; I2 7%). Non-statistically significant reduction in mortality risk was observed. The impact on QoL was variable between studies, with different scores and reporting measures used, thus limiting data pooling. The use of mobile-based telemonitoring strategies in patients with HF reduces risk of hospitalization due to HF. As smartphones and wirelessly connected devices are increasingly available, further research on this topic is warranted, particularly in the foundational therapy.https://orcid.org/0000-0002-4189-4317https://orcid.org/0000-0002-8244-2958https://orcid.org/0000-0001-5401-0018https://orcid.org/0000-0003-1490-1822https://orcid.org/0000-0002-3606-2102Revista Internacional - IndexadaA1N

Rehabilitation System based on the Use of Biomechanical Analysis and Videogames through the Kinect Sensor

El presente artículo muestra la creación de un novedoso sistema para la rehabilitación física de pacientes con múltiples patologías, a través de dinámicas con videojuegos de ejercicio (exergames) y el análisis de los movimientos de los pacientes usando un software desarrollado. Este sistema está basado en el uso del sensor Kinect para ambos fines: divertir al paciente en su terapia a través de exergames y proporcionarle al especialista una herramienta para el registro y análisis de datos de captura de movimiento (MoCap) tomados a través del sensor Kinect y procesados utilizando análisis biomecánico mediante la transformación angular de Euler. Todo el sistema interactivo se encuentra instalado en un centro de rehabilitación y actualmente se realizan investigaciones con diferentes patologías (stroke, IMOC, trauma craneoencefálico, entre otros), los pacientes realizan sus sesiones con el sistema interactivo mientras el especialista registra los datos para un posterior análisis, el cual se realiza en un software creado para dicho fin. El software arroja gráficas de movimiento en los planos sagital, frontal y rotacional de 20 puntos distribuidos en el cuerpo. El sistema final es portable, no-invasivo, económico, de interacción natural con el paciente y de fácil implementación por parte del personal médico.  This paper presents development of a novel system for physical rehabilitation of patients with multiple pathologies, through dynamic with exercise videogames (exergames) and analysis of the movements of patients using developed software. This system is based on the use of the Kinect sensor for both purposes: amusing the patient in therapy through of specialist exergames and provide a tool to record and analyze MoCap data taken through the Kinect sensor and processed using biomechanical analysis through Euler angles. All interactive system is installed in a rehabilitation center and works with different pathologies (stroke, IMOC, craneoencephallic trauma, etc.), patients interact with the platform while the specialist records data for later analysis, which is performed by software designed for this purpose. The motion graphics are shown in the sagittal, frontal and rotationalplanefrom20 points distributed in the body. The final system is portable, non-invasive, inexpensive, natural interaction with the patient and easily implemented for medical purposes

Transformación vía Agrobacterium tumefaciens para inducir tolerancia a la podredumbre blanca del aguacate

