7,141 research outputs found

    Lower Eocene sedimentary succession and microfossil biostratigraphy in the central northern Caucasus basin

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    The lower Eocene sediments from the classical Paleogene section exposed along the Kheu River, northern Caucasus, southern Russia are here studied. This ca. 50m thick succession is lithologically contrasting: the lower and upper parts are composed by soft marls separated by a thick Radiolaria-rich unit of non-calcareous and low-calcareous mudstones with intercalations of compact cherty layers. According to nannofossil and dinocyst biostratigraphy, the unique intercalation of Total Organic Carbon (TOC)-rich sediment (sapropelitic bed) in the lower part of the lower Eocene correspond to the Paleocene-Eocene Thermal Maximum (PETM) and a series of sapropelitic interlayers in the upper marly part of the lower Eocene succession correlates with the Early Eocene Climatic Optimum (EECO). The study of nannofossil and dinocyst assemblages enabled detailed zonal subdivision and first-order calibration of nannofossil and dinocyst bio-events during this time-span. The studied interval of the section embraces the complete succession of nannofossil zones NP9-NP13 of Martini, 1971, CP8-CP11 of Okada and Bukry, 1980 and CNP11-CNE5 of Agnini et al., 2014. By means of dinocyst stratigraphy, the succession of Apectodinium hyperacanthum, Axiodinium augustum, Deflandrea oebisfeldensis, Dracodinium astra, Stenodinium meckelfeldense, Dracodinium varielongitudum, Ochetodinium romanum/Samlandia chlamydophora and Areosphaeridium diktyoplokum zones are identified in the Ypresian part of the Kheu section

    On the multiplicity of the hyperelliptic integrals

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    Let I(t)=δ(t)ωI(t)= \oint_{\delta(t)} \omega be an Abelian integral, where H=y2xn+1+P(x)H=y^2-x^{n+1}+P(x) is a hyperelliptic polynomial of Morse type, δ(t)\delta(t) a horizontal family of cycles in the curves {H=t}\{H=t\}, and ω\omega a polynomial 1-form in the variables xx and yy. We provide an upper bound on the multiplicity of I(t)I(t), away from the critical values of HH. Namely: $ord\ I(t) \leq n-1+\frac{n(n-1)}{2}if if \deg \omega <\deg H=n+1.Thereasoninggoesasfollows:weconsidertheanalyticcurveparameterizedbytheintegralsalong. The reasoning goes as follows: we consider the analytic curve parameterized by the integrals along \delta(t)ofthe of the nPetrovformsof ``Petrov'' forms of H(polynomial1formsthatfreelygeneratethemoduleofrelativecohomologyof (polynomial 1-forms that freely generate the module of relative cohomology of H),andinterpretthemultiplicityof), and interpret the multiplicity of I(t)astheorderofcontactof as the order of contact of \gamma(t)andalinearhyperplaneof and a linear hyperplane of \textbf C^ n.UsingthePicardFuchssystemsatisfiedby. Using the Picard-Fuchs system satisfied by \gamma(t),weestablishanalgebraicidentityinvolvingthewronskiandeterminantoftheintegralsoftheoriginalform, we establish an algebraic identity involving the wronskian determinant of the integrals of the original form \omegaalongabasisofthehomologyofthegenericfiberof along a basis of the homology of the generic fiber of H.Thelatterwronskianisanalyzedthroughthisidentity,whichyieldstheestimateonthemultiplicityof. The latter wronskian is analyzed through this identity, which yields the estimate on the multiplicity of I(t).Still,insomecases,relatedtothegeometryatinfinityofthecurves. Still, in some cases, related to the geometry at infinity of the curves \{H=t\} \subseteq \textbf C^2,thewronskianoccurstobezeroidentically.Inthisalternativeweshowhowtoadapttheargumenttoasystemofsmallerrank,andgetanontrivialwronskian.Foraform, the wronskian occurs to be zero identically. In this alternative we show how to adapt the argument to a system of smaller rank, and get a nontrivial wronskian. For a form \omegaofarbitrarydegree,weareledtoestimatingtheorderofcontactbetween of arbitrary degree, we are led to estimating the order of contact between \gamma(t)andasuitablealgebraichypersurfacein and a suitable algebraic hypersurface in \textbf C^{n+1}.Weobservethat. We observe that ord I(t)growslikeanaffinefunctionwithrespectto grows like an affine function with respect to \deg \omega$.Comment: 18 page

    Development and adjustment of a solar concentrator equipped with a system of orientation to the Sun

