Title: Astro 105: Our Place in the Universe
1Astro 105 Our Place in the Universe
Lecture 14
- Lecturers
- J.P.Ostriker
- A.E.Shapley
- J.E. Gunn
- P. Steinhardt
2Logistics
- Assignment 5 due today!
- Solution set 4 is posted on the course website
and on Blackboard, so no more late assignment
4s accepted. - No homework over Thanksgiving (except to think
about the expansion and geometry of the Universe.
Yeah, right.)
3Overview
- Review of CMB highlights, some questions that
arose last time - How do ripples in the CMB tell you about the
geometry of the Universe? (Finish up cosmological
parameters) - How are the fluctuations in the CMB radiation
related to the rich structure (galaxies,
clusters) we see around us today? - Attempts to map out the distribution of galaxies
in the local and distant Universe
(distantlooking back in time) - Galaxy formation and evolution
4Review
- Hot Big Bang Model (LeMaitre, Gamow, Alpher,
Herman) - Blackbody radiation (Universe as a blackbody)
- When Universe cools to 3000K, it is no longer
opaque, photons can get to us. Radiation that is
coming from so far away that it probes this
Recombination epoch, said to come from the
Surface of Last Scattering - Search for CMB radiation (Penzias, Wilson,
Dicke, Wilkinson, Roll, Peebles) - COBE (FIRAS told us it was a blackbody spectrum,
DMR showed the anisotropies of 1 part in 100,000) - WMAP, current state of the art CMB mission, maps
the surface of last scattering with much higher
spatial resolution, allows for exquisite study of
the characteristic size of the ripples
5Side note on the Big Bang
Last time, the balloon analogy was used to show
the expanding Universe. Note this is a 2D
analogy for 3D space. Where is the center of the
explosion on the surface of the balloon? (not the
center of the balloon!!!!!) There is no center of
the Big Bang explosion -- every galaxy sees the
same thing.
At t0, space is infinitely dense
EVERYWHERE!! Not just at one singularity. Dont
think of it like a bomb exploding.
6The Hot Big Bang Model
- George Gamow, Ralph Alpher, and Robert Herman
- Predicted elemental abundances formed in Hot Big
Bang, and also that the Universe should be filled
with relic radiation corresponding to a blackbody
at 5K
7Review
- Hot Big Bang Model (LeMaitre, Gamow, Alpher,
Herman) - Blackbody radiation (Universe as a blackbody)
- When Universe cools to 3000K, it is no longer
opaque, photons can get to us. Radiation that is
coming from so far away that it probes this
Recombination epoch, said to come from the
Surface of Last Scattering - Search for CMB radiation (Penzias, Wilson,
Dicke, Wilkinson, Roll, Peebles) - COBE (FIRAS told us it was a blackbody spectrum,
DMR showed the anisotropies of 1 part in 100,000) - WMAP, current state of the art CMB mission, maps
the surface of last scattering with much higher
spatial resolution, allows for exquisite study of
the characteristic size of the ripples
8Blackbody Radiation
- Radiation emitted by opaque surface that absorbs
all the light that falls on it, and is
characterized by a certain temperature, T. - Temperature measures the amount of microscopic
motion within a system. - Object at temperature, T, emits a very specific
spectrum, that is a function of the temperature,
T, and the wavelength, l. - Spectrum has a peak at a characteristic
wavelength, which is bluer for higher
temperatures and redder for lower temperatures
9Review
- Hot Big Bang Model (LeMaitre, Gamow, Alpher,
Herman) - Blackbody radiation (Universe as a blackbody)
- When Universe cools to 3000K, it is no longer
opaque, photons can get to us. Radiation that is
coming from so far away that it probes this
Recombination epoch, said to come from the
Surface of Last Scattering - Search for CMB radiation (Penzias, Wilson,
Dicke, Wilkinson, Roll, Peebles) - COBE (FIRAS told us it was a blackbody spectrum,
DMR showed the anisotropies of 1 part in 100,000) - WMAP, current state of the art CMB mission, maps
the surface of last scattering with much higher
spatial resolution, allows for exquisite study of
the characteristic size of the ripples
10Surface of Last Scattering
- The key is that something important happens when
the Universe cools to 3000K, which is about
300,000 years after the Big Bang. - Protons and electrons combine to form atoms, and
photons no longer scatter off of electrons. The
primeval fireball cools to the point that it is
no longer opaque. - Photons can free stream to us, from z1100.
