266 research outputs found

    Characteristics of anomalously high multiplicity cosmic ray interactions

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    Six events with the number of secondaries ranging from 250 to several thousands were registered by an installation consisting of a thin graphite target, above and under which are placed photolayers followed by the usual lead X-ray film and emulsion chambers. Data concerning the number of secondaries and their angular distribution are given. The variance of the angular distribution is compared with data obtained at accelerator energies

    Roughness of moving elastic lines - crack and wetting fronts

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    We investigate propagating fronts in disordered media that belong to the universality class of wetting contact lines and planar tensile crack fronts. We derive from first principles their nonlinear equations of motion, using the generalized Griffith criterion for crack fronts and three standard mobility laws for contact lines. Then we study their roughness using the self-consistent expansion. When neglecting the irreversibility of fracture and wetting processes, we find a possible dynamic rough phase with a roughness exponent of ζ=1/2\zeta=1/2 and a dynamic exponent of z=2. When including the irreversibility, we conclude that the front propagation can become history dependent, and thus we consider the value ζ=1/2\zeta=1/2 as a lower bound for the roughness exponent. Interestingly, for propagating contact line in wetting, where irreversibility is weaker than in fracture, the experimental results are close to 0.5, while for fracture the reported values of 0.55--0.65 are higher.Comment: 15 pages, 6 figure

    Hydrodynamic theory of de-wetting

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    A prototypical problem in the study of wetting phenomena is that of a solid plunging into or being withdrawn from a liquid bath. In the latter, de-wetting case, a critical speed exists above which a stationary contact line is no longer sustainable and a liquid film is being deposited on the solid. Demonstrating this behavior to be a hydrodynamic instability close to the contact line, we provide the first theoretical explanation of a classical prediction due to Derjaguin and Levi: instability occurs when the outer, static meniscus approaches the shape corresponding to a perfectly wetting fluid

    Asymptotic theory for a moving droplet driven by a wettability gradient

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    An asymptotic theory is developed for a moving drop driven by a wettability gradient. We distinguish the mesoscale where an exact solution is known for the properly simplified problem. This solution is matched at both -- the advancing and the receding side -- to respective solutions of the problem on the microscale. On the microscale the velocity of movement is used as the small parameter of an asymptotic expansion. Matching gives the droplet shape, velocity of movement as a function of the imposed wettability gradient and droplet volume.Comment: 8 fig

    Quasicontinuum γ\gamma-decay of 91,92^{91,92}Zr: benchmarking indirect (n,γn,\gamma) cross section measurements for the ss-process

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    Nuclear level densities (NLDs) and γ\gamma-ray strength functions (γ\gammaSFs) have been extracted from particle-γ\gamma coincidences of the 92^{92}Zr(p,p′γp,p' \gamma)92^{92}Zr and 92^{92}Zr(p,dγp,d \gamma)91^{91}Zr reactions using the Oslo method. The new 91,92^{91,92}Zr γ\gammaSF data, combined with photonuclear cross sections, cover the whole energy range from Eγ≈1.5E_{\gamma} \approx 1.5~MeV up to the giant dipole resonance at Eγ≈17E_{\gamma} \approx 17~MeV. The wide-range γ\gammaSF data display structures at Eγ≈9.5E_{\gamma} \approx 9.5~MeV, compatible with a superposition of the spin-flip M1M1 resonance and a pygmy E1E1 resonance. Furthermore, the γ\gammaSF shows a minimum at Eγ≈2−3E_{\gamma} \approx 2-3~MeV and an increase at lower γ\gamma-ray energies. The experimentally constrained NLDs and γ\gammaSFs are shown to reproduce known (n,γn, \gamma) and Maxwellian-averaged cross sections for 91,92^{91,92}Zr using the {\sf TALYS} reaction code, thus serving as a benchmark for this indirect method of estimating (n,γn, \gamma) cross sections for Zr isotopes.Comment: 10 pages and 9 figure

    Partial level density of the n-quasiparticle excitations in the nuclei of the 39< A <201 region