Comunicación presentada en el VII World Avocado Congress, celebrado en Cairns (Australia) del 5 al 9 de septiembre de 2011.[EN] One of the most important limiting factors for avocado production in Spain is the disease caused by the fungus Rosellinia necatrix . Genetic manipulation could be useful for the introduction of fungal resistance traits into this crop. A n efficient Agrobacterium - mediated transformation protocol for avocado using AGL1 Agrobacterium strain and somatic embryos as the target material has been established by our group, although embryo conversion rate into plants needs to be improved. For that reason, we are using the strawberry, another Rosellinia necatrix ́s host, as model species to test the effect of several transgenes (two of fungal origin, chit 42 chitinase and β - 1,3 - glucanase from Trichoderma harzianum , and one of plant origin, At NPR1), on inducing tolerance to this fungus. Strawberry transformation with the β - 1,3 - glucanase gene has allowed the selection of two lines, β6 and β10, with enhanced tolerance to R. necatrix while no positive results were obtained following transformation with the chit - 42 gene. In relation to the At NPR1 gene more than 30 independent transgenic lines have been obtained whose tolerance to R. necatrix is currently under evaluation. Concerning avocado transformation, more than 10 independent transgenic lines (derive d from an embryogenic line of an immature Duke7 zygotic embryo) have been obtained with At NPR1 gene. Plants have been recovered from one line and efforts are underway to recover plants from other lines following micrografting of the transgenic sprouted sho ots onto in vitro germinated seedlings.[ES] Uno de los factores limitantes de la producción de aguacate en España es la enfermedad causada por el hongo R. necatrix. La manipulación genética podría ser de utilidad para introducir caracteres de resistencia en este cultivo. Se ha establecido un sistema eficiente de transformación en aguacate usando la cepa de Agrobacterium AGL1 y células embriogénicas como diana, sin embargo, la conversión en plantas de los embriones transgénicos necesita ser mejorada. Por esta razón, estamos utilizando la fresa, otro huésped de R. necatrix, como especie modelo para testar el efecto de varios transgenes (2 de origen fúngico, la quitinasa chit-42 y la β-1,3-glucanasa de Trichoderma harzianum, y uno derivado de plantas, AtNPR1), en la inducción de tolerancia a este patógeno tras la transformación de esta especie. La transformación de fresa con el gen de β -1,3-glucanasa ha permitido la selección de dos líneas, β6 y β10, con mayor tolerancia a R. necatrix, mientras que no se han obtenido resultados positivos con el gen chit-42. En relación con el gen AtNPR1, se han obtenido más de 30 líneas transgénicas independientes, cuya tolerancia frente a R. necatrix se está evaluando en la actualidad. En relación con la transformación de aguacate, más de 10 líneas transgénicas independientes (derivadas de una línea embriogénica obtenida a partir de un embrión zigótico inmaduro del cv. Duke 7) se han obtenido con el gen AtNPR1. Se han recuperado plantas de una línea y actualmente se está intentando recuperar plantas de otras líneas mediante microinjerto de los embriones transgénicos germinados.Este trabajo se ha realizado en el marco del proyecto AGL2008 - 05453 - C02 - 01/AGR.Peer Reviewe

Lattice dynamics of Sb2Te3 at high pressures