Along the way they redshift, and reflect the
overall expansion and cooling of the universe. - These photons make up the microwave background
radiation. - We cant see farther back than z1100, because
the Universe was opaque.
11Review
- Hot Big Bang Model (LeMaitre, Gamow, Alpher,
Herman) - Blackbody radiation (Universe as a blackbody)
- When Universe cools to 3000K, it is no longer
opaque, photons can get to us. Radiation that is
coming from so far away that it probes this
Recombination epoch, said to come from the
Surface of Last Scattering - Search for CMB radiation (Penzias, Wilson,
Dicke, Wilkinson, Roll, Peebles) - COBE (FIRAS told us it was a blackbody spectrum,
DMR showed the anisotropies of 1 part in 100,000) - WMAP, current state of the art CMB mission, maps
the surface of last scattering with much higher
spatial resolution, allows for exquisite study of
the characteristic size of the ripples
12Detection of CMB
- Dicke, Wilkinson, Roll, Peebles at Princeton,
both experimentalists and theorists - Penzias and Wilson at Bell Labs
- 1964-1965, Detection of excess noise, turned out
to be CMB radiation, fit with predictions - What exactly did they detect (what does 3K noise
mean)??
13Detection of CMB
- Radio antenna collects radio waves (which are
light waves with long wavelengths, longer than 1
mm) - Examples of antennae on TVs, radio dishes,
horns - Radio waves sent to a receiver which records
the strength of the radio signal - CMB detection was a certain flux of radio waves.
If you have a blackbody at 3K, you know exactly
what flux to detect at each wavelength, according
to the BB spectrum.
14Big Bang Nucleosynthesis
- One of the predictions of the Big Bang model is
that, for a given baryon density, Wb, the
primordial abundances of Helium, Deuterium, and
Lithium are all fixed (reaction rates depend on
Wb). - The predictions of the Big Bang model for the
abundances of these light elements are consistent
with the observed values, for a single Wb (value
of Wb is consistent with other estimates)
Major success of Big Bang Model
15Big Bang Nucleosynthesis
- What is deuterium?
- Heavy hydrogen, nucleus with one proton and
one neutron - Produced in Big Bang along with helium and
lithium, and not made anywhere else. - In fact it is destroyed in stars
- The amount of deuterium produced in the Big bang
is very sensitive to the density of baryons - Higher baryon density -- less deuterium, which
gets converted to helium - Measurements made in intergalactic gas at high
redshift
Major success of Big Bang Model
16Review
- Hot Big Bang Model (LeMaitre, Gamow, Alpher,
Herman) - Blackbody radiation (Universe as a blackbody)
- When Universe cools to 3000K, it is no longer
opaque, photons can get to us. Radiation that is
coming from so far away that it probes this
Recombination epoch, said to come from the
Surface of Last Scattering - Search for CMB radiation (Penzias, Wilson,
Dicke, Wilkinson, Roll, Peebles) - COBE (FIRAS told us it was a blackbody spectrum,
DMR showed the anisotropies of 1 part in 100,000) - WMAP, current state of the art CMB mission, maps
the surface of last scattering with much higher
spatial resolution, allows for exquisite study of
the characteristic size of the ripples
172 Big Results From COBE
- FIRAS showed that the spectrum of the CMB
radiation was that of a blackbody with T2.725K
(consistent with prediction that Universe cooled
from initial hot big bang). - DMR showed fluctuations of 1 part in 100,000
(once the motion of the sun, and the emission
from the galaxy are subtracted off) The
fluctuations are regions slightly hotter or
colder than the average temperature of 2.725.
18What are we looking at?
- This is an all-sky map in Galactic coordinates
from COBE. - The plane of our Milky Way runs horizontally
across the middle of the map. - Top map shows the solar system motion in the
Universe (we are not at rest wrt the CMB in every
direction) middle map shows our Galaxy bottom
map shows density fluctuations in the early
Universe (denser-- intrinsically hotter, less
dense-- intrinsically colder), but gravitational
redshift reverses it - This is a map of the surface of last scattering.
