10,631 research outputs found

    The stellar mass-halo mass relation of isolated field dwarfs: a critical test of Λ\LambdaCDM at the edge of galaxy formation

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    We fit the rotation curves of isolated dwarf galaxies to directly measure the stellar mass-halo mass relation (M∗−M200M_*-M_{200}) over the mass range 5×105<M∗/M⊙<1085 \times 10^5 < M_{*}/{\rm M}_\odot < 10^{8}. By accounting for cusp-core transformations due to stellar feedback, we find a monotonic relation with little scatter. Such monotonicity implies that abundance matching should yield a similar M∗−M200M_*-M_{200} if the cosmological model is correct. Using the 'field galaxy' stellar mass function from the Sloan Digital Sky Survey (SDSS) and the halo mass function from the Λ\Lambda Cold Dark Matter Bolshoi simulation, we find remarkable agreement between the two. This holds down to M200∼5×109M_{200} \sim 5 \times 10^9M⊙_\odot, and to M200∼5×108M_{200} \sim 5 \times 10^8M⊙_\odot if we assume a power law extrapolation of the SDSS stellar mass function below M∗∼107M_* \sim 10^7M⊙_\odot. However, if instead of SDSS we use the stellar mass function of nearby galaxy groups, then the agreement is poor. This occurs because the group stellar mass function is shallower than that of the field below M∗∼109M_* \sim 10^9M⊙_\odot, recovering the familiar 'missing satellites' and 'too big to fail' problems. Our result demonstrates that both problems are confined to group environments and must, therefore, owe to 'galaxy formation physics' rather than exotic cosmology. Finally, we repeat our analysis for a Λ\Lambda Warm Dark Matter cosmology, finding that it fails at 68% confidence for a thermal relic mass of mWDM<1.25m_{\rm WDM} < 1.25keV, and mWDM<2m_{\rm WDM} < 2keV if we use the power law extrapolation of SDSS. We conclude by making a number of predictions for future surveys based on these results.Comment: 22 pages; 2 Tables; 10 Figures. This is the version accepted for publication in MNRAS. Key changes: (i) added substantially more information on the surveys used to measure the stellar mass functions; (ii) added tests of the robustness of our results. Results and conclusions unchanged from previously. Minor typos corrected from previous versio

    Dark matter cores all the way down

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    We use high resolution simulations of isolated dwarf galaxies to study the physics of dark matter cusp-core transformations at the edge of galaxy formation: M200 = 10^7 - 10^9 Msun. We work at a resolution (~4 pc minimum cell size; ~250 Msun per particle) at which the impact from individual supernovae explosions can be resolved, becoming insensitive to even large changes in our numerical 'sub-grid' parameters. We find that our dwarf galaxies give a remarkable match to the stellar light profile; star formation history; metallicity distribution function; and star/gas kinematics of isolated dwarf irregular galaxies. Our key result is that dark matter cores of size comparable to the stellar half mass radius (r_1/2) always form if star formation proceeds for long enough. Cores fully form in less than 4 Gyrs for the M200 = 10^8 Msun and 14 Gyrs for the 10^9 Msun dwarf. We provide a convenient two parameter 'coreNFW' fitting function that captures this dark matter core growth as a function of star formation time and the projected stellar half mass radius. Our results have several implications: (i) we make a strong prediction that if LCDM is correct, then 'pristine' dark matter cusps will be found either in systems that have truncated star formation and/or at radii r > r_1/2; (ii) complete core formation lowers the projected velocity dispersion at r_1/2 by a factor ~2, which is sufficient to fully explain the 'too big to fail problem'; and (iii) cored dwarfs will be much more susceptible to tides, leading to a dramatic scouring of the subhalo mass function inside galaxies and groups.Comment: 20 pages; 9 figures; final version to appear in MNRAS including typos corrected in proo

    The Baking Temperature of Bread

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    The purpose of this investigation is to study the temperature of a loaf of bread during the baking process. In the study of fermentation and its application to the rising and baking of bread the questions arose; how high a temperature is attained inside the loaf, is the rise of temperature uniform, or are there points of rapid change. It was thought as the boiling temperature of alcohol was approached or passed some noticeable temperature change might occur. Also that as the crust on the bread was formed and became more rigid thus having a tendency to exert pressure on the inside of the loaf, a rise in temperature would be noted. It was also desired to determine as the condition known as done was reached whether or not a marked rise of temperature might occur

    Reduced-order models of the Martian atmospheric dynamics

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    In this paper we explore the possibility of deriving low-dimensional models of the dynamics of the Martian atmosphere. The analysis consists of a Proper Orthogonal Decomposition (POD) of the atmospheric streamfunction after first decomposing the vertical structure with a set of eigenmodes. The vertical modes were obtained from the quasi-geostrophic vertical structure equation. The empirical orthogonal functions (EOFs) were optimized to represent the atmospheric total energy. The total energy was used as the criterion to retain those modes with large energy content and discard the rest. The principal components (PCs) were analysed by means of Fourier analysis, so that the dominant frequencies could be identified. It was possible to observe the strong influence of the diurnal cycle and to identify the motion and vacillation of baroclinic waves

    Inter-limb asymmetry during rehabilitation understanding formulas and monitoring the "magnitude" and "direction"

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    This article outlines how asymmetry can be used during the rehabilitation process for practitioners, and the importance of both the magnitude and direction of an inter-limb asymmetry
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