Professor Lynn Cominsky - PowerPoint PPT Presentation

1 / 47
About This Presentation
Title:

Professor Lynn Cominsky

Description:

Composition of the Cosmos. March 25, 2003. Lynn Cominsky - Cosmology ... National Center for Supercomputing Applications http://www.ncsa.uiuc.edu/Cyberia/Cosmos ... – PowerPoint PPT presentation

Number of Views:56
Avg rating:3.0/5.0
Slides: 48
Provided by: LynnCo2
Category:

less

Transcript and Presenter's Notes

Title: Professor Lynn Cominsky


1
Astronomy 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

2
Group 8
  • Robert Angeli
  • Jacy Maka
  • Ryan McDaniel
  • Rena Morabe

Let's hear it for Group 8!
3
Composition of the Cosmos
4
Keplers Third Law movie
  • P2 is proportional to a3

5
Dark 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.
6
Virial 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

7
Galaxy 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!
8
Dark 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

9
Hot 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!

10
Dark 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

11
Types 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)

12
Big Bang
  • Written, directed and starring the Physics
    Chanteuse Lynda Williams
  • From her CD Cosmic Cabaret
  • Available from www.scientainment.com

13
Primordial 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
14
Primordial 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!

15
Baryonic 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

16
Baryonic - Brown Dwarfs
  • Mass around 0.08 Mo
  • Do not undergo nuclear burning in cores
  • First brown dwarf star Gliese 229B

17
Baryonic - 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

18
Ghost 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

19
Baryonic 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!

20
Baryonic 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

21
Gravitational Microlensing
  • Scale not large enough to form two separate images

movie
22
Baryonic 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

23
Black 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..

24
Strong Gravitational Lensing
25
Strong Gravitational Lensing
  • HST image of background blue galaxies lensed by
    orange galaxies in a cluster
  • Einsteins rings can be formed for the correct
    alignment

26
Strong Gravitational Lensing
  • Spherical lens
  • Perfect alignment
  • Note formation of Einsteins rings

27
Strong Gravitational Lensing
  • Elliptical lens
  • Einsteins rings break up into arcs if you can
    only see the brightest parts

28
Dark 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

29
Gravitational 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

30
Gravitational 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

31
Baryonic 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

32
Baryonic dust
  • Dust is made of elements heavier than Helium,
    which were previously produced by stars (lt2 of
    total)
  • Dust absorbs and reradiates background light

33
Non-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
34
Neutrino 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

35
Neutrino 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
36
Non-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

37
Searching 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

38
Non-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

39
CDMS for WIMPs
  • Cryogenic Dark Matter Search
  • 6.4 million events studied - 13 possible
    candidates for WIMPs
  • All are consistent with expected neutron flux

40
Detecting 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/

41
HDM 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

42
CDM models vs. density
  • CDM models as a function of z (look-back time)

Largest structures are now just forming
Critical density
Low density
43
Dark 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)

44
Dark 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
45
Web 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

46
Web 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

47
Web 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
Write a Comment
User Comments (0)
About PowerShow.com