S. P. Ewald

Planetary Camera observations of NGC 1275 - Discovery of a central population of compact massive blue star clusters

We have discovered a population of bright blue pointlike sources within 5 kpc of the nucleus of NGC 1275 using HST Planetary Camera observations. The typical object has M_v~- 12 to - 14 (H_0 = 75 km s^(-1) Mpc^(-1); the brightest has M_v~-16. They are all blue, with V- R≾0.3. The color distribution and lack of excess Ha emission are consistent with nearly all being continuum sources. Many of the sources are unresolved even with the HST and consequently have sizes of ≾ 15 pc. We suggest that these are young star clusters that will evolve to look like globular clusters. They are bluer than any clusters seen in the Milky Way or M87, and brighter than the blue clusters seen in the LMC. We derive ages of several hundred million years or less and corresponding masses of 10^5-10^8 M_☉. The existence of these young clusters may be connected with a current or previous interaction with another galaxy, with the cooling flow in NGC 1275, or with some combination. Structure is detected in the underlying galaxy light that is suggestive of a merge between NGC 1275 and a second galaxy some 10^8 yr ago. If this merger triggered star formation, it would naturally account for the observed uniformity of cluster colors. Steady-state star formation in the x-ray cooling flow would imply a wider range in cluster age and color than is seen, unless the clusters disrupt. An interaction with the projected high-velocity, infalling system cannot explain the observations because this system has not yet reached the center of NGC 1275 where the clusters are concentrated, and because it has a total interaction time that is far too short for either the observed cluster lifetimes or the dynamical lifetime of structure in the galaxy. If the presence of recently formed protoglobulars around NGC 1275 is related to a previous merger, this would remove an important objection to the merger hypothesis for elliptical galaxy origins, provided that adequate gas is available in the merger for their formation.

Imaging of the gravitational lens system PG 1115+080 with the Hubble Space Telescope

This paper is the first of a series presenting observations of gravitational lenses and lens candidates, taken with the Wide Field/Planetary Camera (WFPC) of the Hubble Space Telescope (HST). We have resolved the gravitational lens system PG 1115 + 080 into four point sources and a red, extended object that is presumably the lens galaxy; we present accurate relative intensities, colors, and positions of the four images, and lower accuracy intensity and position of the lens galaxy, all at the epoch 1991.2. Comparison with earlier data shows no compelling evidence for relative intensity variations between the QSO components having so far been observed. The new data agree with earlier conclusions that the system is rather simple, and can be produced by the single observed galaxy. The absence of asymmetry in the HST images implies that the emitting region of the quasar itself has an angular radius smaller than about 10 milliarcsec (100 pc for H_0=50, q_0=0.5).

High-Mass, OB Star Formation in M51: [ITAL]HUBBLE SPACE TELESCOPE[/ITAL][ITAL]Hubble Space Telescope[/ITAL] Hα and P[CLC]a[/CLC]α Imaging

(first paragraph) We have obtained Halpha and Palpha emission line images covering the central 3 - 4 arcmin of M51 using the WFPC2 and NICMOS cameras on HST to study the high-mass stellar population. The 0.1 - 0.2 arcsec pixels provide 4.6 - 9 pc resolution in M51 and the Halpha/Palpha line ratios are used to obtain extinction estimates. A sample of 1373 Halpha emission regions is catalogued using an automated and uniform measurement algorithm. Their sizes are typically 10 - 100 pc. The luminosity function for the Halpha emission regions is obtained over the range L_{Halpha} = 10^{36} to 2 times 10^{39} erg s{-1}. The luminosity function is fit well by a power law with dN/dlnL proportional to L^{-1.01}). The power law is significantly truncated and no regions were found with observed L_{Halpha} above 2 times 10^{39} erg s^{-1} (uncorrected for extinction; the maximum seen in ground-based studies is approximately a factor of 5 higher, very likely due to blending of multiple regions). The extinctions derived here increase the maximum intrinsic luminosity to above 10^{40} erg s^{-1}). The logarithmically binned luminosity function is also somewhat steeper (alpha = -1.01) than that found ground-based imaging (alpha = -0.5 to -0.8) - probably also a result of our resolving regions which were blended in the ground-based images. The 2-point correlation function for the HII regions exhibits strong clustering on scales <= 2 arcsec or 96 pc.

