Notes
Slide Show
Outline
1
Astr 5460     Wed., Nov. 3, 2004
  •    This week: Large Scale Structure
  • (Ch. 11, Combes et al., parts)


  •   Unless noted, all figs from Combes et al.
  • Already talked about galaxy clusters a lot, and some distance ladder topics will be covered in more detail in Mike Pierce’s class next semester.
2
Some other issues
  • Discuss homework
    • Not as great as expected – just busier now?  Can turn in problem 6 next week for extra credit – please write up the process!
  • Discuss Observing Project (briefly!)
  • Mid-term exam:
    • 2 hours, take-home, on your honor, only calculator and constants/conversions
    • Some “basic knowledge” questions in addition to more analytic problems.  Know terms, definitions, other intangible issues.
3
Large Scale Structure
  • Galaxy structure – how is the mass in the universe distributed (and recall gas can be important, too!)?  Homogeneous?  On what scale?
  • Text is a bit old (fine for history), but the best newest information will come from SDSS and 2dF.  CHECK IT OUT!
  • Background radiation also of interest (discrete sources vs. true diffuse background).


4
Background “SED”
  • CMBR of special interest (as we will get to) and X-ray is a recent development (CXO).
5
Distance Scales
  • Parallax and Trigonometric Methods:
6
Distance Scales
  • Parallax and Trigonometric Methods
7
Distance Scales
  • Parallax and Trigonometric Methods
    • tan λ = Vt/Vr = μd/Vr
    • So then d = Vr tanλ/4.74μ [pc]
    • Where velocities are in km/s and proper motion μ is in arcseconds per year.
    • Should be something you can derive (it would be a good problem to work in your free time)


8
Distance Scales
  • Parallax and Trigonometric Methods – once Hyades distance known, can use main-sequence cluster fitting.
9
Distance Scales
  • Parallax and Trigonometric Methods – once Hyades distance known, can use main-sequence cluster fitting.
  • Then employ the distance modulus, basically a vertical shift on the CMD diagram, (m-M = 5 logd(pc) -5)
10
Distance Scales
  • Cepheids and Standard Candles
    • Various stars in the instability strip of the H-R diagram with Period-luminosity relations.
11
Distance Scales
  • Cepheids and Standard Candles
    • Various stars in the instability strip of the H-R diagram with Period-luminosity relations.
    • Figures for Cepheids from Horizons (Michael Seeds)
12
Distance Scales
  • The Tully-Fischer Relation
  • L = kΔVα – where the index is ~ 4.
  • Better in the near-IR, as we discussed before, less star formation visible at H-band, so less distortion.
  • The velocity dispersion comes from either 21 cm or stellar optical absorption lines.
13
Distance Scales
  • This is where Combes et al. discusses the Hubble Law:
    • Vr = Hod where Ho is in km/s/Mpc
    • Hubble constant Ho is independent of direction in the sky (that’s important, think about it!)
    • Also recall Ho = h 100 km/s/Mpc
14
Distance Scales
  • The Tully-Fischer Relation
15
Distance Scales
  • Malmquist Bias:
16
Distance Scales
  • The Sunyaev-Zeldovich Effect:
    • Look toward hot intercluster medium in galaxy clusters…Thomson scattering can affect the CMBR seen through such a medium
    • Optical thickness is τT = ∫σTne dl
    • Cluster properties can indeed “hamper” the CMBR
    • The CMBR is heated by the ICM, altering the frequency: Δν/ν = 4kTe/mec2, leading to:
    • ΔT/T = - ∫ 2kTe/mec2 dτT (hν << kTe)
    • At low frequencies, REDUCES the temperature of the CMBR.
    • Can get distance estimates from S-Z effect.
17
Distance Scales
  • The Sunyaev-Zeldovich Effect
  • Measure the X-ray flux, the temperature fluctuations, and the temperature, and can get distance, and hence Ho.
  • Compton effect here
18
Distance Scales
  • Surface-Brightness Fluctuations
  • Surface brightness does not vary with distance – why?
  • How about, say, the number of stars per pixel as a function of distance?  That does change, and the statistical uncertainty does vary with distance.
19
Distance Scales
  • Surface-Brightness Fluctuations
20
The “Third Dimension”
  • Galaxy distributions seen in images are 2-d projections on the sky.
  • Need distances…easiest way is to use the Hubble flow and redshifts, either photometric or spectra (best).
  • Reminder – SDSS and 2dF rule here now.
  • Huchra and Gellar’s “Z-machine” for the CfA survey as recounted in “Lonely Hearts of the Cosmos” by Dennis Overbye – Great!
21
The “Third Dimension”
  • Look at distance “slices” here.
22
The “Third Dimension”
  • The famous “man” in the distribution.  Shows walls, voids, etc.
  • Why elongations, “finger of god” distributions pointing at “us?”
23
Statistical Methods
  • Correlation functions
    • How do you measure, quantitatively, the tendency of galaxies to cluster?
    • Following is specifically from Longair, but also present in Combes et al. with a different presentation.
24
Large-scale Distribution of Galaxies
25
Large-scale Distribution of Galaxies
  • On small scales, the universe is very inhomogeneous (stars, galaxies).  What about larger scales?
  • Angular two-point correlation function w(θ):
26
Large-scale Distribution of Galaxies
  • This function w(θ) describes apparent clustering on the sky down to some magnitude limit.
  • More physically meaningful is the spatial two-point correlation function ξ(r) which describes clustering in 3-D about a galaxy:
27
Large-scale Distribution of Galaxies
  • w(θ) isn’t so hard to measure from various surveys – just need positions.
  •  ξ(r) is harder – must have redshifts to do properly.  Can make some assumptions however.
28
Large-scale Distribution of Galaxies
29
Large-scale Distribution of Galaxies
30
Large-scale Distribution of Galaxies
31
Large-scale Distribution of Galaxies
32
Large-scale Distribution of Galaxies
33
Large-scale Distribution of Galaxies
34
Large Scale Motions
  • Milky Way motion vs. CMBR, a “dipole” with velocity of about 1000 km/s (from COBE)
35
Large Scale Motions
  • “The Great Attractor”