Academic Programs Astronomy Macalester College

Astrophysics of the Local Group
Topics Course, Spring 2002

Lecture Series sponsored by the National Science Foundation through CAREER Grant AST-9984073 awarded to Prof. Kim Venn.
Presented in collaboration with Prof. Evan Skillman and the Department of Astronomy, University of Minnesota.

Webpage developed by Chrissy Blank (Macalester Physics/Astronomy '03)


Visiting Lecturers:
Professor Sidney van den BerghJanuary 31, 2002Dark Matter in the Local Group
Professor Lisa YoungFebruary 7, 2002Gas in Dwarf Spheroidal (dSph) Galaxies
Dr. Chris StubbsFebruary 28, 2002MACHO (MAssive Compact Halo Objects) Surveys
Dr. Abi SahaMarch 7, 2002 Hubble's Constant From Type Ia Supernovae
Dr. Stephen SmarttMarch 14, 2002Supernovae Progenitors & Massive Stars
Dr. Eline TolstoyApril 4, 2002Global Star Formation History
Professor Liliya WilliamsApril 9, 2002Hubble's Constant from Gravitational Lensing
Dr. Matthew ShetroneApril 18, 2002Chemical Evolution of dSph Galaxies
Dr. Taft ArmandroffApril 25, 2002Survey for Dwarf Galaxies
Professor Mario MateoMay 2, 2002The Past, Present & Future of the Local Group



Sidney van den Bergh Dark Matter in the Local Group

Sidney van den Bergh (at left)
Dominion Astrophysical Observatory (DAO), NRC of Canada, Victoria, British Columbia

*Professor van den Bergh wrote the text used in this course, Galaxies of the Local Group (1999, Cambridge University Press), so it was appropriate that he was the first speaker to visit the class.

Balance Sheet for Galactic Matter:

1900: 100% stars

2000: 1% stars and cold gas, 3% hot gas, about 30% cold dark matter and 66% dark energy (we lost 97% of what we thought we knew in 100 years!)

Who "saw" it first? Fritz Zwicky

Zwicky, 1933 (at right; in his most famous pose): first paper mentioning dark matter:
Looked at 8 Coma galaxies. Assuming visual equilbrium, calculated mass-to-light ratio and determined that about 90% of the mass necessary to account for observed ratio was missing and therefore invisible, or "dark".

"The discrepancy appears to be real and important." --Edwin Hubble, 1936

Gerard deValcouleurs The dissenters:

deVaucouleurs, 1960 (at left; second from left): Clusters are expanding like stellar associations, thus the visual theorem is not justified in clusters of galaxies. The picture, taken in 1963, shows the first astronomers to work at the University of Texas. (Incidentally, Professor Venn received her PhD at Texas!)

Yet 75% of all ellptical and 50% of all spiral & irregular galaxies are members of clusters--therefore clusters are not all that unstable after all!!

Rotation Curve for the Milky Way Galaxy More Evidence:

Oort, 1940: Mass-to-light ratio also shows 90% of local group mass is "missing." This discovery was independent of the discovery of missing mass in clusters; Oort didn't cite Zwicky's original 1933 paper.

Rubin & Ford, 1970; Roberts & White..., 1975: radial velocity curve plots radius vs. velocity and flattens out rather than trailing down. This implies that mass continues to increase with radius. At right, see a plot of the radial velocity versus distance for the Milky Way Galaxy. The Keplerian Motion line shows the predicted drop-off for the curve; while the red line is the plot of actual data. Plots of many other galaxies have shown the same trend to a flat, rather than Keplerian curve.

"Cold Dark Matter"

In closing, cold dark matter is not a trivial hypothesis. Cold dark matter could account for up to 30% of the closure density of the universe and is therefore pertinent to study of the past, present and future of the universe.



Lisa Young Gas in Dwarf Spheroidal (dSph) Galaxies

Lisa Young
New Mexico Tech, Socorro, New Mexico Sher25

Is there hydrogen gas in dwarf spheroidal galaxies?