We report an experimental and theoretical lattice dynamics study of antimony telluride (Sb 2Te 3) up to 26 GPa together with a theoretical study of its structural stability under pressure. Raman-active modes of the low-pressure rhombohedral (R-3m) phase were observed up to 7.7 GPa. Changes of the frequencies and linewidths were observed around 3.5 GPa where an electronic topological transition was previously found. Raman-mode changes evidence phase transitions at 7.7, 14.5, and 25GPa. The frequencies and pressure coefficients of the new phases above 7.7 and 14.5 GPa agree with those calculated for the monoclinic C2/m and C2/c structures recently observed at high pressures in Bi 2Te 3 and also for the C2/m phase in the case of Bi 2Se 3 and Sb 2Te 3. Above 25 GPa no Raman-active modes are observed in Sb 2Te 3, similarly to the case of Bi 2Te 3 and Bi 2Se 3. Therefore, it is possible that the structure of Sb 2Te 3 above 25 GPa is the same disordered bcc phase already found in Bi 2Te 3 by x-ray diffraction studies. Upon pressure release, Sb 2Te 3 reverts back to the original rhombohedral phase after considerable hysteresis. Raman- and IR-mode symmetries, frequencies, and pressure coefficients in the different phases are reported and discussed. © 2011 American Physical Society.This work has been done under financial support from Spanish MICINN under Project Nos. MAT2010-21270-C04-03/04 and CSD-2007-00045 and supported by the Ministry of Education, Youth and Sports of the Czech Republic (MSM 0021627501). E. P.-G. acknowledges the financial support of the Spanish MEC under a FPI fellowship. Supercomputer time has been provided by the Red Espanola de Supercomputacion (RES) and the MALTA cluster.Gomis Hilario, O.; Vilaplana Cerda, RI.; Manjón Herrera, FJ.; Rodríguez-Hernández, P.; Pérez-González, E.; Muñoz, A.; Kucek, V.... (2011). Lattice dynamics of Sb2Te3 at high pressures. Physical Review B. 84:174305-1-174305-12. https://doi.org/10.1103/PhysRevB.84.174305S174305-1174305-1284Snyder, G. J., & Toberer, E. S. (2008). Complex thermoelectric materials. Nature Materials, 7(2), 105-114. doi:10.1038/nmat2090Venkatasubramanian, R., Siivola, E., Colpitts, T., & O’Quinn, B. (2001). Thin-film thermoelectric devices with high room-temperature figures of merit. Nature, 413(6856), 597-602. doi:10.1038/35098012Harman, T. C. (2002). Quantum Dot Superlattice Thermoelectric Materials and Devices. Science, 297(5590), 2229-2232. doi:10.1126/science.1072886Chen, J., Sun, T., Sim, D., Peng, H., Wang, H., Fan, S., … Yan, Q. (2010). Sb2Te3Nanoparticles with Enhanced Seebeck Coefficient and Low Thermal Conductivity. Chemistry of Materials, 22(10), 3086-3092. doi:10.1021/cm9038297Yin, Y., Sone, H., & Hosaka, S. (2007). Characterization of nitrogen-doped Sb2Te3 films and their application to phase-change memory. Journal of Applied Physics, 102(6), 064503. doi:10.1063/1.2778737Kim, M. S., Cho, S. H., Hong, S. K., Roh, J. S., & Choi, D. J. (2008). Crystallization characteristics of nitrogen-doped Sb2Te3 films for PRAM application. Ceramics International, 34(4), 1043-1046. doi:10.1016/j.ceramint.2007.09.078Anderson, T. L., & Krause, H. B. (1974). Refinement of the Sb2Te3 and Sb2Te2Se structures and their relationship to nonstoichiometric Sb2Te3−y Se y compounds. Acta Crystallographica Section B Structural Crystallography and Crystal Chemistry, 30(5), 1307-1310. doi:10.1107/s0567740874004729Zhang, H., Liu, C.-X., Qi, X.-L., Dai, X., Fang, Z., & Zhang, S.-C. (2009). Topological insulators in Bi2Se3, Bi2Te3 and Sb2Te3 with a single Dirac cone on the surface. Nature Physics, 5(6), 438-442. doi:10.1038/nphys1270Hasan, M. Z., & Kane, C. L. (2010). Colloquium: Topological insulators. Reviews of Modern Physics, 82(4), 3045-3067. doi:10.1103/revmodphys.82.3045Moore, J. E. (2010). The birth of topological insulators. Nature, 464(7286), 194-198. doi:10.1038/nature08916Xia, Y., Qian, D., Hsieh, D., Wray, L., Pal, A., Lin, H., … Hasan, M. Z. (2009). Observation of a large-gap topological-insulator class with a single Dirac cone on the surface. Nature Physics, 5(6), 398-402. doi:10.1038/nphys1274Wang, G., & Cagin, T. (2007). Electronic structure of the thermoelectric materialsBi2Te3andSb2Te3from first-principles calculations. Physical Review B, 76(7). doi:10.1103/physrevb.76.075201Chen, Y. L., Analytis, J. G., Chu, J.