Title: Professor Lynn Cominsky
1Astronomy 350Cosmology
- Professor Lynn Cominsky
- Department of Physics and Astronomy
- Offices Darwin 329A and NASA EPO
- (707) 664-2655
- Best way to reach me lynnc_at_charmian.sonoma.edu
2Group 8
- Robert Angeli
- Jacy Maka
- Ryan McDaniel
- Rena Morabe
Let's hear it for Group 8!
3Composition of the Cosmos
4Keplers Third Law movie
5Dark Matter Evidence
- In 1930, Fritz Zwicky discovered that the
galaxies in the Coma cluster were moving too fast
to remain bound in the cluster according to the
Virial Theorem
KPNO image of the Coma cluster of galaxies -
almost every object in this picture is a galaxy!
Coma is 300 million light years away.
6Virial Theorem
- Stable galaxies should obey this law 2K -U
- where K½mV2 is the Kinetic Energy
- U -aGMm/r is the Potential Energy (a is
usually 0.5 - 2, and depends on the mass
distribution) - Putting these together, we have MV2r/aG.
- Measure M, r and V2 from observations of the
galaxies then use M and r to calculate Vvirial - Compare Vmeasured to Vvirial
- Vmeasured gt Vvirial which implies M was too small
7Galaxy Rotation Curves
- Measure the velocity of stars and gas clouds
from their Doppler shifts at various distances - Velocity curve flattens out!
- Halo seems to cut off after r 50 kpc
v2GM/r where M is mass within a radius r Since
v flattens out, M must increase with increasing r!
8Dark Matter Activity 1
- Measure the radial velocity as a function of
distance from the center of the galaxy - Calculate the mass of the galaxy at a given
distance from the center, for each radial
velocity - Measure the light coming from the galaxy inside
of a given radius - Calculate the mass of the galaxy again, from the
light that it emits at a given distance from the
center - Plot the masses (from the radial velocity) vs.
the masses (from the light) - Answer the other questions on the worksheet
9Hot gas in Galaxy Clusters
- Measure the mass of light emitting matter in
galaxies in the cluster (stars) - Measure mass of hot gas - it is 3-5 times
greater than the mass in stars - Calculate the mass the cluster needs to hold in
the hot gas - it is 5 - 10 times more than the
mass of the gas plus the mass of the stars!
10Dark Matter Halo
- The rotating disks of the spiral galaxies that we
see are not stable - Dark matter halos provide enough gravitational
force to hold the galaxies together - The halos also maintain the rapid velocities of
the outermost stars in the galaxies
11Types of Dark Matter
- Baryonic - ordinary matter MACHOs, white, red or
brown dwarfs, planets, black holes, neutron
stars, gas, and dust - Non-baryonic - neutrinos, WIMPs or other
Supersymmetric particles and axions - Cold (CDM) - a form of non-baryonic dark matter
with typical mass around 1 GeV/c2 (e.g., WIMPs) - Hot (HDM) - a form of non-baryonic dark matter
with individual particle masses not more than
10-100 eV/c2 (e.g., neutrinos)
12Big Bang
- Written, directed and starring the Physics
Chanteuse Lynda Williams - From her CD Cosmic Cabaret
- Available from www.scientainment.com
13Primordial Matter
- Normal matter is 3/4 Hydrogen (and about 1/4
Helium) because as the Universe cooled from the
Big Bang, there were 7 times as many protons as
neutrons - Almost all of the Deuterium made Helium
Hydrogen 1p 1e
Deuterium 1p 1e 1n
Helium 2p 2e 2n
14Primordial Matter
- The relative amounts of H, D and He depend on h
(protons neutrons) / photons - h is very small - We measure about 1 or 2 atoms
per 10 cubic meters of space vs. 411 photons in
each cubic centimeter - The measured value for h is the same or a little
bit smaller than that derived from comparing
relative amounts of H, D and He - Conclusion we may be missing some of baryonic
matter, but not enough to account for the
observed effects from dark matter!
