2,844 research outputs found

    Anisotropic random resistor networks: a model for piezoresistive response of thick-film resistors

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    A number of evidences suggests that thick-film resistors are close to a metal-insulator transition and that tunneling processes between metallic grains are the main source of resistance. We consider as a minimal model for description of transport properties in thick-film resistors a percolative resistor network, with conducting elements governed by tunneling. For both oriented and randomly oriented networks, we show that the piezoresistive response to an applied strain is model dependent when the system is far away from the percolation thresold, while in the critical region it acquires universal properties. In particular close to the metal-insulator transition, the piezoresistive anisotropy show a power law behavior. Within this region, there exists a simple and universal relation between the conductance and the piezoresistive anisotropy, which could be experimentally tested by common cantilever bar measurements of thick-film resistors.Comment: 7 pages, 2 eps figure

    Nonadiabatic Superconductivity and Vertex Corrections in Uncorrelated Systems

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    We investigate the issue of the nonadiabatic superconductivity in uncorrelated systems. A local approximation is employed coherently with the weak dependence on the involved momenta. Our results show that nonadiabatic vertex corrections are never negligible, but lead to a strong suppression of TcT_c with respect to the conventional theory. This feature is understood in terms of the momentum-frequency dependence of the vertex function. In contrast to strongly correlated systems, where the small q{\bf q}-selection probes the positive part of vertex function, vertex corrections in uncorrelated systems are essentially negative resulting in an effective reduction of the superconducting pairing. Our analysis shows that vertex corrections in nonadiabatic regime can be never disregarded independently of the degree of electronic correlation in the system.Comment: 4 pages, 3 eps fig

    Influence de la déforestation sur le fonctionnement hydrologique de petits bassins versants tropicaux