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    Solar energy is, according to many forecasts, one of the most promising branches of renewable energy. Throughout the world, research is under way and devices are being designed to convert and accumulate solar energy. In this article, work has been done on the manufacture of a solar concentrator, the software part of which is implemented using the SolarOrientation package, the results of the implemented system efficiency.Солнечная энергетика по многим прогнозам является одной из самых перспективных отраслей возобновляемой энергетики. Во всём мире проводятся исследования и проектируются устройства, с помощью которых удаётся преобразовывать и накапливать солнечную энергию. В настоящей статье проведены работы по изготовлению солнечного концентратора, программная часть которого реализована с помощью пакета SolarOrientation, получены результаты эффективности реализованной системы

    Dynamical symmetry restoration for a higher-derivative four-fermion model in an external electromagnetic field

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    A four-fermion model with additional higher-derivative terms is investigated in an external electromagnetic field. The effective potential in the leading order of large-N expansion is calculated in external constant magnetic and electric fields. It is shown that, in contrast to the former results concerning the universal character of "magnetic catalysis" in dynamical symmetry breaking, in the present higher-derivative model the magnetic field restores chiral symmetry broken initially on the tree level. Numerical results describing a second-order phase transition that accompanies the symmetry restoration at the quantum level are presented.Comment: LaTeX, 14 pages, 4 ps-figure

    Quantum Phase Transition in Pr2CuO4 to Collinear Spin State in Inclined Magnetic Field: A Neutron Diffraction Observation

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    In the external field slightly inclined to the xx- or y-axis of the frustrated tetragonal atiferromagnet Pr2CuO4, a transition is discovered from the phase with orthogonal antiferromagnetic spin subsystems along [1,0,0] and [0,1,0] to the phase with the collinear spins. This phase is shown to be due to the pseudodipolar interaction, and transforms into the spin-flop phase S perp H asymptotically at very high field. The discovered phase transition holds at T=0 and is a quantum one, with the transition field being the critical point and the angle between two subsystems being the order parameter

    Искажение спектра сигнала протяженной цели в радаре с непрерывным частотно-модулированным сигналом

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    The problem of spectrum distortion in radar with a continuous frequency modulated signal (FMCW radar) is considered in the case of locating extended targets containing a large number of closely spaced reflection points. An extended target model is introduced for which a beat signal is analyzed based on its representation in the form of an amplitude-modulated oscillation. It is shown that the distortion of the spectrum occurs due to a certain relationship between the distances of the target points, the values of the carrier frequency and the deviation of the probe signal frequency. The results of numerical calculations for various values of the signal parameters and the long target model are given.En el presente artículo se aborda el problema de la distorsión del espectro en radares con señal continua de frecuencia modulada (radar FMCW) al producir objetivos prolongados que contienen un gran número de puntos de reflexión cercanos. El documento introduce un modelo de objetivo extendido para el cual se realiza un análisis de la señal de los latidos en función de su presentación en forma de oscilación de amplitud modulada. Este estudio muestra que la distorsión del espectro se produce como resultado de ciertas relaciones entre las distancias de los puntos de destino, los valores de frecuencia portadora y la frecuencia de desviación de la señal de sondeo. El artículo presenta los resultados de los cálculos numéricos para los diferentes valores de los parámetros de la señal y el modelo de objetivo extendido.No presente artigo, o problema da distorção do espectro em radares com sinal de frequência modulada contínua (radar FMCW) é abordado ao produzir objetivos prolongados que contêm um grande número de pontos de reflexão próximos. O documento introduz um modelo objetivo estendido para o qual uma análise do sinal de batimentos cardíacos é realizada de acordo com sua apresentação na forma de uma oscilação de amplitude modulada. Este estudo mostra que a distorção do espectro ocorre como resultado de certas relações entre as distâncias dos pontos de destino, os valores da freqüência da portadora e a freqüência do desvio do sinal sonoro. O artigo apresenta os resultados dos cálculos numéricos para os diferentes valores dos parâmetros do sinal e do modelo objetivo estendido.Рассмотрена проблема искажения спектра в радаре с непрерывным частотно-модулированным сигналом (FMCW радаре) при лоцировании протяженных целей, содержащих большое число близкорасположенных точек отражения. Введена модель протяженной цели, для которой проведен анализ сигнала биений на основе представления его в виде амплитудно-модулированного колебания. Показано, что искажение спектра возникает в результате определенных соотношений между расстояниями точек цели, значениями несущей частоты и частоты девиации зондирующего сигнала. Приведены результаты численных расчетов для различных значений параметров сигнала и модели протяженной цели
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