Typically dwarf spheroidals are thought to have formed all of their stars in old and intermediate-aged bursts, and to be devoid of gas today. This is unlike transition galaxies and the gas rich dwarf irregular galaxies.

Some 21 cm detections towards dwarf spheroidals with the correct radial velocities, e.g., Carignan et al. (1998) who find H I associated with the Sculptor dwarf spheroidal galaxy. Young noted that a wider field shows similar H I, suggestive of a high velocity cloud complex. Thus, perhaps Sculptor does not have H I.

The image at right, of Sculptor Dwarf Spheroidal Galaxy (the cluster in the center), shows that extensive high velocity clouds are all around the relgion and perhaps not associated directly with Sculptor.

For more information:






Chris Stubbs MACHO Surveys

Chris Stubbs
University of Washington, Seattle, Washington

See Stubbs, at right, looking through a MACHO telescope.

What is out there?

Dark Matter Candidates:

Ordinary StuffExotic Stuff
Neutrinos? very little rest mass and moving very quicklyWIMPs-Weakly Interacting Massive Particles
Matter? stars-we'd see it as gas or plasmaCritical density universe?
Planets? don't emit or absorb much lightAxions? As-yet undiscovered, hypothetical particle
MACHOs? Jupiter-size planets, tiny black holes, and brown dwarves
Massive neutrinos?

How do we look for these objects? Microlensing!! Microlensing

The diagram at left shows how an object, such as a brown dwarf, when between our eye and a star, will bend the light from said star and bring a distorted image to the eye. This image illustrates what it might look like to an observer to ''see'' a brown dwarf pass through their field of vision. The brown dwarf itself is invisible, but it creates a visible disturbance in the light paths it passes through. For the source of this diagram as well as a number of real images showing gravitational lensing, click here.

Sadly, the objects the MACHO surveys are looking for will not be large enough to resolve into multiple images. There is, however, a noticable increase in brightness, just as would be observed with a classical lens and as can be seen in the central simulation of the image at left.

Results?

The number of observed microlensing events leads to conclusions about the density of dark matter in the Galaxy.

For more information:






Abi in the snow Hubble's Constant From Type Ia Supernovae

Abi Saha
National Optical and Astronomical Observatories (NOAO), Tucson, Arizona

Saha stands in the snow, at left, to show his true Minnesota experience!

How reliable are SNeIa as standard candles?

Establish ABSOLUTE scale by looking at galaxies that we know have SNeIa and use the cepheids in those galaxies to determine the distance and thus calculate absolute magnitudes of supernovae.

Problems involve extinction and the need to use HST to see cepheids due to distance and uncommonness.

Additionally, errors in measurement are magnified and influenced by systematic color errors that change perceived reddening.

Finally, plot calibrated cepheids and supernovae with estimated value for H0. The value that came out for this experiment using SNeIa as standard candles was H0~60 km/s/Mpc, and definitely less than 65.

The Cepheid Key Project, however, suggests values up to H0~72 km/s/Mpc.

The chart below shows the absolute magnitude (MB) of SNeIa (open circles) and of cepheid calibrated SNeIa (filled circles) vs. velocity distance using different values for Hubble's constant. Saha argues that H0 must be less than 60 because if H0 is greater than or equal to 70, distant SNeIa must be, on average, less luminous than nearby calibrators. This is highly unlikely!

Chart of supernovae and cepheids using different values of Hubble's constant.

From Saha, et al. The Astrophysical Journal, 1997 486:1-20.

For more information:



Stephen Smartt, Irish Elvis, Kim Venn, Claire Supernovae Progenitors & Massive Stars

Stephen Smartt
University of Cambridge, Cambridge, United Kingdom

At right, see Smartt, Kim Venn, and Clare Venn Skillman with an Irish Elvis on Saint Patrick's Day.

