7,130 research outputs found

    Intermediate-mass black holes in dwarf galaxies out to redshift \sim 2.4 in the Chandra COSMOS Legacy Survey

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    We present a sample of 40 AGN in dwarf galaxies at redshifts zz \lesssim 2.4. The galaxies are drawn from the \textit{Chandra} COSMOS-Legacy survey as having stellar masses 107M3×10910^{7}\leq M_{*}\leq3 \times 10^{9} M_{\odot}. Most of the dwarf galaxies are star-forming. After removing the contribution from star formation to the X-ray emission, the AGN luminosities of the 40 dwarf galaxies are in the range L0.510keV10391044L_\mathrm{0.5-10 keV} \sim10^{39} - 10^{44} erg s1^{-1}. With 12 sources at z>0.5z > 0.5, our sample constitutes the highest-redshift discovery of AGN in dwarf galaxies. The record-holder is cid\_1192, at z=2.39z = 2.39 and with L0.510keV1044L_\mathrm{0.5-10 keV} \sim 10^{44} erg s1^{-1}. One of the dwarf galaxies has M=6.6×107M_\mathrm{*} = 6.6 \times 10^{7} M_{\odot} and is the least massive galaxy found so far to host an AGN. All the AGN are of type 2 and consistent with hosting intermediate-mass black holes (BHs) with masses 104105\sim 10^{4} - 10^{5} M_{\odot} and typical Eddington ratios >1%> 1\%. We also study the evolution, corrected for completeness, of AGN fraction with stellar mass, X-ray luminosity, and redshift in dwarf galaxies out to zz = 0.7. We find that the AGN fraction for 109<M3×10910^{9}< M_{*}\leq3 \times 10^{9} M_{\odot} and LX10411042L_\mathrm{X} \sim 10^{41}-10^{42} erg s1^{-1} is \sim0.4\% for zz \leq 0.3 and that it decreases with X-ray luminosity and decreasing stellar mass. Unlike massive galaxies, the AGN fraction seems to decrease with redshift, suggesting that AGN in dwarf galaxies evolve differently than those in high-mass galaxies. Mindful of potential caveats, the results seem to favor a direct collapse formation mechanism for the seed BHs in the early Universe.Comment: 16 pages, 10 figures, accepted for publication in MNRA

    A quasi-time-dependent radiative transfer model of OH104.9+2.4

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    We investigate the pulsation-phase dependent properties of the circumstellar dust shell (CDS) of the OH/IR star OH104.9+2.4 based on radiative transfer modeling (RTM) using the code DUSTY. Our previous study concerning simultaneous modeling of the spectral energy distribution (SED) and near-infrared (NIR) visibilities (Riechers et al. 2004) has now been extended by means of a more detailed analysis of the pulsation-phase dependence of the model parameters of OH104.9+2.4. In order to investigate the temporal variation in the spatial structure of the CDS, additional NIR speckle interferometric observations in the K' band were carried out with the 6 m telescope of the Special Astrophysical Observatory (SAO). At a wavelength of 2.12 micron the diffraction-limited resolution of 74 mas was attained. Several key parameters of our previous best-fitting model had to be adjusted in order to be consistent with the newly extended amount of observational data. It was found that a simple rescaling of the bolometric flux F_bol is not sufficient to take the variability of the source into account, as the change in optical depth over a full pulsation cycle is rather high. On the other hand, the impact of a change in effective temperature T_eff on SED and visibility is rather small. However, observations, as well as models for other AGB stars, show the necessity of including a variation of T_eff with pulsation phase in the radiative transfer models. Therefore, our new best-fitting model accounts for these changes.Comment: 7 pages, including 5 postscript figures and 3 tables. Published in Astronomy and Astrophysics. (v1: accepted version; v2: published version, minor grammatical changes

    Interplay between carrier and impurity concentrations in annealed Ga1x_{1-x}Mnx_{x}As intrinsic anomalous Hall Effect

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    Investigating the scaling behavior of annealed Ga1x_{1-x}Mnx_{x}As anomalous Hall coefficients, we note a universal crossover regime where the scaling behavior changes from quadratic to linear, attributed to the anomalous Hall Effect intrinsic and extrinsic origins, respectively. Furthermore, measured anomalous Hall conductivities when properly scaled by carrier concentration remain constant, equal to theoretically predicated values, spanning nearly a decade in conductivity as well as over 100 K in TC_{C}. Both the qualitative and quantitative agreement confirms the validity of new equations of motion including the Berry phase contributions as well as tunablility of the intrinsic anomalous Hall Effect.Comment: 4 pages, 5 figure

    Shear stress fluctuations in the granular liquid and solid phases

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    We report on experimentally observed shear stress fluctuations in both granular solid and fluid states, showing that they are non-Gaussian at low shear rates, reflecting the predominance of correlated structures (force chains) in the solidlike phase, which also exhibit finite rigidity to shear. Peaks in the rigidity and the stress distribution's skewness indicate that a change to the force-bearing mechanism occurs at the transition to fluid behaviour, which, it is shown, can be predicted from the behaviour of the stress at lower shear rates. In the fluid state stress is Gaussian distributed, suggesting that the central limit theorem holds. The fibre bundle model with random load sharing effectively reproduces the stress distribution at the yield point and also exhibits the exponential stress distribution anticipated from extant work on stress propagation in granular materials.Comment: 11 pages, 3 figures, latex. Replacement adds journal reference and addresses referee comment
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