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    Les rĂ©gions tropicales subissent une dĂ©forestation importante. En AmĂ©rique du Sud,la forĂȘt est gĂ©nĂ©ralement remplacĂ©e par une prairie, C'est pourquoi nous avons Ă©tudiĂ© le comportement hydrologique de 2 petits (1,5 ha) bassins versants. Un bassin (bassin B) est recouvert par une forĂȘt primaire, tandis que le second (bassin A) a Ă©tĂ© dĂ©frichĂ© et transformĂ© en prairie (Digitaria swazilandensis, programme ÉCÉREX, ORSTOM/CTFT). Ces bassins, situĂ©s en Guyane Française, sont proches (500 m), escarpĂ©s et principalement constituĂ©s par des sols Ă  drainage vertical ralenti. Le climat est de type tmpical humide avec une tempĂ©rature moyenne (26 °C) et des prĂ©cipitations moyennes annuelles (3500 Ă  3900 mm/an) Ă©levĂ©es. L'Ă©vapotranspiration rĂ©elle et potentielle de la forĂȘt primaire sont respectivement Ă©gales Ă  1470 mm/an et 1565 mm/an, En pĂ©riode d'Ă©tiage, nous avons observĂ© un Ă©coulement permanent Ă  l'exutoire du bassin A, alors que le bassin B en est dĂ©pourvu. Deux crues (24 mai 1992 et 15 mai 1993) ont Ă©tĂ© Ă©tudiĂ©es, simultanĂ©ment sur les 2 bassins. Pendant les crues, nous avons prĂ©levĂ© des Ă©chantillons d'eau des prĂ©cipitations (pluie et pluviolessivat), des ruisseaux et du sol. Sur ces sites, l'eau circulant dans les couches peu profondes du sol prĂ©sente une concentration Ă©levĂ©e en K+ et faible en Cl-. Une signature opposĂ©e caractĂ©rise l'eau des couches pmfondes du sol. L'analyse des relations existant entre les traceurs chimiques (K+, Cl-) et isotopique l80) ainsi l'Ă©tude des propriĂ©tĂ©s hydrodynamiques du sol permet de dĂ©composer qualitativement l'hydrogramme de crue en 3 rĂ©servoirs: sol superficiel (Ă©coulement hypodermique), sol intermĂ©diaire (de 0 Ă  - 0,4 m), sol profond (bassin B) ou nappe (bassin A). Une dĂ©composition quantitative a Ă©tĂ© effectuĂ©e en utilisant des traceurs chimique (Cl-) et isotopique l80). Nous avons ainsi montrĂ© que les crues sur les 2 bassins sont dominĂ©es par l'Ă©coulement issu des couches intermĂ©diaires du sol qui reprĂ©sente environ la moitiĂ© de l'Ă©coulement total de crue. Cependant,les mĂ©canismes de gĂ©nĂ©ration des crues diffĂšrent sur les 2 bassins. Sur le bassin A, les couches profondes du sol sont saturĂ©es avant la crue et participent donc Ă  la totalitĂ© de la crue. Au contraire, sur le bassin B, les couches profondes de sol atteignent la saturation peu de temps avant le pic de crue et participent donc essentiellement aux Ă©coulement pendant la dĂ©crue. Ces rĂ©sultats confirment les Ă©tudes hydrologiques rĂ©alisĂ©es prĂ©cĂ©demment (FRITSCH, 199Ù) et permettent d'identifier les mĂ©canismes de genĂšse des crues et ainsi de mettre en Ă©vidence l'effet de la dĂ©forestation.The tropical regions are subjected to fast deforestation. In South America, the tropical rain forest is being replaced by grassland. Thus, we have studied the hydrological behaviour of two small (1.5 ha) watersheds. One basin (hereafter named "B" basin) is still covered by primary forest while the second one (hereafter named "A" basin) was cleared and transformed to grassland (Digitaria swazilandensis, ÉCÉREX program, supported by ORSTOM/CTFT). These basins, located in French Guyana, are close to one another (500 m), steep, and are principally constituted of soils showing lateral drainage. The tropical humid climate is characterized by a high mean interannual temperature (26ÂĄC), which varies slightly from month to month, and by a high mean annual precipitation (3500 to 3900 mm yr-1). Precipitation mainly occurs during the main wet season from May to June and during a secondary wet season from December to January. Real evapotranspiration of the natural forest is 1470 mm yr-1 and potential evapotranspiration is 1565 mm yr-1. During the low-water level period, we have observed perennial runoff at the outlet at the "A" basin while the "B" basin is without permanent flow. We have studied two runoff events (24 May 1992 and 15 May 1993) in both basins. On 24 May 1992, the runoff event was caused by a rainfall lasting for about 10 hours. Total precipitation was 53.8 mm. The main event amounted to 32 mm. The main peak of the hydrograph corresponded to the heaviest rainfalls. On 15 May 1993, the runoff event was caused by a rain lasting for about 13 hours. Total precipitation was 64.0 mm. The main peak of the hydrograph (86.2 L s-1) corresponded again to the heaviest rainfalls. Spatial variability of the precipitation amount was high, especially for the most intense events that have the largest standard deviations. Interception by the canopy amounted to 5.3% of the rainfall in 1992 and 4.3% in 1993. High rapid runoff coefficients were observed, i.e., 0.28 for 24 May 1992 and 0.43 for 15 May 1993. No overland flow was observed in the watershed.Samples of rainwater, throughfall, stream water, and soil water were regularly collected in both watersheds during the runoff events. Temporal variations in the isotopic composition of the stream water at the outlet of the watershed paralleled variations in rainwater but with a distinct shift. The difference between the two signatures could be due to a mixture between:- Rainwater and water present in the watershed before the event and whose isotopic composition is different and variable over space. - Rainwater and water originating from various reservoirs whose contribution to the stream varies with time. The analysis of runoff events using the isotope tracer method revealed the existence in the stream of a mixture of water originating from rain and from one or several other reservoirs in the watershed. Isotope tracers alone were not sufficient to estimate the depth of the soil water contributing to the runoff event. On one hand, temporal variability in the isotopic composition of rainwater was very similar to the vertical spatial variability in the isotopic composition of soil water. On the other hand, surface evaporation in the watershed was negligible: the isotopic signature of water originating from soil during runoff events was the consequence of successive infiltrated rain events. Oxygen-18 content in rain water strongly varied with time but only slightly with space because of the small area of the watershed. Because of this temporal variability, an average isotope content of rainwater could not be used when calculating the contribution of "new water" at the outlet of the watershed.Using chemical and isotope tracers is a way to identify and quantify the contribution of the various water reservoirs to runoff. We were thus able to separate runoff hydrographs into simple components (water from superficial layer, intermediate layer and deep layer). In these watersheds, shallow water was characterized by relatively high concentration in potassium and very low concentration in chloride. An opposite signature characterized deep waterA "deep water" chemical tracer (chloride) - isotope tracer (18O) diagram shows the evidence of a hysteresis relationship:1. The decreasing limb of this relationship (rising segment of the hydrograph) is due to a decrease in heavy isotope content resulting from the decrease of oxygen-18 content in the precipitation and from the arrival of water from upper soil layers with low concentrations of chloride. 2. The increasing limb (falling segment of the hydrograph and recession) is associated with the arrival at the outlet of deep waters containing relatively high concentrations of chloride and heavy isotopes. Using chemical (Cl-) and isotope (18O) tracers, quantitative hydrograph separation was achieved with a simple 2- or 3- component conservative-mixing model. This information allowed qualitative hydrograph separation into 3 reservoirs: superficial soil layers, intermediate soil layers (0 to -0.4 m), deep soil layers ("B" watershed) or ground water ("A" watershed).Thus, the runoff event of both basins was dominated by the intermediate soil layers reservoir, which represents half of the total flow for both basins. However, the processes of runoff generation differ: in the "A" watershed, the deep soil layers were saturated before the rain: the contribution is significant throughout the runoff . In the "B" watershed, the deep soil layers become saturated a few times before the peak flow: their contribution dominates during the recession. These results confirm previous hydrological studies (Fritsch, 1990), which showed the high reactivity of the watershed, and give a better insight into the mechanisms involved.Some of these observations can also be used at a larger scale: 1. Identification of the reservoirs contributing to the runoff event by analyzing the relationships between oxygen-18 content and the flow rate, and between isotope and chemical tracers. 2. Simultaneous samplings along the stream in order to detect a possible zonation of the watershed. These samples must be taken during a runoff event as well as during a low-water level period to check whether the tracer concentrations in the continuous or discontinuous water table supplying the stream are heterogeneous. If the signature of the water table is heterogeneous or if the stream is supplied by several water tables with different chemical concentrations, the watershed must be divided into several homogeneous sub-watersheds