Supernova 1987A closeup

Close up of supernova 1987A, at left. Courtesy of Hubble Space Telescope.

How do massive stars evolve? Which ones will go supernovae?

Supernovae drive the chemical evolution of gasses because they are the main sites for nucleosynthisis and are responsible for blowing matter out into the universe which can then recombine into new stars. Supernovae are thus associated with gamma-ray bursts as well.

Only 1-2 supernovae occur every 100 years! Therefore it can be rather difficult to find them. Many have actually been seen by accident on slides from other, unrelated observations that just happened to catch the supernova in the corner.

Sher25 can be seen as the bright star with the faint ring around it in the upper left of the image below.

Sher25
Classifying Supernovae:

Supernovae are classified based on the presence of hydrogen gas in the parent galaxy as well as the presence or absence of other elements in the particular progenitor star. Following the table below, the first question is whether there was hydrogen or not. Hydrogen gas implies Type II, and no hydrogen implies Type I. Then within Type I the three types a, b, and c are determined by presence of either silicon, helium, or neither. Type II are classified by other properties determined by photometry.

Hydrogen?No H2 present:H2 present:
General group?Type I supernovaeType II supernovae
Other properties?SiHeneitherPhotometry/spectral properties
Specific type?IaIbIcIIpIInII...

Conclusions:

For more information:

Eline Tolstoy and Clare Global Star Formation History

Eline Tolstoy
Kapteyn Instituut; Groningen, Netherlands

Clare doing Tolstoy's hair, at right.

How far back in history can we see?

The horizon of optical observations is at a redshift of about z=6.

What are the different indicators of star formation rates?

  • Luminosities at 1500 and 2800 angstrom wavelengths of light
  • H alpha and O II absorption lines
  • Far infra-red wavelengths
  • Sub-millimeter wavelengths
  • Radio wavelengths
  • Counting stars...
All of these fall under the heading of ''flux'' where you assume a stare formation rate based on intensities at different wavelengths of light.

The question of global stare formation rates is complicated because we don't know if historical objects look like objects we can recognize from the present or near past.

Star Formation Rate Density vs. Redshift: Looking back in time

A.M. Hopkins did us the service of compiling the star formation densities measured at different redshifts in 13 different papers. As shown in the chart below, the gray area covers to the extremes of uncertainty. Click on the chart to go to the full refereed journal article from The Astrophysical Journal.

Star Formation Rate Density vs. Redshift

For more information:



Hubble's Constant from Gravitational Lensing

Liliya Williams
University of Minnesota, Minneapolis, Minnesota

After the first few talks, particularly those of Stubbs and Saha, it became clear that we needed more background on gravitational lensing and Hubble's constant. Thus we turned to our neighbor, Liliya Williams, at the University of Minnesota, to help us understand Hubble's constant and its relationship to gravitational lensing.

Gravitational Lensing:

Gravitational lensing (see Chris Stubbs' talk on MACHO surveys, above, for other information on gravitational lensing) creates images in only odd numbers. In the image at right, you can see how the light from a single object can be bent around a galaxy and create multiple images. Turns out that what is happening is that the light is following the distortion, or the curve, of spacetime due to the dense region of matter and its associated gravitational force that is a galaxy or a star or any other massive object.

How does H0 ''Pop Out,'' Exactly?!

The project uses curved (as opposed to Euclidian) geometry to map the path between the object and the observer. A saddle point is defined in the length of time it takes for the light to reach the observer. Different lengths of time pop out due to the curvature of spacetime that results from the uneven distribution of matter density in space. The time delay surface is the difference between the times with and without the occurence of lensing. This surface defines the cosmology of the region of space and, using a complicated formula, ejects a value for H0.



Matt Shetrone and Clare Chemical Evolution of Dwarf Spheroidal (dSph) Galaxies

Constraints on Galaxy Formation from Abundance Ratios in Nearby Galaxies

Matt Shetrone
Hobby-Eberly Telescope, University of Texas at Austin, Texas

Shetrone and Clare walk Brown Bear around, left.

