1,456 research outputs found

    Cold giant planets evaporated by hot white dwarfs

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    Atmospheric escape from close-in Neptunes and hot Jupiters around Sun-like stars driven by extreme ultraviolet (EUV) irradiation plays an important role in the evolution of exoplanets and in shaping their ensemble properties. Intermediate and low mass stars are brightest at EUV wavelengths at the very end of their lives, after they have expelled their envelopes and evolved into hot white dwarfs. Yet the effect of the intense EUV irradiation of giant planets orbiting young white dwarfs has not been assessed. We show that the giant planets in the solar system will experience significant hydrodynamic escape caused by the EUV irradiation from the white dwarf left behind by the Sun. A fraction of the evaporated volatiles will be accreted by the solar white dwarf, resulting in detectable photospheric absorption lines. As a large number of the currently known extrasolar giant planets will survive the metamorphosis of their host stars into white dwarfs, observational signatures of accretion from evaporating planetary atmospheres are expected to be common. In fact, one-third of the known hot single white dwarfs show photospheric absorption lines of volatile elements, which we argue are indicative of ongoing accretion from evaporating planets. The fraction of volatile contaminated hot white dwarfs strongly decreases as they cool. We show that accretion from evaporating planetary atmospheres naturally explains this temperature dependence if more than 50% of hot white dwarfs still host giant planets

    Dynamic equilibrium sets atomic content of galaxies across cosmic time

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    We analyze 88 independent high-resolution cosmological zoom-in simulations of disk galaxies in the NIHAO simulations suite to explore the connection between the atomic gas fraction and angular momentum of baryons throughout cosmic time. The study is motivated by the analytic model of \citet{obreschkow16}, which predicts a relation between the atomic gas fraction fatmf_{\rm atm} and the global atomic stability parameter q≡jσ/(GM)q \equiv j\sigma / (GM), where MM and jj are the mass and specific angular momentum of the galaxy (stars+cold gas) and σ\sigma is the velocity dispersion of the atomic gas. We show that the simulated galaxies follow this relation from their formation (z≃4z\simeq4) to present within ∼0.5\sim 0.5 dex. To explain this behavior, we explore the evolution of the local Toomre stability and find that 90%90\%--100%100\% of the atomic gas in all simulated galaxies is stable at any time. In other words, throughout the entire epoch of peak star formation until today, the timescale for accretion is longer than the timescale to reach equilibrium, thus resulting in a quasi-static equilibrium of atomic gas at any time. Hence, the evolution of fatmf_{\rm atm} depends on the complex hierarchical growth history primarily via the evolution of qq. An exception are galaxies subject to strong environmental effects.Comment: 12 pages, 7 figures; accepted to Ap

    Analysis of Emotional Intelligence as a Competition for Effective Productivity

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    Background. Emotional intelligence is an essential competence that must be evaluated within a personnel selection process. The level of IE influences the results of a company favorably. In this research, the dependence that exists between the effective productivity of the workers in specific of the commercial area and the emotional intelligence was analyzed. Methodology. The studied population was 88 active workers in the area as mentioned earlier; 40% were male and 60% female. Those evaluated were aged 25 to 40 years, with experience in the average sales area of 3 years. To validate the questions that were handled as an instrument, the Pearson correlation was used; Chi-square to calculate the dependence of variables. Results and discussion. As a result, we obtained ten dependent variables with which we can conclude that there is a relationship between the level of emotional intelligence with the effective productivity that collaborates with the commercial area within an organization. Conclusion. Based on the results we conclude that people with a high level of Emotional Self-understanding (AE) can control their emotions to act correctly in each situation

    Extremely Metal-Poor Galaxies: The HI Content

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    Extremely metal-poor (XMP) galaxies are chemically, and possibly dynamically, primordial objects in the local Universe. Our objective is to characterize the HI content of the XMP galaxies as a class, using as a reference the list of 140 known local XMPs compiled by Morales-Luis et al. (2011). We have observed 29 XMPs, which had not been observed before at 21 cm, using the Effelsberg radio telescope. This information was complemented with HI data published in literature for a further 53 XMPs. In addition, optical data from the literature provided morphologies, stellar masses, star-formation rates and metallicities. Effelsberg HI integrated flux densities are between 1 and 15 Jy km/s, while line widths are between 20 and 120 km/s. HI integrated flux densities and line widths from literature are in the range 0.1 - 200 Jy km/s and 15 - 150 km/s, respectively. Of the 10 new Effelsberg detections, two sources show an asymmetric double-horn profile, while the remaining sources show either asymmetric (7 sources) or symmetric (1 source) single-peak 21 cm line profiles. An asymmetry in the HI line profile is systematically accompanied by an asymmetry in the optical morphology. Typically, the g-band stellar mass-to-light ratios are ~0.1, whereas the HI gas mass-to-light ratios may be up to 2 orders of magnitude larger. Moreover, HI gas-to-stellar mass ratios fall typically between 10 and 20, denoting that XMPs are extremely gas-rich. We find an anti-correlation between the HI gas mass-to-light ratio and the luminosity, whereby fainter XMPs are more gas-rich than brighter XMPs, suggesting that brighter sources have converted a larger fraction of their HI gas into stars. The dynamical masses inferred from the HI line widths imply that the stellar mass does not exceed 5% of the dynamical mass, while the \ion{H}{i} mass constitutes between 20 and 60% of the dynamical mass. (abridged)Comment: 30 pages, accepted for A&
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