1,734 research outputs found

    Constraints on the Asymptotic Baryon Fractions of Galaxy Clusters at Large Radii

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    While X-ray measurements have so far revealed an increase in the volume-averaged baryon fractions fb(r)f_b(r) of galaxy clusters with cluster radii rr, fb(r)f_b(r) should asymptotically reach a universal value fb(∞)=fbf_b(\infty)=f_b, provided that clusters are representative of the Universe. In the framework of hydrostatic equilibrium for intracluster gas, we have derived the necessary conditions for fb(∞)=fbf_b(\infty)=f_b: The X-ray surface brightness profile described by the β\beta model and the temperature profile approximated by the polytropic model should satisfy γ≈2(1−1/3β)\gamma\approx2(1-1/3\beta) and γ≈1+1/3β\gamma\approx1+1/3\beta for β1\beta1, respectively, which sets a stringent limit to the polytropic index: γ<4/3\gamma<4/3. In particular, a mildly increasing temperature with radius is required if the observationally fitted β\beta parameter is in the range 1/3<β<2/31/3<\beta<2/3. It is likely that a reliable determination of the universal baryon fraction can be achieved in the small β\beta clusters because the disagreement between the exact and asymptotic baryon fractions for clusters with β>2/3\beta>2/3 breaks down at rather large radii (\ga30r_c) where hydrostatic equilibrium has probably become inapplicable. We further explore how to obtain the asymptotic value fb(∞)f_b(\infty) of baryon fraction from the X-ray measurement made primarily over the finite central region of a cluster. We demonstrate our method using a sample of 19 strong lensing clusters, which enables us to place a useful constraint on fb(∞)f_b(\infty): 0.094±0.035≤fb(∞)≤0.41±0.180.094\pm0.035 \leq f_b(\infty) \leq 0.41\pm0.18. An optimal estimate of fb(∞)f_b(\infty) based on three cooling flow clusters with β=0.142±0.007\beta = 0.142\pm0.007 or ΩM=0.35±0.09\Omega_M = 0.35\pm0.09.Comment: 6 pages + 4 figures; accepted for publication in MNRA

    Constraints on the warm dark matter model from gravitational lensing

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    Formation of sub-galactic halos is suppressed in warm dark matter (WDM) model due to thermal motion of WDM particles. This may provide a natural resolution to some puzzles in standard cold dark matter (CDM) theory such as the cusped density profiles of virialized dark halos and the overabundance of low mass satellites. One of the observational tests of the WDM model is to measure the gravitationally lensed images of distant quasars below sub-arcsecond scales. In this Letter, we report a comparison of the lensing probabilities of multiple images between CDM and WDM models using a singular isothermal sphere model for the mass density profiles of dark halos and the Press-Schechter mass function for their distribution and cosmic evolution. It is shown that the differential probability of multiple images with small angular separations down to 10 milliarcseconds should allow one to set useful constraints on the WDM particle mass. We discuss briefly the feasibility and uncertainties of this method in future radio surveys (e.g. VLBI) for gravitational lensing.Comment: 3 pages, 1 figure, accepted for publication in ApJ Let

    A comparison of different cluster mass estimates: consistency or discrepancy ?

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    Rich and massive clusters of galaxies at intermediate redshift are capable of magnifying and distorting the images of background galaxies. A comparison of different mass estimators among these clusters can provide useful information about the distribution and composition of cluster matter and their dynamical evolution. Using a hitherto largest sample of lensing clusters drawn from literature, we compare the gravitating masses of clusters derived from the strong/weak gravitational lensing phenomena, from the X-ray measurements based on the assumption of hydrostatic equilibrium, and from the conventional isothermal sphere model for the dark matter profile characterized by the velocity dispersion and core radius of galaxy distributions in clusters. While there is an excellent agreement between the weak lensing, X-ray and isothermal sphere model determined cluster masses, these methods are likely to underestimate the gravitating masses enclosed within the central cores of clusters by a factor of 2--4 as compared with the strong lensing results. Such a mass discrepancy has probably arisen from the inappropriate applications of the weak lensing technique and the hydrostatic equilibrium hypothesis to the central regions of clusters as well as an unreasonably large core radius for both luminous and dark matter profiles. Nevertheless, it is pointed out that these cluster mass estimators may be safely applied on scales greater than the core sizes. Namely, the overall clusters of galaxies at intermediate redshift can still be regarded as the dynamically relaxed systems, in which the velocity dispersion of galaxies and the temperature of X-ray emitting gas are good indicators of the underlying gravitational potentials of clusters.Comment: 16 pages with 7 PS figures, MNRAS in pres

    Correlation Between the Halo Concentration (c) and the Virial Mass (Mvir) Determined from X-ray Clusters

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    Numerical simulations of structure formation have suggested that there exists a good correlation between the halo concentration c (or the characteristic density delta_c) and the virial mass Mvir for any virialized dark halo described by the Navarro, Frenk & White (1995) density profile. In this Letter, we present an observational determination of the c-Mvir (or delta_c-Mvir) relation in the mass range of 10^14< Mvir <10^16 (solar mass) using a sample of 63 X-ray luminous clusters. The best-fit power law relation, which is roughly independent of the values of Omega_M and Lambda, is c propto Mvir^(-0.5) or delta_c propto Mvir^(-1.2), indicating n=-0.7 for a scale-free power spectrum of the primordial density fluctuations. We discuss the possible reasons for the conflict with the predictions by typical CDM models such as SCDM, LCDM and OCDM.Comment: 13 pages, 1 figure, two tables. Accepted for publication in ApJ
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