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V. Charmandaris

Publications and source records attributed to V. Charmandaris.

208 records · Page 12Linked to original sources

HST observations of the very young SMC ``blob'' N88A

High-resolution Hubble Space Telescope images have allowed us for the first time to resolve the compact SMC ionized ``blob'' N88A (diameter 3.5 arcsec or 1 pc). This very young HII region, which is hatching from its natal molecular cloud, is heavily affected by absorbing dust associated with the cloud. The interstellar reddening towards N88A is on average Av~1.5 mag and strikingly rises to more than 3.5 mag in a narrow dust band crossing the core of the HII region. Such a high extinction is unprecedented for an HII region in the metal-poor SMC. We present the photometry of some 70 stars lying towards the OB association at the center of which lies N88A. The exciting star(s) of N88A is not detected, due to the heavy extinction. The chronology of star formation is discussed for the whole region.

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Very young massive stars in the Small Magellanic Cloud, revealed by HST

High spatial resolution imaging with the Hubble Space Telescope allowed us to resolve the compact HII, region N81 lying in the Small Magellanic Cloud (SMC). We show the presence of a tight cluster of newborn massive stars embedded in this nebular ``blob'' of about 10 arcsecs, across. This is the first time the stellar content and internal morphology of such an object is uncovered. These are among the youngest massive stars in this galaxy accessible to direct observations at ultraviolet and optical wavelengths. Six of them are grouped in the core region of about 2 arcsecs diameter, with a pair of the main exciting stars in the very center separated by only 0.27 arcsecs or 0.08 pc. The images display violent phenomena such as stellar winds, shocks, ionization fronts, typical of turbulent starburst regions. Since the SMC is the most metal-poor galaxy observable with very high angular resolution, these observations provide important templates for studying star formation in the very distant metal-poor galaxies which populate the early Universe.

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The Gas Dynamics of Shell Galaxies

It is widely accepted that shell galaxies form as a result of a merger between an elliptical and a small disk galaxy. Simulations of the stellar component have shown that the shells are created either by ``phase-wrapping'' of debris on nearly radial orbits (Quinn 1984), or by ``spatial-wrapping'' of matter in thin disks (Dupraz & Combes 1987; Hernquist & Quinn 1989; Quillen etal 1993). However, recent HI observations of several shell galaxies (Schiminovich etal 1994, 1995) revealed the presence of gaseous shells displaced from the stellar ones, which questioned the validity of the ``phase-wrapping'' mechanism. Our numerical simulations indicate that these new observations can actually be accommodated within the standard picture for the formation of shell galaxies.

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Molecular Gas in The Cartwheel Galaxy

We present the first detection of molecular gas in the Cartwheel, the prototype of a collisional ring galaxy formed in the head-on encounter of two galaxies. Until now, only very little atomic gas and no CO had been detected in the centre, where gas is theoretically expected to pile up. Using the Swedish ESO Submm Telescope, we detected both 12CO(1-0) and (2-1) line emission towards the central position. The line ratio and the line widths suggest that the CO(2--1) emission is sub-thermal and that the CO(1-0) emission arises within the central 22'' (13 kpc); it is probably associated with the inner ring and nucleus. We infer a mass of molecular gas (H2) of 1.5 to 6 10^9 M_sol, which is significantly higher than the approx. 10^8 M_sol of atomic gas within that region. The low excitation of the gas, whether it is due to a low temperature or a low density, is consistent with the weak star-forming activity observed in the centre of the Cartwheel.

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A barred spiral at the centre of the giant elliptical radio galaxy Centaurus A

We report observations at mid-infrared and sub-millimeter wavelengths of Centaurus A (CenA, NGC 5128), the giant elliptical galaxy that harbors the closest radio loud Active Galactic Nucleus (AGN) to Earth. The dust emission from the deep interior of CenA reveals a bisymmetric structure with a diameter of 5' (5 kpc), centred at the AGN. This structure is remarkably similar to that of a barred spiral galaxy, with the bar lying in a plane that is tilted ~18 degrees from the line of sight. The true nature of the distribution of dust in the inner regions of CenA is noticeably displaced from the more chaotic and widespread optical obscuration. The barred spiral is a quasi-stable structure formed at the center of the giant elliptical from the tidal debris of a gas-rich object(s) accreted in the past 10^9 years. The total size and mass of interstellar gas in the barred spiral at the center of CenA is comparable to the small Local Group spiral galaxy Messier 33. The observation of this remarkable structure opens the more general question on whether the dusty hosts of giant radio galaxies like CenA, are "symbiotic" galaxies composed of a barred spiral inside an elliptical, where the bar serves to funnel gas toward the AGN.

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Dust in the Wheel: The Cartwheel Galaxy in the Mid-IR

We present mid-infrared images at $6.7 μm$ and $15 μm$ of ``The Cartwheel'' (AM~0035-33), the prototypical collisional ring galaxy. The observations, taken with ISOCAM, reveal the distribution of hot dust in the galaxy and its two companions in the north-east. The intensity of the mid-IR emission from the outer star forming ring of the Cartwheel shows considerable azimuthal variation and peaks at the most active H$α$ region of the ring. The 15 $μm$ to 6.7 $μm$ flux ratio of 5.2 is the highest among all the galaxies of our sample. A surprising result of our observations is the discovery of significant emission from the inner regions of the galaxy, including the inner ring, spokes and nucleus, where previously only low level H$α$ emission had been reported. At 6.7 $μm$, this emission is stronger than the one from the outer star forming ring, and at 15 $μm$, it represents 40% of the emission from the outer ring. The H$α$ to mid-IR flux ratios from the inner regions are consistent with the heating of grains from weak star formation activity.

