854 research outputs found

    Arachidonic acid-induced release of calcium in permeabilized human neutrophils

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    AbstractThe addition of arachidonic acid to a suspension of digitonin-permeabilized human neutrophils was found to induce, in a dose-dependent manner (ED50 about 15 μM), the release of calcium from internal stores. Arachidic acid was without effect, while linoleic acid and linolenic acid were (on a concentration basis) at least 5-times less active than arachidonic acid. The activity of arachidonic acid appears to be due to the fatty acid itself and not to one of its metabolites. The pool of calcium mobilized by arachidonic acid includes that sensitive to inositol 1,4,5-trisphosphate. These results demonstrate a significant intracellular role for arachidonic acid at the level of the internal mobilization of calcium in human neutrophils

    Strongly Time-Variable Ultra-Violet Metal Line Emission from the Circum-Galactic Medium of High-Redshift Galaxies

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    We use cosmological simulations from the Feedback In Realistic Environments (FIRE) project, which implement a comprehensive set of stellar feedback processes, to study ultra-violet (UV) metal line emission from the circum-galactic medium of high-redshift (z=2-4) galaxies. Our simulations cover the halo mass range Mh ~ 2x10^11 - 8.5x10^12 Msun at z=2, representative of Lyman break galaxies. Of the transitions we analyze, the low-ionization C III (977 A) and Si III (1207 A) emission lines are the most luminous, with C IV (1548 A) and Si IV (1394 A) also showing interesting spatially-extended structures. The more massive halos are on average more UV-luminous. The UV metal line emission from galactic halos in our simulations arises primarily from collisionally ionized gas and is strongly time variable, with peak-to-trough variations of up to ~2 dex. The peaks of UV metal line luminosity correspond closely to massive and energetic mass outflow events, which follow bursts of star formation and inject sufficient energy into galactic halos to power the metal line emission. The strong time variability implies that even some relatively low-mass halos may be detectable. Conversely, flux-limited samples will be biased toward halos whose central galaxy has recently experienced a strong burst of star formation. Spatially-extended UV metal line emission around high-redshift galaxies should be detectable by current and upcoming integral field spectrographs such as the Multi Unit Spectroscopic Explorer (MUSE) on the Very Large Telescope and Keck Cosmic Web Imager (KCWI).Comment: 16 pages, 8 figures, accepted for publication in MNRA

    Magnetic and Thermodynamic Properties of the Collective Paramagnet-Spin Liquid Pyrochlore Tb2Ti2O7

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    In a recent letter [Phys. Rev. Lett. {\bf 82}, 1012 (1999)] it was found that the Tb3+^{3+} magnetic moments in the Tb2_2Ti2_2O7_7 pyrochlore lattice of corner-sharing tetrahedra remain in a {\it collective paramagnetic} state down to 70mK. In this paper we present results from d.c. magnetic susceptibility, specific heat data, inelastic neutron scattering measurements, and crystal field calculations that strongly suggest that (1) the Tb3+^{3+} ions in Tb2_2Ti2_2O7_7 possess a moment of approximatively 5μB\mu_{\rm B}, and (2) the ground state gg-tensor is extremely anisotropic below a temperature of O(100)O(10^0)K, with Ising-like Tb3+^{3+} magnetic moments confined to point along a local cubic diagonal(e.g.towardsthemiddleofthetetrahedron).SuchaverylargeeasyaxisIsinglikeanisotropyalonga diagonal (e.g. towards the middle of the tetrahedron). Such a very large easy-axis Ising like anisotropy along a direction dramatically reduces the frustration otherwise present in a Heisenberg pyrochlore antiferromagnet. The results presented herein underpin the conceptual difficulty in understanding the microscopic mechanism(s) responsible for Tb2_2Ti2_2O7_7 failing to develop long-range order at a temperature of the order of the paramagnetic Curie-Weiss temperature θCW101\theta_{\rm CW} \approx -10^1K. We suggest that dipolar interactions and extra perturbative exchange coupling(s)beyond nearest-neighbors may be responsible for the lack of ordering of Tb2_2Ti2_2O7_7.Comment: 8 POSTSCRIPT figures included. Submitted to Physical Review B. Contact: [email protected]

    Modelling chemical abundance distributions for dwarf galaxies in the Local Group: the impact of turbulent metal diffusion

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    We investigate stellar metallicity distribution functions (MDFs), including Fe and α{\alpha}-element abundances, in dwarf galaxies from the Feedback in Realistic Environments (FIRE) project. We examine both isolated dwarf galaxies and those that are satellites of a Milky Way-mass galaxy. In particular, we study the effects of including a sub-grid turbulent model for the diffusion of metals in gas. Simulations that include diffusion have narrower MDFs and abundance ratio distributions, because diffusion drives individual gas and star particles toward the average metallicity. This effect provides significantly better agreement with observed abundance distributions of dwarf galaxies in the Local Group, including the small intrinsic scatter in [α{\alpha}/Fe] vs. [Fe/H] (less than 0.1 dex). This small intrinsic scatter arises in our simulations because the interstellar medium (ISM) in dwarf galaxies is well-mixed at nearly all cosmic times, such that stars that form at a given time have similar abundances to within 0.1 dex. Thus, most of the scatter in abundances at z = 0 arises from redshift evolution and not from instantaneous scatter in the ISM. We find similar MDF widths and intrinsic scatter for satellite and isolated dwarf galaxies, which suggests that environmental effects play a minor role compared with internal chemical evolution in our simulations. Overall, with the inclusion of metal diffusion, our simulations reproduce abundance distribution widths of observed low-mass galaxies, enabling detailed studies of chemical evolution in galaxy formation.Comment: 19 pages, 13 figures, published in MNRA

    What Does a habitus of the Soul Do? : The Case of the habitus of Faith in Bonaventure, Peter John Olivi and John Duns Scotus

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    While a habitus can be described as a disposition towards a certain type of act, such a definition is not sufficient to encompass the diversity of uses the medieval thinkers made of this concept. It is the aim of this paper to examine the habitus of faith in the voluntarist Franciscan tradition in order to illustrate several of its functions and how these varied from author to author. Studying how the habitus of faith works for Bonaventure, Peter John Olivi and John Duns Scotus allows us to examine different takes on these functions and illustrate the variety of possible positions even within a tradition that emphasizes the freedom and agency of the moral subject above all. We will emphasize the capacity a habitus grants to pick out its proper objects, in the present case, the objects of faith; the capacity to elicit certain acts that without it would not have been possible or at least that would not have had the moral value the habitus grants them; the capacity to unite several powers in the accomplishment of a given act.Peer reviewe

    Femtosecond time resolved CARS spectroscopy of H2-N2 mixtures in the Dicke regime: Experiments and modeling of velocity effects

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    International audienceIn this paper, we present measurements and modeling of femtosecond time resolved CARS signal in H2-N2 mixtures at low densities. Three approaches have been used to model the CARS response. The first is the usual sum of Voigt profiles. In the second approach, the speed dependent Voigt profile is used. In the last approach, a new model of the CARS signal is developed which takes into account the velocity changes induced by collisions and the speed dependence of the collisional parameters. The velocity changes are modeled using the Keilson and Storer memory function; the radiator speed dependences of the collisional parameters are determined from their temperature dependences. The results show that the changes of the velocity have important effects for the H2/N2 system at the Dicke density regime
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