    Nonadiabatic Pauli susceptibility in fullerene compounds

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    Pauli paramagnetic susceptibility χ\chi is unaffected by the electron-phonon interaction in the Migdal-Eliashberg context. Fullerene compounds however do not fulfill the adiabatic assumption of Migdal's theorem and nonadiabatic effects are expected to be relevant in these materials. In this paper we investigate the Pauli spin susceptibility in nonadiabatic regime by following a conserving approach based on Ward's identity. We find that a sizable renormalization of χ\chi due to electron-phonon coupling appears when nonadiabatic effects are taken into account. The intrinsic dependence of χ\chi on the electron-phonon interaction gives rise to a finite and negative isotope effect which could be experimentally detected in fullerides. In addition, we find an enhancement of the spin susceptibility with temperature increasing, in agreement with the temperature dependence of χ\chi observed in fullerene compounds. The role of electronic correlation is also discussed.Comment: Revtex, 10 pages, 8 figures include

    Longitudinal and transversal piezoresistive response of granular metals

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    In this paper, we study the piezoresistive response and its anisotropy for a bond percolation model of granular metals. Both effective medium results and numerical Monte Carlo calculations of finite simple cubic networks show that the piezoresistive anisotropy is a strongly dependent function of bond probability p and of bond conductance distribution width \Delta g. We find that piezoresistive anisotropy is strongly suppressed as p is reduced and/or \Delta g is enhanced and that it vanishes at the percolation thresold p=p_c. We argue that a measurement of the piezoresistive anisotropy could be a sensitive tool to estimate critical metallic concentrations in real granular metals.Comment: 14 pages, 7 eps figure

    Band-filling effects on electron-phonon properties of normal and superconducting state

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    We address the effect of band filling on the effective electron mass m∗m^* and the superconducting critical temperature TcT_c in a electron-phonon system. We compare the vertex corrected theory with the non-crossing approximation of the Holstein model within a local approximation. We identify two regions of the electron density where m∗m^* and TcT_c are enhanced or decreased by the inclusion of the vertex diagrams. We show that the crossover between the enhancement at low density and the decrease towards half filling is almost independent of the microscopic electron-phonon parameters. These different behaviors are explained in terms of the net sign of the vertex diagrams which is positive at low densities and negative close to half filling. Predictions of the present theory for doped MgB2_2, which is argued to be in the low density regime, are discussed.Comment: 13 revtex pages, figures eps include

    Parallel pumping of magnetic vortex gyrations in spin-torque nano-oscillators

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    We experimentally demonstrate that large magnetic vortex oscillations can be parametrically excited in a magnetic tunnel junction by the injection of radio-frequency (rf) currents at twice the natural frequency of the gyrotropic vortex core motion. The mechanism of excitation is based on the parallel pumping of vortex motion by the rf orthoradial field generated by the injected current. Theoretical analysis shows that experimental results can be interpreted as the manifestation of parametric amplification when rf current is small, and of parametric instability when rf current is above a certain threshold. By taking into account the energy nonlinearities, we succeed to describe the amplitude saturation of vortex oscillations as well as the coexistence of stable regimes.Comment: Submitted to Phys. Rev. Let

    Phonon-induced spin relaxation of conduction electrons in aluminum

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    Spin-flip Eliashberg function αS2F\alpha_S^2F and temperature-dependent spin relaxation time T1(T)T_1(T) are calculated for aluminum using realistic pseudopotentials. The spin-flip electron-phonon coupling constant λS\lambda_S is found to be 2.5×10−52.5\times 10^{-5}. The calculations agree with experiments validating the Elliott-Yafet theory and the spin-hot-spot picture of spin relaxation for polyvalent metals.Comment: 4 pages; submitted to PR

    Penentration of dynamic localized states in DC-driven Josephson junction ladders by discrete jumps

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    We give a theoretical study of unusual resistive (dynamic) localized states in anisotropic Josephson junction ladders, driven by a DC current at one edge. These states comprise nonlinearly coupled rotating Josephson phases in adjacent cells, and with increasing current they are found to expand into neighboring cells by a sequence of sudden jumps. We argue that the jumps arise from instabilities in the ladder's superconducting part, and our analytic expressions for the peculiar voltage (rotational frequency) ratios and I-V curves are in very good agreement with direct numerical simulations.Comment: Accepted, Physical Review E. 5 pages, 5 figures. Revtex, with postscript figure
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