Questions about galaxy formation:

  • What are the building blocks for the halo of a galaxy?
  • From what does the halo accumulate?
  • Are there bits that didn't accumulate that are similar to the bits that did?
  • What do these extraneous bits look like? Could we recognize them unassociated?
  • If stars trace dark matter, do they then have the same origin?

What clues do we have to answer these questions?How do they pan out?
Halo metallicity:Doesn't tell the whole story.
High resolution, high signal-to-noise (S/N) spectra:Only way to reach weak line features--Cu, Eu, Ba; [Ba/Eu] then plot gives turn-on point for AGB stars. Also, assumptions about Ca lines tracing Fe lines are removed
Type II supernovae produce more magnesium than iron:Type Ia supernovae ''turn on'' at a certain point and drive ratio down
Determine ratios of s- to r-process elements (heavy elements) from meteorites:More reliable than supernova model; if [Ba/Eu] < 0, r-processes dominate, not AGB star. Thus restricts the timescale for star bursts and formation.
Mg to Fe ratio:Changes the number of free electrons in the atmosphere; thus changes both opacity and temperature
Alpha to Fe ratio:Alpha elements come from Type II supernovae and Fe from type Ia, therefore their ratio gives the ratio of the history of II:Ia supernovae in galaxies.

Results?

  • Dwarf spheroidal galaxy properties: metal poor and alpha elements enhanced.
  • Alpha elements in dwarf spheroidals are inconsistent with galactic halo stars.
  • There is no consistent picture for galaxy halo formation at this point; for example, the Milky Way Galaxy halo is not made of disrupted dwarf spheroidal galaxies.

The chart above demonstrates the previous conclusions by showing the abundances of alpha elements in dwarf spheroidal galaxies versus solar metallicity. The symbols are as follows:

  • blue triangles, Carina
  • blue triangles plus circles, Leo I
  • red triangles, Sculptor
  • red triangles plus circles, Fornax
  • green triangles, Draco, Ursa Minor, and Sextans from SCS01
  • black crosses, Glactic disk stars
  • open squares, halo data from McWilliam et al. 1995
  • light blue stars, UVES data from a study of LMC star clusters of different ages
  • light blue crosses, Galactic globular cluster measurements

For more information:

  • Nissen and Schuster. ''Chemical composition of halo and disk stars with overlapping metallicities.'' Astronomy and Astrophysics 326, 751-762 (1997).
  • Shetrone, Venn, Tolstoy. AJ 2002, submitted.
  • Tolstoy, Venn, Shetrone et al. AJ 2002, submitted.


Taft and Clare read together Survey for Dwarf Galaxies

Searches for Low Surface Brightness dSph Galaxies in the Local Group

Taft Armandroff
National Optical and Astronomical Observatories (NOAO) Tucson, Arizona

At left, Armandroff and Clare read together.

Motivation:

  • Luminosity function of the local group
    1. Creative/destructive processes (frequency distribution)
    2. Deviation in mass spectrum
    3. Self-shielding against photoionization
    4. Destruction by dynamical processes
    5. Cold dark matter theory
  • Environmental imapcts that form/destroy dSph galaxies
  • Additional dynamical probes: SIM and GAIA measure tangential motions
  • Previous Local Group surveys have not been as intensive as around Andromeda.





Local Group


How to find dwarfs:

The best way is with deep CCD imaging of faint, clumped stars. Take the radial velocity of every star and look for clumping in radial velocities.

At left, the image shows a map of the local group sky with the Roman numerals pointing out the locations of Armandroff's new Andromeda galaxy findings.

Impact of the search:

  • M31 is not poor in dwarf spheroidal galaxies
  • The luminosity function is looking very similar to the luminosity function of the Milky Way Galaxy, but still far fewer dwarf galaxies have been found than expected from Cold Dark Matter Theory.
  • Now we can compare luminosity functions of other clusters, especially rich clusters.
Future searches:

  • SDSS color-color diagrams see Willman et al (2002); they are expected to go down to about the 27th magnitude, which is about 1 magnitude fainter than Sextans, the faintest known dSph!
  • LSST 8m and fast surveys: all of the sky in about a week!