15Baryonic Dark Matter
- Baryons are ordinary matter particles
- Protons, neutrons and electrons and atoms that we
cannot detect through visible radiation - Primordial Helium (and Hydrogen) recently
measured increased total baryonic content
significantly - Brown dwarfs, red dwarfs, planets
- Possible primordial black holes?
- Baryonic content limited by primordial Deuterium
abundance measurements
16Baryonic - Brown Dwarfs
- Mass around 0.08 Mo
- Do not undergo nuclear burning in cores
- First brown dwarf star Gliese 229B
17Baryonic - Red Dwarf Stars
- HST searched for red dwarf stars in the halo of
the Galaxy - Surprisingly few red dwarf stars were found, lt 6
of mass of galaxy halo
18Ghost Galaxies
- Also known as low surface brightness galaxies
- Studies have shown that fainter, elliptical
galaxies have a larger percentage of dark matter
(up to 99) - This leads to the surprising conclusion that
there may be many more ghostly galaxies than
those we can see! - Each ghost galaxy has a mass around 10 million Mo
19Baryonic MACHOs
- Massive Compact Halo Objects
- Many have been discovered through gravitational
micro-lensing - Not enough to account for Dark Matter
- And few in the halo!
20Baryonic MACHOs
- 4 events towards the LMC
- 45 events towards the Galactic Bulge
- 8 million stars observed in LMC
- 10 million stars observed in Galactic Bulge
- 27,000 images since 6/92
21Gravitational Microlensing
- Scale not large enough to form two separate images
movie
22Baryonic black holes
- Primordial black holes would form at 10-5 s after
the Big Bang from regions of high energy density - Sizes and numbers of primordial black holes are
unknown - If too large, you would be able to see their
effects on stars circulating in the outer Galaxy - Black holes also exist at the centers of most
galaxies but are accounted for by the
luminosity of the galaxys central region
23Black Hole MACHO
- Isolated black hole seen in Galactic Bulge
- Distorts gravitational lensing light curve
- Mass of distorting object can be measured
- No star is seen that is bright enough..
24Strong Gravitational Lensing
25Strong Gravitational Lensing
- HST image of background blue galaxies lensed by
orange galaxies in a cluster - Einsteins rings can be formed for the correct
alignment
26Strong Gravitational Lensing
- Spherical lens
- Perfect alignment
- Note formation of Einsteins rings
27Strong Gravitational Lensing
- Elliptical lens
- Einsteins rings break up into arcs if you can
only see the brightest parts
28Dark Matter telescope
- At least 8 meter telescope
- About 3 degree field of view with high angular
resolution - Resolve all background galaxies and find
redshifts - Goal is 3D maps of universe back to half its
current age
29Gravitational Lens Movie 1
- Movie shows evolution of distortion as cluster
moves past background during 500 million years
- Dark matter is clumped around orange cluster
galaxies - Background galaxies are white and blue
30Gravitational Lens Movie 2
- Movie shows evolution of distortion as cluster
moves past background during 500 million years
- Dark matter is distributed more smoothly around
the cluster galaxies - Background galaxies are white and blue
31Baryonic cold gas
- We can see almost all the cold gas due to
absorption of light from background objects - Gas clouds range in size from 100 pc (Giant
Molecular Clouds) to Bok globules (0.1 pc) - Mass of gas is about the same as mass of stars,
and is part of total baryon inventory
32Baryonic dust
- Dust is made of elements heavier than Helium,
which were previously produced by stars (lt2 of
total) - Dust absorbs and reradiates background light
33Non-baryonic - neutrinos
- Start with a decaying neutron at rest
- This reaction does not conserve energy because
the proton and electron together do not weigh as
much as the neutron - The reaction also does not conserve momentum, as
nothing is moving to the left - The anti-neutrino makes it all balance
electron
34Neutrino mysteries
- Neutrinos are believed to have zero mass and
therefore can travel at the speed of light - Neutrinos interact very weakly with other
