1,351 research outputs found

    A concave-convex problem with a variable operator

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    We study the following elliptic problem A(u)=λuq-A(u) = \lambda u^q with Dirichlet boundary conditions, where A(u)(x)=Δu(x)χD1(x)+Δpu(x)χD2(x)A(u) (x) = \Delta u (x) \chi_{D_1} (x)+ \Delta_p u(x) \chi_{D_2}(x) is the Laplacian in one part of the domain, D1D_1, and the pp-Laplacian (with p>2p>2) in the rest of the domain, D2D_2 . We show that this problem exhibits a concave-convex nature for 1<q<p11<q<p-1. In fact, we prove that there exists a positive value λ\lambda^* such that the problem has no positive solution for λ>λ\lambda > \lambda^* and a minimal positive solution for 0<λ<λ0<\lambda < \lambda^*. If in addition we assume that pp is subcritical, that is, p<2N/(N2)p<2N/(N-2) then there are at least two positive solutions for almost every 0<λ<λ0<\lambda < \lambda^*, the first one (that exists for all 0<λ<λ0<\lambda < \lambda^*) is obtained minimizing a suitable functional and the second one (that is proven to exist for almost every 0<λ<λ0<\lambda < \lambda^*) comes from an appropriate (and delicate) mountain pass argument

    Velocity profiles in shear-banding wormlike micelles

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    Using Dynamic Light Scattering in heterodyne mode, we measure velocity profiles in a much studied system of wormlike micelles (CPCl/NaSal) known to exhibit both shear-banding and stress plateau behavior. Our data provide evidence for the simplest shear-banding scenario, according to which the effective viscosity drop in the system is due to the nucleation and growth of a highly sheared band in the gap, whose thickness linearly increases with the imposed shear rate. We discuss various details of the velocity profiles in all the regions of the flow curve and emphasize on the complex, non-Newtonian nature of the flow in the highly sheared band.Comment: 4 pages, 5 figures, submitted to Phys. Rev. Let

    Cohomological tautness for Riemannian foliations

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    In this paper we present some new results on the tautness of Riemannian foliations in their historical context. The first part of the paper gives a short history of the problem. For a closed manifold, the tautness of a Riemannian foliation can be characterized cohomologically. We extend this cohomological characterization to a class of foliations which includes the foliated strata of any singular Riemannian foliation of a closed manifold

    Polar foliations and isoparametric maps

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    A singular Riemannian foliation FF on a complete Riemannian manifold MM is called a polar foliation if, for each regular point pp, there is an immersed submanifold Σ\Sigma, called section, that passes through pp and that meets all the leaves and always perpendicularly. A typical example of a polar foliation is the partition of MM into the orbits of a polar action, i.e., an isometric action with sections. In this work we prove that the leaves of FF coincide with the level sets of a smooth map H:MΣH: M\to \Sigma if MM is simply connected. In particular, we have that the orbits of a polar action on a simply connected space are level sets of an isoparametric map. This result extends previous results due to the author and Gorodski, Heintze, Liu and Olmos, Carter and West, and Terng.Comment: 9 pages; The final publication is available at springerlink.com http://www.springerlink.com/content/c72g4q5350g513n1

