Using the Sunyaev-Zeldovich Effect to Constrain H0
- Introduction
- Importance of H0 to Cosmology
- Constrain age, expansion history of universe
- Get distances to galaxies via Hubble's law
- Traditional Method: Distance Ladder
- Cepheid distance scale
- Secondary Indicators: TF, FP, SNeIa, etc
- Results, ie from HST Key Project Team showing H0=72
- Uncertainties: how distance errors add up
- Describe need for a direct distance indicator
- CMB constraints on H0
- Quick description of physics
- Results from WMAP5: H0=73, consistent w/ HST KP results
- Why do it w/ SZ?
- Different systematic effects
- Doesn't rely on ladder w/ error buildup
- Good to have cross-checks
- SZ Physics - Ideal case
- CMB properties: temp, spectrum, temp fluctuations
- Properties of clusters: hot gas, emitting X-rays through
free-free radiation, characteristic mass, luminosity, temp
- Compton Scattering
- Physical description
- Effect on spectrum
- Discriminating SZ fluctuations from CMB fluctuations
- SZ signal
- Dependancy on cluster properties: ne, T, size
- Dependancy on H0
- Solving for H0
- Data Source
- Millimeter arrays: OVRO, BIMA, others
- X-ray satellites: Einstein, ROSAT, Chandra, etc
- Data for imaging: need X-ray maps
- Data for spectroscopy: to get cluster temperature
- Complications
- Clusters not relaxed
- Describe cluster accretion history
- Destroys symmetry (show pictures of unrelaxed clusters from
Chandra)
- Artificially heats clusters beyond the virial temperature
- Simulations show this bias; allow us to correct (e.g.,
Roettiger etal 1997)
- Need high data quality
- Show uncertainty in spectral fits, and how that translates to
uncertainty in T
- Need good spatial resolution to get ne,T profiles (show good
and bad data)
- Modeling needed to turn projected T, ne into 3-D profiles
- Results
- Early work (1990s)
- Data source: OVRO/ROSAT
- Individual cluster variations (eg Abell 2218)
- H0 fits: all over the pllace
- More recent work (2000s)
- New millimeter arrays (CARMA, DASI)
- New Xray data (Chandra)
- Show examples of good data, ie SZ signal and X-ray maps
- Bigger samples (Bonamente et al sample)
- Recent H0 determinations
- H0=66 (Jones etal 2005)
- H0=77 (Bonemente etal 2006)
- Dominant source of uncertainty
- Cluster X-ray profile fitting
- Temperature effects
- Future work
- H0
- Bigger SZ samples
- New arrays, better spatial
resolution (examples)
- Simulations: what N-body
simulations need to give (ie in terms of corrections for accretion
effects)
- Other parameters -- briefly how SZ
can constrain
- New projects coming online:
- Summary
- References
(and you should have a dozen or so references in place by
now, and they should come from advanced textbooks, journal articles,
conference reviews, project webpages, etc...)