Abstract:We investigate the well‐known correlations between the dynamical mass‐to‐light ratio (M/L) and other global observables of elliptical (E) and lenticular (S0) galaxies. We construct two‐integral Jeans and three‐integral Schwarzschild dynamical models for a sample of 25 E/S0 galaxies with SAURON integral‐field stellar kinematics to about one effective (half‐light) radius Re. They have well‐calibrated I‐band Hubble Space Telescope WFPC2 and large‐field ground‐based photometry, accurate surface brightness fluctuat… Show more
“…assumptions are supported by results of realistic simulations carried out by Lablanche et al (2012) and previous works (Cappellari et al 2006;Cappellari 2008) that have shown that the errors introduced by the uncertainty in these quantities are insignificant compared to the errors on the stellar kinematics of our galaxies.…”
We present the results on the stellar Initial Mass Function (IMF) normalisation of 68 massive (M * = 10 11 − 10 12 M ⊙ ) Early-Type Galaxies (ETGs) at redshift of ∼1. This was achieved by deriving the stellar Mass-to-Light ratio (M/L) of the galaxies through axis-symmetric dynamical modelling and comparing it to the same derived via stellar population modelling through full spectrum fitting. The study also employs an Abundance Matching technique to account for the dark matter within the galaxies. The results demonstrate that massive ETGs at high redshifts on average have a Salpeter-like IMF normalisation, while providing observational evidence supporting previous predictions of low dark matter fraction in the inner regions (<1R e ) of galaxies at higher redshift.
“…assumptions are supported by results of realistic simulations carried out by Lablanche et al (2012) and previous works (Cappellari et al 2006;Cappellari 2008) that have shown that the errors introduced by the uncertainty in these quantities are insignificant compared to the errors on the stellar kinematics of our galaxies.…”
We present the results on the stellar Initial Mass Function (IMF) normalisation of 68 massive (M * = 10 11 − 10 12 M ⊙ ) Early-Type Galaxies (ETGs) at redshift of ∼1. This was achieved by deriving the stellar Mass-to-Light ratio (M/L) of the galaxies through axis-symmetric dynamical modelling and comparing it to the same derived via stellar population modelling through full spectrum fitting. The study also employs an Abundance Matching technique to account for the dark matter within the galaxies. The results demonstrate that massive ETGs at high redshifts on average have a Salpeter-like IMF normalisation, while providing observational evidence supporting previous predictions of low dark matter fraction in the inner regions (<1R e ) of galaxies at higher redshift.
“…Dynamical modeling using the orbitsuperposition method is considered to be the state-of-theart technique and allows one to recover both the galaxy gravitational potential and the orbital structure with an accuracy of 15% (Thomas et al 2005;Krajnovic et al 2005). Schwarzschild modeling is now widely used for mass measurements of supermassive black holes, for determination of the total mass profile and its decomposition into luminous and dark matter components as well as for constraining the orbital structure (e.g., Gebhardt et al 2003;Cappellari et al 2006; Thomas et al 2007bThomas et al , 2011McConnell et al 2012McConnell et al , 2013Rusli et al 2013). As such an approach only makes sense with high quality observational data allowing the determination of the high order lineof-sight velocity moments (namely, in addition to velocity and projected velocity dispersion also the third and the fourth order Gauss-Hermite moments (e.g., Gerhard 1993;van der Marel and Franx 1993) or better yet the complete line-of-sight velocity distribution), it can only be applied to nearby galaxies.…”
We compare the performance of mass estimators for elliptical galaxies that rely on the directly observable surface brightness and velocity dispersion profiles, without invoking computationally expensive detailed modeling. These methods recover the mass at a specific radius where the mass estimate is expected to be least sensitive to the anisotropy of stellar orbits. One method (Wolf et al. 2010) uses the total luminosityweighted velocity dispersion and evaluates the mass at a 3D half-light radius r 1/2 , i.e., it depends on the global galaxy properties. Another approach (Churazov et al. 2010) estimates the mass from the velocity dispersion at a radius R 2 where the surface brightness declines as R −2 , i.e., it depends on the local properties. We evaluate the accuracy of the two methods for analytical models, simulated galaxies and real elliptical galaxies that have already been modeled by the Schwarzschild's orbit-superposition technique. Both estimators recover an almost unbiased circular speed estimate with a modest RMS scatter ( 10%). Tests on analytical models and simulated galaxies indicate that the local estimator has a smaller RMS scatter than the global one. We show by examination of simulated galaxies that the projected velocity dispersion at R 2 could serve as a good proxy for the virial galaxy mass. For simulated galaxies the total halo mass scales with σ p (R 2 ) as M vir M ⊙ h −1 ≈ 6 · 10 12 σ p (R 2 ) 200 km s −1 4 with RMS scatter ≈ 40%.
“…2, we show the same trends but now as a function of the total mass of the galaxies. We have derived the mass values assuming it approximates to the virial mass derived from the best-fitting M vir − σ relation presented in [1]. The figure displays a trend with λ R such that smaller values are found in more massive galaxies.…”
Section: Core and Cusp Galaxies In The Sauron Samplementioning
Summary. In this proceeding we look at the relationship between the photometric nuclear properties of early-type galaxies from Hubble Space Telescope imaging and their overall kinematics as observed with the SAURON integral-field spectrograph. We compare the inner slope of their photometric profiles and the Slow/Fast rotator classes, defined by the amplitude of a newly defined λR parameter, to show that slow rotators tend to be more massive systems and display shallower inner profiles and fast rotators steper ones. It is important to remark, however, that there is not a one-to-one relationship between the two photometric and kinematic groups.
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