    Young Galaxy Candidates in the Hubble Frontier Fields. I. Abell 2744

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    We report the discovery of 24 Lyman-break candidates at 7<z<10.5, in the Hubble Frontier Fields (HFF) imaging data of Abell 2744 (z=0.308), plus Spiter/IRAC data and archival ACS data. The sample includes a triple image system with a photometric redshift of z~7.4. This high redshift is geometrically confirmed by our lens model corresponding to deflection angles that are 12% larger than the lower-redshift systems used to calibrate the lens model at z=2.019. The majority of our high-redshift candidates are not expected to be multiply lensed given their locations in the image plane and the brightness of foreground galaxies, but are magnified by factors of ~1.3-15, so that we are seeing further down the luminosity function than comparable deep field imaging. It is apparent that the redshift distribution of these sources does not smoothly extend over the full redshift range accessible at z<12, but appears to break above z=9. Nine candidates are clustered within a small region of 20" across, representing a potentially unprecedented concentration. Given the poor statistics, however, we must await similar constraints from the additional HFF clusters to properly examine this trend. The physical properties of our candidates are examined using the range of lens models developed for the HFF program by various groups including our own, for a better estimate of underlying systematics. Our spectral-energy-distribution fits for the brightest objects suggest stellar masses of ~1E9 solar mass, star-formation rates of ~4 solar mass per yr, and a typical formation redshift of z<19.Comment: 17 pages, 7 figures, 6 tables, submitted to the Astrophysical Journa

    Evidence for Ubiquitous, High-EW Nebular Emission in z~7 Galaxies: Towards a Clean Measurement of the Specific Star Formation Rate using a Sample of Bright, Magnified Galaxies

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    Growing observational evidence now indicates that nebular line emission has a significant impact on the rest-frame optical fluxes of z~5-7 galaxies observed with Spitzer. This line emission makes z~5-7 galaxies appear more massive, with lower specific star formation rates. However, corrections for this line emission have been very difficult to perform reliably due to huge uncertainties on the overall strength of such emission at z>~5.5. Here, we present the most direct observational evidence yet for ubiquitous high-EW [OIII]+Hbeta line emission in Lyman-break galaxies at z~7, while also presenting a strategy for an improved measurement of the sSFR at z~7. We accomplish this through the selection of bright galaxies in the narrow redshift window z~6.6-7.0 where the IRAC 4.5 micron flux provides a clean measurement of the stellar continuum light. Observed 4.5 micron fluxes in this window contrast with the 3.6 micron fluxes which are contaminated by the prominent [OIII]+Hbeta lines. To ensure a high S/N for our IRAC flux measurements, we consider only the brightest (H_{160}<26 mag) magnified galaxies we have identified in CLASH and other programs targeting galaxy clusters. Remarkably, the mean rest-frame optical color for our bright seven-source sample is very blue, [3.6]-[4.5]=-0.9+/-0.3. Such blue colors cannot be explained by the stellar continuum light and require that the rest-frame EW of [OIII]+Hbeta be greater than 637 Angstroms for the average source. The bluest four sources from our seven-source sample require an even more extreme EW of 1582 Angstroms. Our derived lower limit for the mean [OIII]+Hbeta EW could underestimate the true EW by ~2x based on a simple modeling of the redshift distribution of our sources. We can also set a robust lower limit of >~4 Gyr^-1 on the specific star formation rates based on the mean SED for our seven-source sample. (abridged)Comment: 9 pages, 6 figures, 1 table, submitted to the Astrophysical Journa

    Tautness for riemannian foliations on non-compact manifolds

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    For a riemannian foliation F\mathcal{F} on a closed manifold MM, it is known that F\mathcal{F} is taut (i.e. the leaves are minimal submanifolds) if and only if the (tautness) class defined by the mean curvature form κμ\kappa_\mu (relatively to a suitable riemannian metric μ\mu) is zero. In the transversally orientable case, tautness is equivalent to the non-vanishing of the top basic cohomology group Hn(M/F)H^{^{n}}(M/\mathcal{F}), where n = \codim \mathcal{F}. By the Poincar\'e Duality, this last condition is equivalent to the non-vanishing of the basic twisted cohomology group Hκμ0(M/F)H^{^{0}}_{_{\kappa_\mu}}(M/\mathcal{F}), when MM is oriented. When MM is not compact, the tautness class is not even defined in general. In this work, we recover the previous study and results for a particular case of riemannian foliations on non compact manifolds: the regular part of a singular riemannian foliation on a compact manifold (CERF).Comment: 18 page