These photons have traveled to us since the
Universe was a few 100,000 yrs old. Remember
19Review
- Hot Big Bang Model (LeMaitre, Gamow, Alpher,
Herman) - Blackbody radiation (Universe as a blackbody)
- When Universe cools to 3000K, it is no longer
opaque, photons can get to us. Radiation that is
coming from so far away that it probes this
Recombination epoch, said to come from the
Surface of Last Scattering - Search for CMB radiation (Penzias, Wilson,
Dicke, Wilkinson, Roll, Peebles) - COBE (FIRAS told us it was a blackbody spectrum,
DMR showed the anisotropies of 1 part in 100,000) - WMAP, current state of the art CMB mission, maps
the surface of last scattering with much higher
spatial resolution, allows for exquisite study of
the characteristic size of the ripples
20Current State of the Art WMAP
- Wilkinson Microwave Anisotropy Probe
(NASA/Goddard/Princeton), launched in 2001, still
collecting data, named for Princeton physicist
David Wilkinson - All-sky map, but at much higher angular
resolution than COBE (sharper image) - Allows us to answer questions about the geometry
of the Universe (as well as a bunch of other
parameters). Is it closed, flat, or open? - COBEs angular resolution was about 7 degrees
(14 times the diameter of the full moon), while
WMAP has resolution of 0.3 degrees (a bit less
than the diameter of the full moon)
21Current State of the Art WMAP
Resolution more than 20 times better with WMAP
22A Characteristic Scale
- It turns out that there is a specific angular
scale (hot/cold patch size), on which we expect
to see the most contrast. This scale corresponds
to the angular size that the observable Universe
at z1100 subtends on the sky today (about 1
degree) - Figuring out the exact angular size where we see
the most variation tells us about the global
geometry of the Universe (closed/flat/open)
23A Characteristic Scale
24A Characteristic Scale Geometry
- Hopefully, you can see how the characteristic
size of the pattern depends on the overall
geometry of space - When the Universe is closed, the pattern subtends
a larger angular size (like the angles of the
triangle adding up to more than 180 degrees)
when the Universe is open, the pattern subtends a
smaller angular size for a flat universe, the
pattern will subtend a size that is intermediate. - The verdict from BOOmerang and WMAP The Universe
is spatially flat!! - This means WmWL 1
- Next big mission Planck, to be launched in 2007.
25A Characteristic Scale Geometry
- Weve already made a pretty good case for Wm0.3.
- The CMB therefore offers independent evidence
that WL0, and yields a value (0.7) consistent
with the results from Type Ia Supernovae and the
acceleration of the Universe. - This is amazing the CMB anisotropies and the
measurements of distances and redshifts of
supernovae are two completely indpendent methods
that provide evidence for a spatially flat
Universe with non-zero cosmological constant and
less than critical matter density.
26Working Timeline since BB
27Evidence for BB Model
- Galaxies are receding from each other, the
expansion of the universe - Success of the Hot Big Bang model for producing
the relative abundances of light elements like
Helium, Deuterium, and Lithium - Detection of 3K blackbody CMB radiation
28The Ripples (Anisotropies)
- Weve discussed how the temperature anisotropies
correspond to density fluctuations in the
Universe at z1100. - Two important questions about the anisotropies
- 1. What caused the initial fluctuations in
density? - How do the fluctuations evolve?
- Or, more generally how do we go from a
Universe that appears so simple and smooth (the
maps enhance the fluctuations) to one that
contains so much structure? - Mapping the distribution of galaxies and
comparing with simulations helps us understand
2., at least.
29The Ripples (Anisotropies)
- Temperature fluctuations in the early universe,
from the slight clumping of matter (map on
surface of last scattering) - Structure growing as denser regions attract more
matter, seeded from the early fluctuations -
- The first stars form in the regions of highest
density - More stars turning on, galaxies forming
- The modern era
30Ideas of structure formation
31Structure Formation
- While we believe that on the largest scales is
homogeneous and isotropic, the distribution
of matter in the Universe is not completely
uniform - Our galaxy lies in what is called the Local
Group, with M31 (falling towards us), the Large
and Small Magellanic Clouds, and lots of other
small galaxies - Already in the time of Hubble and Zwicky, we
knew that galaxies were also found in groups and
clusters. Nearby clusters include the Virgo
Cluster (hundreds, maybe thousands of galaxies),
and the Coma cluster. Clusters are grouped in
even larger structures. - Hierarchical clustering.
- Deep Thoughts Questions What came first? The
galaxies or the clusters? When did the galaxies
start to form?