For more information:

  • Armandroff, Davies, and Jacoby. ''A Survey for Low Surface Brightness Galaxies around M31. I. The Newly Discovered Dwarf Andromeda V. The Astronomical Journal, 116:2287-2296, 1998 November.
  • Klypin et al. ApJ 1999 522:82.
  • Moore et al. 1999 ApJ 524:19.








Mario and Clare at the baseball game The Present, Past and Future of the Local Group

Mario Mateo
University of Michigan, Ann Arbor, Michigan

Clare and Mateo at the baseball game, at left.

The class watched anxiously as Mario Mateo, Kim Venn, and Barron Koralesky tried, in vain, to project Mateo's talk from his laptop onto the screen. Alas, it was not to be and the students sat back to see what Mateo could manage off the top of his head while his talk remained trapped in technology. Most expected a loose, general, non-specific talk. Yet all were pleasantly surprised as Mateo went through sheet after sheet of overhead transparency plastic. He gave us charts and graphs, statistics, and a fully cohesive and highly impressive talk right from his head. Not an event to have missed!

Paleontology vs. Astronomy:

Both scientists are looking back in time, but astronomers really can ''see'' back in time, while paleontologists can actually touch their objects of study.

Present:

Primary nearby sample:

  • Dwarf dominated (from our perspective)
  • 4-5 ''large'' galaxies
  • 2 dominate light and visible mass (M31 and Milky Way galaxies)
  • ~12 dwarf irregular (dIrr) galaxies signaling recent star formation
  • ~15 dwarf spheroidal (dSph) galaxies that are mostly old and gassless
  • ~5 transition systems
  • Dwarfs are clustered around M31 and MWG

The Hubble Sequence of galaxies?

The Hubble sequence is not apparent through the Hubble deep field surveys; but it is possible that we are in the middle of it and the rest of the sequence will become clear in the future.

The Local Group in Three Dimensions




The figure at right is a 3-D map of the current Local Group of Galaxies.

Past:

Density fluctuations in early universe evolved to present-day local group.

Cold Dark Matter Models:

  • Initial conditions: Dark matter halos with embedded baryonic disks (gas and stars)
  • Inject dwarf models into potential of large galactic system: Mparent/Mdwarf > 30
  • In the local group, relevant dynamical time scales are ~3-4 Gyr (age of local group is ~10-12 Gyr)
Tests:
  • Searches for streams
  • Kinematics (internal) with 8m telescopes and multi-object spectrographs to get 1000's of velocities
  • Kinematics (external) with SIM and GAIA and micro-arcsecond measurments to obtain orbits of everything in the galaxy using high resolution parallax (the Local Group is the limit for parallax)

Future:

  • Milky Way Galaxy and Large Magellanic Cloud (plus Small Magellanic Cloud connected by Magellanic Stream) will merge in 3-4 Gyr
  • LMC is gone
  • MWG: Velocity dispersions of galactic disk increase in all directions, heating and thickening the disk. Injects young, metal-poor stars.
  • M31 and MWG will eventually merge. In ~10 Gyr, systems will combine to form a large elliptical system.



Main Conclusions:

  • It is plausible that morphological transformation of galaxies is inevitable. Some minor, some transformative.
  • Don't sweat galaxy details all the time. Step back and see the big picture!
For more information:

  • Mayer, et al. ''Tidal Stirring and the Origin of Dwarf Spheroidals in the Local Group.'' The Astrophsyical Journal, 547:L123-L127, 2001 February 1.
  • Mateo, Mario. Annual Review of Astronomy and Astrophysics, 1998. Volume 36, page 435.


Page last updated August 28, 2002
cblank@macalester.edu


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