-H., Liu, Z. K., Mo, S.-K., Qi, X. L., … Shen, Z.-X. (2009). Experimental Realization of a Three-Dimensional Topological Insulator, Bi2Te3. Science, 325(5937), 178-181. doi:10.1126/science.1173034Badding, J. V., Meng, J. F., & Polvani, D. A. (1998). Pressure Tuning in the Search for New and Improved Solid State Materials. Chemistry of Materials, 10(10), 2889-2894. doi:10.1021/cm9802393Polvani, D. A., Meng, J. F., Chandra Shekar, N. V., Sharp, J., & Badding, J. V. (2001). Large Improvement in Thermoelectric Properties in Pressure-Tuned p-Type Sb1.5Bi0.5Te3. Chemistry of Materials, 13(6), 2068-2071. doi:10.1021/cm000888qChandra Shekar, N. V., Polvani, D. A., Meng, J. F., & Badding, J. V. (2005). Improved thermoelectric properties due to electronic topological transition under high pressure. Physica B: Condensed Matter, 358(1-4), 14-18. doi:10.1016/j.physb.2004.12.020Ovsyannikov, S. V., Shchennikov, V. V., Vorontsov, G. V., Manakov, A. Y., Likhacheva, A. Y., & Kulbachinskii, V. A. (2008). Giant improvement of thermoelectric power factor of Bi2Te3 under pressure. Journal of Applied Physics, 104(5), 053713. doi:10.1063/1.2973201Ovsyannikov, S. V., & Shchennikov, V. V. (2010). High-Pressure Routes in the Thermoelectricity or How One Can Improve a Performance of Thermoelectrics†. Chemistry of Materials, 22(3), 635-647. doi:10.1021/cm902000xLi, C., Ruoff, A. L., & Spencer, C. W. (1961). Effect of Pressure on the Energy Gap of Bi2Te3. Journal of Applied Physics, 32(9), 1733-1735. doi:10.1063/1.1728426Khvostantsev, L. G., Orlov, A. I., Abrikosov, N. K., & Ivanova, L. D. (1980). Thermoelectric properties and phase transition in Sb2Te3 under hydrostatic pressure up to 9 GPa. Physica Status Solidi (a), 58(1), 37-40. doi:10.1002/pssa.2210580103Sakai, N., Kajiwara, T., Takemura, K., Minomura, S., & Fujii, Y. (1981). Pressure-induced phase transition in Sb2Te3. Solid State Communications, 40(12), 1045-1047. doi:10.1016/0038-1098(81)90248-9Khvostantsev, L. G., Orlov, A. I., Abrikosov, N. K., & Ivanova, L. D. (1985). Kinetic Properties and Phase Transitions in Sb2Te3 under Hydrostatic Pressure up to 9 GPa. physica status solidi (a), 89(1), 301-309. doi:10.1002/pssa.2210890132Thonhauser, T., Scheidemantel, T. J., Sofo, J. O., Badding, J. V., & Mahan, G. D. (2003). Thermoelectric properties ofSb2Te3under pressure and uniaxial stress. Physical Review B, 68(8). doi:10.1103/physrevb.68.085201Thonhauser, T. (2004). Influence of negative pressure on thermoelectric properties of Sb2Te3. Solid State Communications, 129(4), 249-253. doi:10.1016/j.ssc.2003.10.006Einaga, M., Tanabe, Y., Nakayama, A., Ohmura, A., Ishikawa, F., & Yamada, Y. (2010). New superconducting phase of Bi2Te3under pressure above 11 GPa. Journal of Physics: Conference Series, 215, 012036. doi:10.1088/1742-6596/215/1/012036Zhang, J. L., Zhang, S. J., Weng, H. M., Zhang, W., Yang, L. X., Liu, Q. Q., … Jin, C. Q. (2010). Pressure-induced superconductivity in topological parent compound Bi2Te3. Proceedings of the National Academy of Sciences, 108(1), 24-28. doi:10.1073/pnas.1014085108Jacobsen, M. K., Kumar, R. S., Cornelius, A. L., Sinogeiken, S. V., Nico, M. F., Elert, M., … Nguyen, J. (2008). HIGH PRESSURE X-RAY DIFFRACTION STUDIES OF Bi[sub 2−x]Sb[sub x]Te[sub 3] (x = 0,1,2). doi:10.1063/1.2833001Nakayama, A., Einaga, M., Tanabe, Y., Nakano, S., Ishikawa, F., & Yamada, Y. (2009). Structural phase transition in Bi2Te3 under high pressure. High Pressure Research, 29(2), 