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Rebecca A. W. Elson

Publications and source records attributed to Rebecca A. W. Elson.

9 recordsLinked to original sources
arXiv2001

The Metal-rich Globular Cluster NGC6553: Observations with WFPC2, STIS, and NICMOS

We present a HST study of the metal-rich globular cluster NGC6553 using WFPC2, NICMOS and STIS. Our primary motivation is to calibrate the STIS broad-band LP magnitude against $V_{555}$ and $I_{814}$ magnitudes for stars of known metallicity and absolute (visual) magnitude, for application to our study of LMC globular clusters. NGC6553 has been shown in earlier studies to have a very unusual colour-magnitude diagram, so we also use our data to investigate the reddening, distance, luminosity function and structure of this cluster. We deduce a higher metallicity and smaller distance modulus than did some previous studies, but emphasise that very large patchy extinction on small angular scales prohibits accurate determination of the parameters of this cluster. The horizontal branch of NGC6553 in ($V,V-I$) is tilted at an angle close to that of the reddening vector. We show that extinction does not, however, explain the tilt, which is presumably a metallicity effect. The colour-magnitude diagram shows an apparent second turnoff some 1.5 magnitudes fainter than that of the cluster. We show that this is most likely the background Galactic bulge: however, in that case, the colour-magnitude diagram of NGC6553 is not a good match to that of the field bulge population. The cluster is probably more metal-rich than is the mean field bulge star.

astro-ph↗
arXiv1997

Two serendipitous low-mass LMC clusters discovered with HST

We present V and I photometry of two open clusters in the LMC down to V ~ 26. The clusters were imaged with the Wide Field and Planetary Camera - 2 on board of the Hubble Space Telescope, as part of the Medium Deep Survey Key-Project. Both are low luminosity (Mv ~ -3.5), low mass systems (M ~ 10^3 Msolar). The chance discovery of these two clusters in two parallel WFPC2 fields suggests a significant incompleteness in the LMC cluster census near the bar. One of the clusters is roughly elliptical and compact, with a steep light profile, a central surface brightness Mu_v(0) 20.2 mag/arcsec2, half-light radius Rhl ~ 0.9 pc (total visual major diameter D ~ 3 pc) and an estimated mass M ~ 1500 Msolar. From the colour-magnitude diagram and isochrone fits we estimate its age as t ~ 2-5 10^8 years. Its mass function has a fitted slope of Gamma = Δlog ϕ(M) / Δlog M = -1.8 +/- 0.7 in the range probed (0.9 < M/Msolar < 4.5). The other cluster is more irregular and sparser, having shallower density and surface brightness profiles. We obtain Gamma = -1.2 +/- 0.4, and estimate its mass as M ~ 400 Msolar. A derived upper limit for its age is t < 5 10^8 years. Both clusters have mass functions with slopes similar to that of R136, a massive LMC cluster, for which HST results indicate Gamma ~ -1.2. They also seem to be relaxed in their cores and well contained in their tidal radii.

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arXiv1997

HST Imaging of the Globular Clusters in the Fornax Cluster: NGC 1379

We present B and I photometry for ~300 globular cluster candidates in NGC 1379, an E0 galaxy in the Fornax Cluster. Our data are from both Hubble Space Telescope (HST) and ground-based observations. The HST photometry (B only) is essentially complete and free of foreground/background contamination to ~2 mag fainter than the peak of the globular cluster luminosity function. Fitting a Gaussian to the luminosity function we find =24.95+-0.30 and σ_B = 1.55+-0.21. We estimate the total number of globular clusters to be 436+- 30. To a radius of 70 arcsec we derive a moderate specific frequency, S_N=3.5 +- 0.4. At radii r~ 3-6 kpc the surface density profile of the globular cluster system is indistinguishable from that of the underlying galaxy light. At r \ltsim 2.5 kpc the profile of the globular cluster system flattens, and at r \ltsim 1 kpc, the number density appears to decrease. The (B-I) colour distribution of the globular clusters (from ground-based data) is similar to that for Milky Way globulars, once corrected for background contamination. It shows no evidence for bimodality or for the presence of a population with [Fe/H]\gtsim -0.5. Unlike in the case of larger, centrally located cluster ellipticals, neither mergers nor a multiphase collapse are required to explain the formation of the NGC 1379 globular cluster system. We stress the importance of correcting for background contamination: the colour distribution of background galaxies is strongly peaked slightly bluer than the peak of a typical globular cluster distribution. This can create the impression of skewed colour distributions, or bimodality where none exists.

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arXiv1997

HST Observations of the Field Star Population in the Large Magellanic Cloud

We present $V$ and $I$ photometry, obtained with the Hubble Space Telescope, for $\sim 15,800$ stars in a field in the inner disk of the Large Magellanic Cloud. We confirm previous results indicating that an intense star formation event, probably corresponding to the formation of the LMC disk, occurred a few times $10^9$ years ago. We find a small but real difference between our field and one further out in the disk observed by Gallagher et al (1996): either star formation in the inner disk commenced slightly earlier, or the stars are slightly more metal rich. We also find evidence for a later burst, around 1 Gyr ago, which may correspond to the formation of the LMC bar. About 5% of the stars in our field are substantially older than either burst, and are probably members of an old disk or halo population with age $\sim 12$ Gyr.