Stellar photometry with the Hubble Space Telescope Wide-Field/Planetary Camera: a progress report

We describe the prospects for the use of the Wide-Field/Planetary Camera (WFPC) for stellar photometry. The large halos of the point-spread function (PSF) resulting from spherical aberration and from spatial, temporal, and color variations of the PSF are the main limitations to accurate photometry. Degradations caused by crowding are exacerbated by the halos of the PSF. Here we attempt to quantify these effects and determine the current accuracy of stellar photometry with the WFPC. In realistic cases, the brighter stars in crowded fields have 0.09 mag errors; fainter stars have larger errors depending on the degree of crowding. We find that measuring Cepheids in Virgo Cluster galaxies is not currently possible without inordinate increases in exposure times.

High-Mass, OB Star Formation in M51: Hubble Space Telescope Hα and Paα Imaging

(first paragraph) We have obtained Halpha and Palpha emission line images covering the central 3 - 4 arcmin of M51 using the WFPC2 and NICMOS cameras on HST to study the high-mass stellar population. The 0.1 - 0.2 arcsec pixels provide 4.6 - 9 pc resolution in M51 and the Halpha/Palpha line ratios are used to obtain extinction estimates. A sample of 1373 Halpha emission regions is catalogued using an automated and uniform measurement algorithm. Their sizes are typically 10 - 100 pc. The luminosity function for the Halpha emission regions is obtained over the range L_{Halpha} = 10^{36} to 2 times 10^{39} erg s{-1}. The luminosity function is fit well by a power law with dN/dlnL proportional to L^{-1.01}). The power law is significantly truncated and no regions were found with observed L_{Halpha} above 2 times 10^{39} erg s^{-1} (uncorrected for extinction; the maximum seen in ground-based studies is approximately a factor of 5 higher, very likely due to blending of multiple regions). The extinctions derived here increase the maximum intrinsic luminosity to above 10^{40} erg s^{-1}). The logarithmically binned luminosity function is also somewhat steeper (alpha = -1.01) than that found ground-based imaging (alpha = -0.5 to -0.8) - probably also a result of our resolving regions which were blended in the ground-based images. The 2-point correlation function for the HII regions exhibits strong clustering on scales <= 2 arcsec or 96 pc.

High mass, ob star formation in m51 : hst halpha and palpha imaging

(first paragraph) We have obtained Halpha and Palpha emission line images covering the central 3 - 4 arcmin of M51 using the WFPC2 and NICMOS cameras on HST to study the high-mass stellar population. The 0.1 - 0.2 arcsec pixels provide 4.6 - 9 pc resolution in M51 and the Halpha/Palpha line ratios are used to obtain extinction estimates. A sample of 1373 Halpha emission regions is catalogued using an automated and uniform measurement algorithm. Their sizes are typically 10 - 100 pc. The luminosity function for the Halpha emission regions is obtained over the range L_{Halpha} = 10^{36} to 2 times 10^{39} erg s{-1}. The luminosity function is fit well by a power law with dN/dlnL proportional to L^{-1.01}). The power law is significantly truncated and no regions were found with observed L_{Halpha} above 2 times 10^{39} erg s^{-1} (uncorrected for extinction; the maximum seen in ground-based studies is approximately a factor of 5 higher, very likely due to blending of multiple regions). The extinctions derived here increase the maximum intrinsic luminosity to above 10^{40} erg s^{-1}). The logarithmically binned luminosity function is also somewhat steeper (alpha = -1.01) than that found ground-based imaging (alpha = -0.5 to -0.8) - probably also a result of our resolving regions which were blended in the ground-based images. The 2-point correlation function for the HII regions exhibits strong clustering on scales <= 2 arcsec or 96 pc.