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The dark side of star formation in the Antennae galaxies

We compare mid-infrared images of the Antennae galaxies (NGC 4038/39) from the Infrared Space Observatory, with optical images from the Hubble Space Telescope. The mid-infrared observations show that the most intense starburst in this colliding system of galaxies takes place in an off-nucleus reg ion that is inconspicuous at optical wavelengths. The analyses of the mid-infrar ed spectra indicate that the most massive stars are being formed in an optically obscured knot of 50 pc radius, which produces about 15% of the total luminosity from the Antennae galaxies between 12.5 microns and 18 microns. The mid-infrared observations reported here demonstrate that the interpretation of star formation properties in colliding/merging systems based on visible wavelengths alone can be profoundly biased due to dust obscuration. The multiwavelength view of this nearby prototype merging system suggests caution in deriving scenarios of early evolution of high redshift galaxies using only observations in the narrow rest-frame ultraviolet wavelength range.

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The Head-on Collision between Two Gas-Rich Galaxies: Neutral Hydrogen Debris from the Centrally-smooth Ring Galaxy VIIZw466

We present VLA observations of the distribution and kinematics of the HI gas in the classical ring galaxy VIIZw466 and its immediate surroundings. The HI gas corresponding to the bright optical star forming ring exhibits the typical profile of a rotating-expanding ring. The systemic velocity of the galaxy is found to be 14,468km/s. A formal fit to the HI kinematics in the ring is consistent with both ring rotation and expansion (expansion velocity 32 km/s). However, H\,I in the northeast quadrant of the ring is severely disturbed, showing evidence of tidal interaction. We also detect a hydrogen plume from the southern edge-on companion galaxy (G2) pointing towards the ring galaxy. This, and other peculiarities associated with G2 suggest that it is the intruder galaxy which recently collided with VIIZw466 and formed the ring. Numerical hydrodynamic models are presented which show that most of the observed features can be accounted for as a result of the impact splash between two gas disks. The resultant debris is stretched by ring wave motion in the bridge and later forms accretion streams onto the two galaxies.Finally, we detect HI emission from two previously unknown dwarf galaxies located northeast and southeast of VIIZw466 respectively. This brings the total number of members of the VIIZw466 group to five. Using the projected mass method, the upper limit of the dynamical mass of the group was estimated to be Mo =3.5x10^{12} M_sun, which implies that the mass to light ratio of the group is (M/L)_{group} \approx$ 70. This rather low value of M/L, as compared with other loose groups, suggests the group may be in a state of collapse at the present time. Plunging orbits would naturally lead to an enhanced probability of head-on collisions and ring galaxy formation.

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The Neutral Hydrogen Disk of Arp 10 (=VV 362) : A Non-equilibrium Disk Associated with a Galaxy with Rings and Ripples

We present VLA \ion{H}{1} and optical spectra of the peculiar galaxy Arp~10. Originally believed to be an example of a classical colliding ring galaxy with multiple rings, the new observations show a large disturbed neutral hydrogen disk extending 2.7 times the radius of the bright optical ring. We also present evidence for optical shells or ripples in the outer isophotes of the galaxy reminiscent of the ripples seen in some early type systems. The small elliptical originally believed to be the companion is shown to be a background galaxy. The \ion{H}{1} disk consists of two main parts: a very irregular outer structure, and a more regular inner disk associated with the main bright optical ring. In both cases, the \ion{H}{1} structures do not exactly trace the optical morphology. In the outer parts, the \ion{H}{1} distribution does not correlate well with the optical ripples. Even the inner \ion{H}{1} disk does not correspond well morphologically nor kinematically to the optical rings. These peculiarities lead us to believe that the potential in which the \ion{H}{1} disk resides is significantly out of equilibrium --- a situation which would inherently produce rings of star formation. We suggest that Arp~10 is the result of the intermediate stage of a merger between a large \ion{H}{1} rich disk and a gas-poor disk system. As such, it may represent an example of a class of mergers which lies intermediate between the ``ripple and shell'' accretion systems and the head-on collisional ring galaxies.

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Threshold Star Formation Effects in the Peculiar Galaxy Arp~10 (=~VV 362)

We present images of the peculiar galaxy Arp~10 which reveal two rings of concurrent star formation. Apart from a bright ring visible on early photographs of the system, an even brighter inner ring of \ion{H}{2} regions is found within the nuclear bulge of the galaxy. A very faint ring-arc of \ion{H}{2} regions is also seen associated with a third outer ring or shell. An investigation of the H$α$ fluxes in the rings reveals an increase in the emission where the ring surface density in the R-band light exceeds 21.3$\pm$0.2 mag arcsec$^{-2}$. If the R-band light is dominated by old stars in the underlying density wave, then the results suggest evidence for a Star Formation law which exhibits a threshold dependence on the strength of the density wave in the rings. Even if the R-band continuum in the ring is heavily contaminated with red light from the underlying young stars then a smaller, but still significant non-linear enhancement in the star formation rates (SFR) in one segment of the second ring is required to explain the results. In either case, strong trends in the SFR with azimuth around Ring~2 are in good agreement with off-center collisional ring galaxy models.

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