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arXiv1996

Red Giants in the Halo of the S0 Galaxy NGC 3115: A Distance and a Bimodal Metallicity Distribution

Using the Hubble Space Telescope, we resolve the red giant branch in the halo of the S0 galaxy NGC 3115. We measure magnitudes and $(V-I)$ colours for stars down to 1.5 magnitudes below the tip of the red giant branch. From the brightest stars we estimate a distance modulus $(m-M)_0=30.21 \pm 0.30$, corresponding to a distance of $11.0 \pm 1.5$ Mpc. This is in excellent agreement with the value $(m-M)_0=30.17 \pm 0.13$ determined from the planetary nebula luminosity function. Our results rule out the shorter distance modulus $(m-M)_0=29.65$ determined from surface brightness fluctuations. A histogram of $(V-I)$ colours shows a clear bimodality, indicating the presence of two distinct halo populations of roughly equal size. One has [Fe/H]$\sim -0.7$ and one has [Fe/H]$\sim -1.3$. This is the most distant galaxy in which a Population II halo has been resolved, and it is the first time a colour bimodality has been observed among the halo stars of any early-type galaxy.

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arXiv1996

HST Photometry of 47 Tuc and Analysis of the Stellar Luminosity Function in Milky-Way Clusters

We present V and I photometry for a field 5' from the center of 47 Tuc. The field was imaged with the HST WFPC2 as part of the Medium Deep Survey project. The luminosity function (LF) continually rises in the domain $5 < M_I < 9$ with a slope $Δlog Φ(M) / ΔM \sim 0.15$ and then drops off sharply. We compare our LF with that derived by De Marchi \& Paresce for a neighbouring HST field. The two independent LFs are very similar in the entire range of luminosities probed ($M_I < 10$). Comparisons are also made to other HST LFs derived by several authors for different clusters in the Galaxy. We use the KS test to assess the significance of the differences found. The LFs obtained with HST are consistent with being derived from the same population down to $M_I \sim 9.0$. Beyond that, statistically significant variations arise. Globular cluster LFs also differ according to the prominence of a plateau in the bright end ($5 < M_I < 6.5$). Mass functions are sensitive to the mass-luminosity relation. Different approaches to deriving the 47 Tuc mass function from its LF lead to markedly different results at the low mass end. For $M > 0.4 M_\odot$, the 47 Tuc mass function is significantly different from that of \wcen. The calibrated HST $M_V(V-I)$ colour-magnitude diagrams (CMDs) show a trend with metallicity in the sense of metal richer systems having redder CMDs for a fixed absolute magnitude. The main-sequence becomes shallower with increasing metallicity. For metal-rich systems, the CMDs derived from HST are in general agreement with previous ground-based studies. However, the CMDs of metal poor subdwarfs observed from the ground are shallower than those of globular clusters observed with HST.

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arXiv1995

The Globular Clusters in M87: A Bimodal Colour Distribution

We present $V$ and $I$ photometry for $\sim 150$ globular clusters with $20 < V < 27$ $\sim 2.5$ arcmin from the centre of M87, the cD galaxy in the Virgo cluster. The data were acquired with the Hubble Space Telescope which, with effective resolution 0.1 arcsec, allows us for the first time to distinguish between globular clusters and most background galaxies on the basis of morphology, and to obtain accurate photometry even at faint magnitudes. The $(V-I)$ distribution of the clusters is clearly bimodal, implying a corresponding bimodality in the metallicity distribution, with peaks at [Fe/H]$\approx -1.5$ and $-0.5$. We also find that the brightest clusters are predominantly metal poor, while the fainter clusters are divided roughly eaually between metal poor and metal rich. Our sample is essentially complete to $ V\approx 25$, a full magnitude past the expected peak of a ``universal" luminosity function, and the observed luminosity function is well represented by the standard gaussian distribution with $ =-7.2$ and $σ= 1.4$.

astro-ph↗
arXiv1995

HST Star Counts at High Galactic Latitudes

We use star counts from 13 deep HST fields imaged with the {\it Wide Field Camera - 2} in order to constrain the amount of dark matter in the Galaxy that can be in the form of low-mass main sequence stars or white-dwarfs. Based on the number of red stars found in our fields, we exclude the possibility that more than 25\% of the massive dark halo is made up of M dwarfs or subdwarfs; fairly massive ($M \sim 0.2 M_\odot$) and yet extremely faint ($M_I$ \gtsima $14.5$) stellar candidates would have to be invoked in order to make the observed number of stars compatible with that predicted by a stellar dark halo. White dwarfs must also be intrinsically very faint ($M_I$ \gtsima $14$) in order to be consistent with the observed number of faint stars in the HST fields. We also rule out an increasing or flat stellar luminosity function beyond $M_V \sim 13$. The inferred slope of the disk luminosity function is intermediary between local, volume-limited surveys and ground-based photometric ones. Finally, the magnitude counts are well fitted by existing models for the structure of the Galaxy, with only small changes in the fiducial values of the model parameters. The colour distribution, however, is not well reproduced by the models. It is unclear at present if this reflects inadequacies of the available models or uncertainties in the colour-magnitude diagrams for low metallicity stars and in the photometric calibration.

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