Title: A Survey of Local Group Galaxies Currently Forming Stars
1A Survey of Local Group GalaxiesCurrently
Forming Stars
Phil Massey Lowell Observatory April 14, 2003
2The Team
- Paul Hodge, Univ. of Washington
- Shadrian Holmes, Univ. of Texas
- George Jacoby, WIYN
- Nichole King, Lowell Observatory
- Phil Massey (PI), Lowell Observatory
- Knut Olsen, CTIO/NOAO
- Abi Saha, KPNO/NOAO
- Chris Smith, CTIO/NOAO
3Overview
- We are imaging all of the galaxies of the Local
Group that are currently forming stars - broad-band (UBVRI)
- narrow-band (H?, OIII, SII)
- with the KPNO and CTIO 4-m telescopes and
Mosaic CCD cameras.
4Motivation Our Science
- The galaxies of the Local Group serve as our
laboratories for studying star formation and
stellar evolution as a function of metallicity,
Z. (Z varies by a factor of 17 from WLM to M31.)
5Why should the metallicity matter?
- Star Formation
- Lower metallicity gas should have a lower cooling
rate, and hence higher temperatures ?larger
Jeans mass, leading to a top-heavy IMF (Larson
1998). - But over the limited metallicity range (3x)
SMC?LMC?MW this effect isnt seen!
6IMF Slope in OB Associations
Z0.018
Z0.008
Z0.004
7IMF
- Variations that are seen in the IMF slope are
statistical, not physical (Massey 1998, Kroupa
2001) - But what would happen if we extended this to
- one-tenth solar (WLM) to 2x solar (M31)???
- The answer is important for understanding the
integrated properties of galaxies at large
look-back times.
8Star Formation/metallicity (cont)
- Some expect that the upper mass limit will vary
as a function of metallicity - True only if radiation pressure acting on grains
is the limiting factor in determining the mass of
the highest mass star that can form. - So far we find that the upper mass limits are
purely statistical, and not physical. What ever
it is that limits the ultimate mass of a star we
have yet to encounter it in nature (cf. Massey
Hunter 1998 ApJ 493, 180).
9Why should the metallicity matter ? (continued)
- Massive Star Atmospheres and Evolution
- Stellar winds are driven by radiation pressure
through highly ionized metal lines. Mass-loss
rates will depend upon Z?, where ? ? 0.5-1.0 - This mass-loss has a profound effect on the
evolution of high-mass stars.
10Relative number of red supergiants (RSGs) and
Wolf-Rayet stars (W-Rs)
log Number RSGs/WRs
From Massey 2003, ARAA 41 (in press)
log (O/H) 12
11Relative number of red supergiants (RSGs) and
Wolf-Rayet stars (W-Rs)
log Number RSGs/WRs
From Massey 2003, ARAA 41 (in press)
log (O/H) 12
12Need good observational database
- New generation of high mass evolutionary models
are becoming available, which include the
important effects of rotation (mixing introduced
by meridional circulation and shear
instabilities). - Need solid observational database to help guide
the theorists.
13Our Science (continued)
Along the way well find The most massive
supergiants. Luminous Blue Variables and other
luminous stars with H? emission. Star formation
rates for massive stars. Distribution and
numbers of evolved massive stars (RSGs, WRs).
HII regions, SNRs, PNe, and the extent of the
diffuse emission.
14Your Science
- This survey will provide the source list
(finding charts) for spectroscopy with 8-10-m
telescopes for decades to come. Our data
products include - Stacked images (UBVRI, H?, OIII, SII)
- Individual dithered images (suitable for
photometry). - Calibration
- Catalog of UBVRI photometry of roughly 300
million stars
15What Were Doing The Sample
- M31 (10 fields) Pegasus Dwarf
- M33 (3 fields) Phoenix
- IC 10 IC 1613
- NGC 6822 Sextans A
- WLM Sextans B
16How Are We Doing?
- ?M31 (10 fields) ? Pegasus Dwarf
- ?M33 (3 fields) ? Phoenix
- ? IC 10 ? IC 1613
- ? NGC 6822 ? Sextans A
- ? WLM ? Sextans B
17What Were Doing (continued)
- Aiming for a S/N of 3 at UBVRI25,
- in 1 seeing.