32Structure Formation
Northern galactic hemisphere
- Lick Observatory Counts of galaxies in 10
arcminute by 10 arcminute cells (1967) - No redshifts, but still the clustering is clear,
started the theorists (i.e. Peebles) thinking
33Structure Formation
- 1960-1980s
- Bottom-up structure formation (Peebles) begin
with small objects that form first, which then
merge to form larger objects - Top-down structure formation (Zeldovich, Silk)
structure forms first on the largest scales
pancakes (supercluster and cluster), which then
fragment into smaller objects - It turns out that the nature of dark matter
affects what type of structure formation occurs - If we have hot dark matter, i.e. matter that
moves at close to the speed of light at z1000,
the idea is that all the small-scale fluctuations
get washed out early in the Universe by the
relativistic motions of the particles, and you
only get large-scale clumps. One such example is
the neutrino. - If we have cold dark matter, matter that moves
non-relativistically in the early universe,
small-scale fluctuations dont get destroyed
34Structure Formation
z0, i.e. today
- CDM simulation, more clustering of objects on
smaller scales (small clumps) - 300 Mpc on a side, slice of simulation with dark
matter
- HDM simulation, less clustering of objects on
smaller scales (small clumps) - 300 Mpc on a side, slice of simulation with dark
matter
(courtesy, M. White)
35Structure Formation
- We now know that Hot Dark Matter doesnt work.
Galaxies form too late (we have now observed
galaxies, which correspond to small-scale
fluctuations) out to high redshift. In HDM model,
these dont form until zcorrelations observed today among the positions
of galaxies mapped out in redshift surveys dont
match the predictions for HDM - Cold Dark Matter with bottom-up structure
formation is the favored model. - BUT in the 1960s and 1970s, we didnt have a
detailed map of the galaxies and (by inference)
the underlying dark matter distribution, to test
the models. - Therefore, an important goal was to map out the
3D large-scale structure in the Universe. This
large-scale structure is the descendant of the
density ripples revealed in the CMB.
36Galaxy Redshift Surveys Mapping the Universe
37Galaxy Redshift Surveys
- As of 1970s, there were only 250 published
redshifts of galaxies, mainly from Humason,
Mayall, and Sandage - (Side note remember from Jim Gunns lecture and
lecture on the expansion of the Universe, Sandage
was Hubbles student (heir), has spent his lifes
work trying to determine Hubble Constant and
deceleration of the Universe.) - Why so few redshifts?
- Redshifts were HARD!! As opposed to images,
where all the wavelengths of light that emanate
from a given galaxy location expose the same
corresponding location on the photographic plate.
With spectra (required for redshifts), the light
gets spread out into all of its component
wavelengths. So, any specific place on the
photographic plate receives less light. - Goal of redshift surveys use Hubbles law to
approximate distances with redshifts. Make a 3D
map of the galaxies.
38CfA Redshift Surveys
- Mid-Late 1970s Marc Davis, Princeton graduate
student of Wilkinson and Peebles, tries to
calculate how galaxies should be clustered in
space, goes to Harvard Center for Astrophysics
(CfA) as an assistant professor in the late
1970s, embarks on a survey of galaxies, along
with Dave Latham, John Huchra, and grad student
John Tonry - Use a new detector for measuring spectra (not
photographic plates), but not CCDs yet
Davis
Latham
Huchra
Tonry
Geller
39CfA Redshift Surveys
- Conduct the survey on Mt. Hopkins near Tucson,
on a 60 telescope, 1977-1982 - Obtain redshifts for 2400 galaxies drawn from
catalog of Zwicky, brighter than a certain limit
(mag14.5), 3000 times fainter than what the
naked eye can see. The average redshift of the
galaxies they target is 0.015, or 5000
km/s. The furthest is about z0.03. - Covered a large area on the sky 2.7 steradians
(how big is that?) - First quantitative estimates of the clustering
of galaxies
Davis
Latham
Huchra
Tonry
Geller
40CfA Redshift Surveys
- Second CfA Survey, started by John Huchra and
Margaret Geller in 1984, completed 1995 - Measured redshifts for 18,000 galaxies
- What did they find?