particles - There are about 100 million neutrinos per cubic
meter - There are three types of neutrinos (and
anti-neutrinos) electron, muon and tau - More (or less) types of neutrinos would lead to
more (or less) primordial Helium than we see
35Neutrino mysteries
- Not enough neutrinos are detected from the
nuclear reactions in the Sun (Solar neutrino
problem) - Oscillations between different types of neutrinos
would solve the Solar neutrino problem - Oscillations also imply that neutrinos have a
small amount of mass
electron neutrino
muon neutrino
36Non-baryonic - axions
- Extremely light particles, with typical mass of
10-6 eV/c2 - Interactions are 1012 weaker than ordinary weak
interaction - Density would be 108 per cubic centimeter
- Velocities are low
- Axions may be detected when they convert to low
energy photons after passing through a strong
magnetic field
37Searching for axions
- Superconducting magnet to convert axions into
microwave photons - Cryogenically cooled microwave resonance chamber
- Cavity can be tuned to different frequencies
- Microwave signal amplified if seen
38Non-baryonic - WIMPs
- Weakly Interacting Massive Particles
- Predicted by Supersymmetry (SUSY) theories of
particle physics - Supersymmetry tries to unify the four forces of
physics by adding extra dimensions - WIMPs would have been easily detected in
acclerators if M lt 15 GeV/c2 - The lightest WIMPs would be stable, and could
still exist in the Universe, contributing most if
not all of the Dark Matter
39CDMS for WIMPs
- Cryogenic Dark Matter Search
- 6.4 million events studied - 13 possible
candidates for WIMPs - All are consistent with expected neutron flux
40Detecting WIMPs?
- Laboratory experiments - DAMA experiment 1400 m
underground at Gran Sasso Laboratory in Italy
announced the discovery of seasonal modulation
evidence for 52 GeV WIMPs - 100 kg of Sodium Iodide, operated for 4 years
- CDMS has 0.5 kg of Germanium, operated for 1
year, but claims better - background rejection techniques
- http//www.lngs.infn.it/
41HDM vs. CDM models
- Supercomputer models of the evolution of the
Universe show distinct differences - Rapid motion of HDM particles washes out small
scale structure the Universe would form from
the top down - CDM particles dont move very fast and clump to
form small structures first bottom up
42CDM models vs. density
- CDM models as a function of z (look-back time)
Largest structures are now just forming
Critical density
Low density
43Dark Matter and Dark Energy
- Assume that Wtotal 1, then for
- Ho 65 km s-1 Mpc-1, we measure
- Wb 0.04 (/- 0.001) (baryons)
- Wm 0.4 (/- 0.2) (all matter)
- 0.001 lt Wnlt 0.1 (hot dark matter)
- WL 0.6 0.7 (dark energy)
- This makes the age of the Universe around 15
billion years - http//www.physics.ucla.edu/dm20/talks/1a.pdf
- (Joel Primacks talk at DM2000)
44Dark Matter Activity 2
- You will search a paper plate galaxy for some
hidden mass by observing its effect on how the
galaxy rotates
In order to balance, the torques on both sides
must be equal T1 F1X1 F2X2 T2 where F1
m1g and F2 m2g
45Web Resources
- Astronomy picture of the Day http//antwrp.gsfc.na
sa.gov/apod/astropix.html - Imagine the Universe http//imagine.gsfc.nasa.gov
- Dark Matter 2000 (conference at UCLA)
http//www.physics.ucla.edu/dm20/ - Center for Particle Astrophysics
http//cfpa.berkeley.edu/ - Dark Matter telescope http//www.dmtelescope.org/d
arkmatter.html
46Web Resources
- Jonathan Dursis Dark Matter Tutorials Java
applets - http//www.astro.queensu.ca/dursi/dm-tutorial/dm0
.html - MACHO project http//wwwmacho.mcmaster.ca/
- National Center for Supercomputing Applications
http//www.ncsa.uiuc.edu/Cyberia/Cosmos/MystDarkMa
tter.html - Pete Newburys Gravitational Lens movies
http//www.iam.ubc.ca/newbury/lenses/research.htm
l
47Web Resources
- Alex Gary Markowitz Dark Matter Tutorial
http//www.astro.ucla.edu/agm/darkmtr.html - Martin Whites Dark Matter Models
- http//cfa-www.harvard.edu/mwhite/modelcmp.html
- Livermore Laboratory axion search
- http//www-phys.llnl.gov/N_Div/Axion/axion.html