- Also imaging in H?, OIII, SII
- Each field 5 ditherings, then stacked.
18Hasnt All This Been Done Before?
- Yes, but not with our depth, area, photometric
accuracy and resolution! - Photographic plates had the area coverage and
(usually) the resolution, but neither the
photometric accuracy nor depth. - CCD studies had the depth and accuracy but not
always the resolution and certainly not the area
coverage. - Wal Sargent story...
19Comparison of M31 CCD Surveys
20Basic Processing
- Generally following the Valdes IRAF pipeline
but with some enhancements. - Better flat-fielding techniques.
- Better determination of sky and scaling in the
stacking process (via scripts using aperture
photometry). - Details, and software, can be found at our web
site http//www.lowell.edu/massey/lgsurvey
21Photometry
- For the purposes of photometry, we treat each
- Mosaic camera as 8 separate instruments
- PSF variations within a single chip modest
compared to chip-to-chip variations. - Different DQE-wavelength dependence for each chip
means different color terms and even different
zero-points (despite flat-fielding efforts).
22U flat divided by I flat
Variations ?30
23Photometry software
- Its a factor of 40 times more work (8 chips x 5
ditherings) but at least when were done we have
1 photometry. - Weve developed a series of IRAF scripts and
FORTRAN programs that allow us to do the
photometry automatically, chip-by-chip,
dither-by-dither. - All of this is freely available from our web
site - http//www.lowell.edu/massey/lgsurvey
24How weve solved the calibration problem
Lowells dark-sky site at Anderson Mesa
25External Calibration using Lowell s 1.2-m Hall
Telescope
- Can use only the most pristine, photometric
nights. - Select the best calibrated Landolt standards
covering a complete range of colors - Investigate gravity effects on the U-band filter
26U solution always squirrelly near U-B0.
U-B
27Its a matter of some gravity....
28Progress Report---How are We Doing?
- All images for M31 (10 fields), M33 (3 fields),
NGC 6822, IC10, WLM, Phoenix, Sextans A, and
Sextans B are now released, and sitting in the
NOAO NSA archive, as well as our own dedicated
ftp site (which makes bulk downloads easier). - Poor weather in early September prevented us from
completing the project still need IC1613 and the
Pegasus dwarf, plus repeat of poor seeing frames. - Calibration in progress and catalog should be
complete on schedule, release Jan 2004.
29Did We Achieve our 1.0 seeing goal?
30(No Transcript)
311.3
320.76
331.3
340.76
35Poor seeing matters!
- To redo the images with seeing gt 1.3 would
require only a few additional nights.
36Sadly...
- Weve been told that our time has run out, and we
arent eligible for additional time via the
survey TAC. - So, weve made our best case to the standard TAC
and well see what happens. - (Wal Sargent Cautionary Tale)
37M31 in 10 fields
38M31 in 10 fields
39M31 Fields 2 3
40M33-North
41M33-Center
42NGC 6822
43Phoenix
44WLM
45Whats Next?
46M31
47N206 in M31
ob78-231
48HST/ FUV ob78-231
- Bianchi, Hutchings, Massey (1996, AJ, 111, 2303)
49To take high S/N optical spectra at B19 requires
a really big telescope...
The 6.5-m MMT
50Optical (blue) spectrum ob78-231
Spectrum in collaboration with Kathy Eastwood
51OB78-231 at H?
Spectrum in collaboration with Kathy Eastwood
52Meanwhile, these data are already being used...
- Ben Williams PhD thesis (Univ Washington)
- Williams MNRAS 340, 143 based up a bootstrap
calibration. - Forms optical basis for identifying super-soft
Chandra counterparts (DiStefano et al., in prep) - Images have been featured in
- APOD 27 Sept 2001
- Astronomy Magazine (Sky Gem feature), Dec 02
- Upcoming Mercury article on super star clusters
(Hunter, Elmegreen, Massey 2003, in press)
53Real Science
- ...will come once the calibrated photometry is
complete this summer. (Catalog will be released
at the AAS meeting in Jan 2004).
54Follow-up Work In Progress
- Well be pushing our studies of stellar winds to
high metallicities (M31) using Cycle 12 time on
HST (40 orbits 80 parallels just awarded) - We also hope to begin extending our studies of
the IMF to the more distant galaxies of the Local
Group using DEIMOS on KeckII.