- Frothy structure, large filamentary
superclusters up to 60 Mpc in extent, large voids
20-30 Mpc in diameter - Is this a fair sample? Complementary to pencil
beam surveys that go to higher redshift, but
cover smaller area on the sky
Davis
Latham
Huchra
Tonry
Geller
41CfA Redshift Surveys
- Slice of the Universe , 1100 galaxies in a
strip 6 degrees by 130 degrees, part of CfA2
redshift survey (credit SAO Huchra) - Stick man!!!
Davis
Latham
Huchra
Tonry
Geller
42CfA Redshift Surveys
- 6 Slices of the Universe (thicker than the
last image, credit SAO, John Huchra) - Do you see the Great Wall, largest structure
detected in any redshift survey when it was
found? Hundreds of Mpc in extent in longest
dimension.
Davis
Latham
Huchra
Tonry
Geller
43CfA Redshift Surveys
- The CfA redshift surveys allowed for comparison
with theoretical predictions. - In subsequent years, other surveys pushed out to
higher redshifts. Most recently, two large
surveys are the 2 Degree Field (2dF) Galaxy
Redshift survey, and the Sloan Digital Sky Survey
(SDSS). - These (especially SDSS) represent the state of
the art in redshift surveys.
Davis
Latham
Huchra
Tonry
Geller
44Sloan Digital Sky Survey
- Started in the late 1980s, by Jim Gunn
(Princeton), Richard Kron, and Donald York (U.
Chicago). - Goal Surveying 25 of the whole sky. How many
square degrees are there in the sky (lets
calculate that in terms of full moons)? - Observations started in 1998-1999, conducted on
a special-purpose 2.5 meter telescope in Apache
Point, New Mexico. Use of CCDs for both imaging
and spectroscopy much more sensitive! - First part, imaging in 5 color filters, 100
million celestial objects - Second part, spectroscopy of more than 1 million
galaxies and quasars, 608 objects at a time (vs.
CfA redshift survey, which was 1 object at a
time), using a fiber spectrograph
(credit M. Strauss Sci. Am. Article)
45Sloan Digital Sky Survey
(credit M. Strauss Sci. Am. Article)
- Comparison of SDSS slice with CfA2 slice (find
stick man!) - SDSS Great Wall 300 Mpc long
- This SDSS slice represents 1 of SDSS volume
46Sloan Digital Sky Survey
- SDSS provides the best statistical map of galaxy
positions and luminosities to date, for
comparison with numerical simulations, which have
also advanced a lot in the last twenty years. - One important question is, are galaxies
unbiased tracers of the underlying dark matter
distribution.
(credit M. Strauss Sci. Am. Article)
47Sloan Digital Sky Survey
- Not just redshift survey (though it is the best
one at z0!!) - So much more, in countless areas of astronomy
- Galaxy luminosity function what is the relative
number of galaxies as a function of intrinsic
luminosity (there are a lot more faint galaxies
than bright ones) - The structure of our Milky Way and Local Group
- Exotic stellar and moving objects
- Galaxy and Black Hole evolution
- Quasars in the early universe, understand how
the intergalactic gas returned from neutral to
ionized at z6. - More, more, more. This is a true goldmine of
data, and its right here!
48Higher zDEEP2 Redshift Survey
- University of California project to survey
40,000 galaxies at z1 (8 billion light years
away) using the Keck 10-meter telescope in
Hawaii, 4 square degrees on the sky. - Galaxies about 10,000 times fainter than faint
limit of original CfA survey - Goal is to look at large scale structure at z1
(how has the large-scale structure evolved over 8
billion years), as well as galaxy evolution. - This project is led by Marc Davis and Sandy
Faber.
Map of galaxies in DEEP2 field (courtesy A. Coil)
49Even Higher z
- We have statistical samples of galaxies at z2,
z3, z4, back to when the Universe was only 1-2
billion years old. Interesting selection
techniques. You have to be trickier than just
trying to get redshifts for all galaxies brighter
than a certain flux value. - We can even study the large-scale distribution
of these distant galaxies. - We also want to understand how the galaxy
internal properties evolve, and how the galaxies
actually form. We can tell from just looking at
them that these galaxies in the early Universe do
not look like nearby spirals and ellipticals, but
much more irregular. - But, galaxy formation is a topic for another
day
50What caused the initial ripples?
- One of the questions at the beginning was what
caused the initial fluctuations in density that
we observe in the CMB radiation? - One theory is something called inflation. This
theory is described in Chapter 9, pp. 137-148, in
the book by Martin Rees. We may discuss this
later on.