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    Level density and radiative strength functions are obtained from the analysis of two-step cascades intensities following the thermal neutrons capture. The data on level density are approximated by the sum of the partial level densities corresponding to n quasiparticles excitation. The most probable values of the collective enhancement factor of the level density are found together with the thresholds of the next Cooper nucleons pair breaking. These data allow one to calculate the level density of practically any nucleus in given spin window in the framework of model concepts, taking into account all known nuclear excitation types. The presence of an approximation results discrepancy with theoretical statements specifies the necessity of rather essentially developing the level density models. It also indicates the possibilities to obtain the essentially new information on nucleon correlation functions of the excited nucleus from the experiment.Comment: 29 pages, 8 figures, 2 table

    Level density of 56^{56}Fe and low-energy enhancement of γ\gamma-strength function

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    The 55^{55}Mn(d,n)56(d,n)^{56}Fe differential cross section is measured at Ed=7E_d=7 MeV\@. The 56^{56}Fe level density obtained from neutron evaporation spectra is compared to the level density extracted from the 57^{57}Fe(3(^3He,αγ)56\alpha\gamma)^{56}Fe reaction by the Oslo-type technique. Good agreement is found between the level densities determined by the two methods. With the level density function obtained from the neutron evaporation spectra, the 56^{56}Fe γ\gamma-strength function is also determined from the first-generation γ\gamma matrix of the Oslo experiment. The good agreement between the past and present results for the γ\gamma-strength function supports the validity of both methods and is consistent with the low-energy enhancement of the γ\gamma strength below ∼4\sim 4 MeV first discovered by the Oslo method in iron and molybdenum isotopes.Comment: 7 pages, 5 figure

    Understanding Human and Ecosystem Dynamics in the Kola Arctic : A Participatory Integrated Study

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    The Lake Imandra watershed is located in one of the most developed regions in the Arctic - the Kola Peninsula of Russia. Approximately 300 000 people live on the roughly 27 000 km² watershed, making it one of the most densely populated areas of the Arctic. Most of the people are involved in large-scale mineral extraction and processing and the infrastructure needed to support this industry. This paper reports the results of a pilot project staged for the Lake Imandra watershed that has put human dynamics within the framework of ecosystem change to integrate available information and formulate conceptual models of likely future scenarios. The observation period is one of both rapid economic growth and human expansion, with an overall economic decline in the past decade. We are applying the Participatory Integrated Assessment (PIA) approach to integrate information, identify information gaps, generate likely future scenarios, and link scientific findings to the decision-making process. We found an increasingly vulnerable human population in varying states of awareness about their local environment and fully cognizant of their economic troubles, with many determined to attempt maintenance of relatively high population densities in the near future even as many residents of northern Russia migrate south. A series of workshops have involved the citizens and local decision makers in an attempt to tap their knowledge of the region and to increase their awareness about the linkages between the socioeconomic and ecological components.Le bassin hydrographique du lac Imandra est situé dans l'une des régions les plus développées de l'Arctique, soit la presqu'île de Kola, en Russie. Près de 300 000 personnes vivent dans la zone du bassin qui couvre environ 27 000 km², ce qui en fait l'une des régions les plus peuplées de l'Arctique. La plupart des habitants travaillent dans l'extraction et le traitement miniers à grande échelle ainsi que dans l'infrastructure qui soutient cette industrie. Le présent article rapporte les résultats d'un projet pilote mis sur pied pour le bassin du lac Imandra, projet qui a placé la dynamique humaine dans le cadre du changement des écosystèmes, afin d'intégrer l'information disponible et de formuler des modèles conceptuels de scénarios probables dans l'avenir. La période d'observation en est une à la fois de croissance économique et d'expansion démographique rapides, suivie d'un déclin général au cours de la dernière décennie. On a recours à la méthode d'évaluation participative intégrée (EPI) pour intégrer l'information, y dégager des lacunes, générer des scénarios probables dans l'avenir et établir un lien entre résultats de la recherche et processus décisionnel. On a trouvé qu'il y avait une population humaine de plus en plus vulnérable qui était sensibilisée à divers degrés aux problèmes locaux de l'environnement et pleinement consciente des difficultés économiques, population dont une bonne part était fermement décidée à tenter de maintenir à brève échéance des densités de population relativement élevées, alors même que les résidents du nord de la Russie migrent en grand nombre vers le Sud. On a tenu une série d'ateliers avec citoyens et décideurs locaux pour chercher à capter leurs connaissances de la région et à accroître leur sensibilisation aux liens existant entre les composantes socio-économiques et écologiques
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