245-249. doi:10.1080/08957950902951633Einaga, M., Ohmura, A., Nakayama, A., Ishikawa, F., Yamada, Y., & Nakano, S. (2011). Pressure-induced phase transition of Bi2Te3to a bcc structure. Physical Review B, 83(9). doi:10.1103/physrevb.83.092102Zhu, L., Wang, H., Wang, Y., Lv, J., Ma, Y., Cui, Q., … Zou, G. (2011). Substitutional Alloy of Bi and Te at High Pressure. Physical Review Letters, 106(14). doi:10.1103/physrevlett.106.145501Itskevich, E. S., Kashirskaya, L. M., & Kraidenov, V. F. (1997). Anomalies in the low-temperature thermoelectric power of p-Bi2Te3 and Te associated with topological electronic transitions under pressure. Semiconductors, 31(3), 276-278. doi:10.1134/1.1187126Polian, A., Gauthier, M., Souza, S. M., Trichês, D. M., Cardoso de Lima, J., & Grandi, T. A. (2011). Two-dimensional pressure-induced electronic topological transition in Bi2Te3. Physical Review B, 83(11). doi:10.1103/physrevb.83.113106Vilaplana, R., Santamaría-Pérez, D., Gomis, O., Manjón, F. J., González, J., Segura, A., … Kucek, V. (2011). Structural and vibrational study of Bi2Se3under high pressure. Physical Review B, 84(18). doi:10.1103/physrevb.84.184110Richter, W., & Becker, C. R. (1977). A Raman and far-infrared investigation of phonons in the rhombohedral V2–VI3 compounds Bi2Te3, Bi2Se3, Sb2Te3 and Bi2(Te1−xSex)3 (0 <x < 1), (Bi1−ySby)2Te3 (0 <y < 1). Physica Status Solidi (b), 84(2), 619-628. doi:10.1002/pssb.2220840226Sosso, G. C., Caravati, S., & Bernasconi, M. (2009). Vibrational properties of crystalline Sb2Te3from first principles. Journal of Physics: Condensed Matter, 21(9), 095410. doi:10.1088/0953-8984/21/9/095410Dagens, L. (1978). Phonon anomaly near a Fermi surface topological transition. Journal of Physics F: Metal Physics, 8(10), 2093-2113. doi:10.1088/0305-4608/8/10/010Dagens, L., & Lopez-Rios, C. (1979). Thermodynamic properties of a metal near a Fermi surface topological transition: the anomalous electron-phonon interaction contribution. Journal of Physics F: Metal Physics, 9(11), 2195-2216. doi:10.1088/0305-4608/9/11/011Goncharov, A. ., & Struzhkin, V. . (2003). Pressure dependence of the Raman spectrum, lattice parameters and superconducting critical temperature of MgB2: evidence for pressure-driven phonon-assisted electronic topological transition. Physica C: Superconductivity, 385(1-2), 117-130. doi:10.1016/s0921-4534(02)02311-0Antonangeli, D., Farber, D. L., Said, A. H., Benedetti, L. R., Aracne, C. M., Landa, A., … Klepeis, J. E. (2010). Shear softening in tantalum at megabar pressures. Physical Review B, 82(13). doi:10.1103/physrevb.82.132101Santamaría-Pérez, D., Vegas, A., Muehle, C., & Jansen, M. (2011). Structural behaviour of alkaline sulfides under compression: High-pressure experimental study on Cs2S. The Journal of Chemical Physics, 135(5), 054511. doi:10.1063/1.3617236Vilaplana, R., Gomis, O., Manjón, F. J., Segura, A., Pérez-González, E., Rodríguez-Hernández, P., … Kucek, V. (2011). High-pressure vibrational and optical study of Bi2Te3. Physical Review B, 84(10). doi:10.1103/physrevb.84.104112Larson, P. (2006). Effects of uniaxial and hydrostatic pressure on the valence band maximum inSb2Te3: An electronic structure study. Physical Review B, 74(20). doi:10.1103/physrevb.74.205113Lošťák, P., Beneš, L., Civiš, S., & Süssmann, H. (1990). Preparation and some physical properties of Bi2−xInxSe3 single crystals. Journal of Materials Science, 25(1), 277-282. doi:10.1007/bf00544220Horák, J., Quayle, P. C., Dyck, J. S., Drašar, Č., Lošt’ák, P., & Uher, C. (2008). Defect structure of Sb2−xCrxTe3 single crystals. Journal of Applied Physics, 103(1), 013516. doi:10.1063/1.2826940Piermarini, G. J., Block, S., & Barnett, J. D. (1973). Hydrostatic