    Finitness of the basic intersection cohomology of a Killing foliation

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    We prove that the basic intersection cohomology IHpˉ(M/F), {I H}^{^{*}}_{_{\bar{p}}}{(M/\mathcal{F})}, where F\mathcal{F} is the singular foliation determined by an isometric action of a Lie group GG on the compact manifold MM, is finite dimensional

    A Census of Star-Forming Galaxies in the z~9-10 Universe based on HST+Spitzer Observations Over 19 CLASH clusters: Three Candidate z~9-10 Galaxies and Improved Constraints on the Star Formation Rate Density at z~9

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    We utilise a two-color Lyman-Break selection criterion to search for z~9-10 galaxies over the first 19 clusters in the CLASH program. A systematic search yields three z~9-10 candidates. While we have already reported the most robust of these candidates, MACS1149-JD, two additional z~9 candidates are also found and have H_{160}-band magnitudes of ~26.2-26.9. A careful assessment of various sources of contamination suggests <~1 contaminants for our z~9-10 selection. To determine the implications of these search results for the LF and SFR density at z~9, we introduce a new differential approach to deriving these quantities in lensing fields. Our procedure is to derive the evolution by comparing the number of z~9-10 galaxy candidates found in CLASH with the number of galaxies in a slightly lower redshift sample (after correcting for the differences in selection volumes), here taken to be z~8. This procedure takes advantage of the fact that the relative volumes available for the z~8 and z~9-10 selections behind lensing clusters are not greatly dependent on the details of the lensing models. We find that the normalization of the UV LF at z~9 is just 0.28_{-0.20}^{+0.39}\times that at z~8, ~1.4_{-0.8}^{+3.0}x lower than extrapolating z~4-8 LF results. While consistent with the evolution in the UV LF seen at z~4-8, these results marginally favor a more rapid evolution at z>8. Compared to similar evolutionary findings from the HUDF, our result is less insensitive to large-scale structure uncertainties, given our many independent sightlines on the high-redshift universe.Comment: 22 pages, 11 figures, 5 tables, accepted for publication in the Astrophysical Journal, updated to include the much deeper Spitzer/IRAC observations over our three z~9-10 candidate

    A Geometrically Supported z10z\sim10 Candidate Multiply-Imaged by the Hubble Frontier Fields Cluster Abell 2744

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    The deflection angles of lensed sources increase with their distance behind a given lens. We utilize this geometric effect to corroborate the zphot9.8z_{phot}\simeq9.8 photometric redshift estimate of a faint near-IR dropout, triply-imaged by the massive galaxy cluster Abell 2744 in deep Hubble Frontier Fields images. The multiple images of this source follow the same symmetry as other nearby sets of multiple images which bracket the critical curves and have well defined redshifts (up to zspec3.6z_{spec}\simeq3.6), but with larger deflection angles, indicating that this source must lie at a higher redshift. Similarly, our different parametric and non-parametric lens models all require this object be at z4z\gtrsim4, with at least 95\% confidence, thoroughly excluding the possibility of lower-redshift interlopers. To study the properties of this source we correct the two brighter images for their magnifications, leading to a SFR of 0.3M\sim0.3 M_{\odot}/yr, a stellar mass of 4×107M\sim4\times10^{7} M_{\odot}, and an age of 220\lesssim220 Myr (95\% confidence). The intrinsic apparent magnitude is 29.9 AB (F160W), and the rest-frame UV (1500A˚\sim1500 \AA) absolute magnitude is MUV,AB=17.6M_{UV,AB}=-17.6. This corresponds to 0.1Lz=8\sim0.1 L^{*}_{z=8} (0.2Lz=10\sim0.2 L^{*}_{z=10}, adopting dM/dz0.45dM^{*}/dz\sim0.45), making this candidate one of the least luminous galaxies discovered at z10z\sim10.Comment: 7 pages, 4 figures, 1 table; V2: very minor changes, ApJ Letters Accepte
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