limits in liquids and solids to 100 kbar. Journal of Applied Physics, 44(12), 5377-5382. doi:10.1063/1.1662159Errandonea, D., Meng, Y., Somayazulu, M., & Häusermann, D. (2005). Pressure-induced transition in titanium metal: a systematic study of the effects of uniaxial stress. Physica B: Condensed Matter, 355(1-4), 116-125. doi:10.1016/j.physb.2004.10.030Syassen, K. (2008). Ruby under pressure. High Pressure Research, 28(2), 75-126. doi:10.1080/08957950802235640Hohenberg, P., & Kohn, W. (1964). Inhomogeneous Electron Gas. Physical Review, 136(3B), B864-B871. doi:10.1103/physrev.136.b864Kresse, G., & Hafner, J. (1993). Ab initiomolecular dynamics for liquid metals. Physical Review B, 47(1), 558-561. doi:10.1103/physrevb.47.558Kresse, G., & Hafner, J. (1994). Ab initiomolecular-dynamics simulation of the liquid-metal–amorphous-semiconductor transition in germanium. Physical Review B, 49(20), 14251-14269. doi:10.1103/physrevb.49.14251Kresse, G., & Furthmüller, J. (1996). Efficiency of ab-initio total energy calculations for metals and semiconductors using a plane-wave basis set. Computational Materials Science, 6(1), 15-50. doi:10.1016/0927-0256(96)00008-0Kresse, G., & Furthmüller, J. (1996). Efficient iterative schemes forab initiototal-energy calculations using a plane-wave basis set. Physical Review B, 54(16), 11169-11186. doi:10.1103/physrevb.54.11169Blöchl, P. E. (1994). Projector augmented-wave method. Physical Review B, 50(24), 17953-17979. doi:10.1103/physrevb.50.17953Kresse, G., & Joubert, D. (1999). From ultrasoft pseudopotentials to the projector augmented-wave method. Physical Review B, 59(3), 1758-1775. doi:10.1103/physrevb.59.1758Perdew, J. P., Ruzsinszky, A., Csonka, G. I., Vydrov, O. A., Scuseria, G. E., Constantin, L. A., … Burke, K. (2008). Restoring the Density-Gradient Expansion for Exchange in Solids and Surfaces. Physical Review Letters, 100(13). doi:10.1103/physrevlett.100.136406Mujica, A., Rubio, A., Muñoz, A., & Needs, R. J. (2003). High-pressure phases of group-IV, III–V, and II–VI compounds. Reviews of Modern Physics, 75(3), 863-912. doi:10.1103/revmodphys.75.863Blanco, M. A., Francisco, E., & Luaña, V. (2004). GIBBS: isothermal-isobaric thermodynamics of solids from energy curves using a quasi-harmonic Debye model. Computer Physics Communications, 158(1), 57-72. doi:10.1016/j.comphy.2003.12.001Cardona, M. (2004). Phonon widths versus pressure. High Pressure Research, 24(1), 17-23. doi:10.1080/08957950310001635819Cardona, M. (2004). Effects of pressure on the phonon–phonon and electron–phonon interactions in semiconductors. physica status solidi (b), 241(14), 3128-3137. doi:10.1002/pssb.200405202Ulrich, C., Mroginski, M. A., Goñi, A. R., Cantarero, A., Schwarz, U., Muñoz, V., & Syassen, K. (1996). Vibrational Properties of InSe under Pressure: Experiment and Theory. physica status solidi (b), 198(1), 121-127. doi:10.1002/pssb.2221980117Kulibekov, A. M., Olijnyk, H. P., Jephcoat, A. P., Salaeva, Z. Y., Onari, S., & Allakhverdiev, K. R. (2003). Raman scattering under pressure and the phase transition in ɛ-GaSe. physica status solidi (b), 235(2), 517-520. doi:10.1002/pssb.200301613Cheng, W., & Ren, S.-F. (2011). Phonons of single quintuple Bi2Te3and Bi2Se3films and bulk materials. Physical Review B, 83(9). doi:10.1103/physrevb.83.094301Buga, S. G., Serebryanaya, N. R., Dubitskiy, G. A., Semenova, E. E., Aksenenkov, V. V., & Blank, V. D. (2011). Structure and electrical properties of Sb2Te3and Bi0.4Sb1.6Te3metastable phases obtained by HPHT treatment. High Pressure Research, 31(1), 86-90. doi:10.1080/08957959.2010.52342