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HI in Galaxies

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A hyperfine transition is one that takes. place due to a change in the spin of an electron ... Neutral particles (uncharged) Very light, but containing mass ... – PowerPoint PPT presentation

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Title: HI in Galaxies


1
HI in Galaxies
Karen ONeil NRAO - GB
2
Atmospheric opacity has governed our view onto
the sky
A Brief Introduction
3
The most common transition of neutral
Hydrogen (HI) is at 21-cm (1420.4058 MHz)
A Brief Introduction
4
The most common transition of neutral
Hydrogen (HI) is at 21-cm (1420.4058 MHz)
A Brief Introduction
  • Hyperfine transition (forbidden)
  • Hyperfine transition (forbidden)
  • Decay half-life of 12 million years

5
The most common transition of neutral
Hydrogen (HI) is at 21-cm (1420.4058 MHz)
A Brief Introduction
1950 Ewen Purcell announced the first
discovery of HI!
Ed Purcell Taffy Bowen Doc Ewen
6
The most common transition of neutral
Hydrogen (HI) is at 21-cm (1420.4058 MHz)
A Brief Introduction
  • Detection of HI should be virtually impossible
  • 1950 Ewen Purcell announced detection of HI!

7
The most common transition of neutral
Hydrogen (HI) is at 21-cm (1420.4058 MHz)
A Brief Introduction
Atmosphere is (mostly) transparent at 1420 MHz
Galaxies typically have lots of HI
21-cm HI emission is (relatively) easy to study!
8
So what?
What do you with do with it?
9
Tracing the structureand star formation
potential in galaxies
10
Tracing the structureand star formation
potential in galaxies
The midplane of the Milky Way Galaxy near the
constellation Perseus.
Image from CGPS www.ras.ucalgary.ca/CGPS/
11
Tracing the structureand star formation
potential in galaxies
GSH138-01-094 An Expanding Shell in the Milky
Way Galaxy
Image from CGPS www.ras.ucalgary.ca/CGPS/
12
Tracing the structureand star formation
potential in galaxies
Neutral Hydrogen around Cass A
Image from CGPS www.ras.ucalgary.ca/CGPS/
13
Tracing the structureand star formation
potential in galaxies
Atomic Hydrogen Mushroom Cloud
Image from CGPS www.ras.ucalgary.ca/CGPS/
14
Tracing the structureand star formation
potential in galaxies
M101
15
Tracing the structureand star formation
potential in galaxies
UGC 12695
16
Tracing the structureand star formation
potential in galaxies
From the HI Rogues Gallery - http//www.nrao.edu/
astrores/HIrogues/
17
Tracing the structureand star formation
potential in galaxies
From the HI Rogues Gallery - http//www.nrao.edu/
astrores/HIrogues/
18
Tracing the structureand star formation
potential in galaxies
From the HI Rogues Gallery - http//www.nrao.edu/
astrores/HIrogues/
19
Tracing the structureand star formation
potential in galaxies
and even discovering new galaxies!
Kilborn, et. Al 2000
20
What else can you do?
21
Obtaining rotation curves
22
Obtaining rotation curves
If you know an objects velocity at a given
radius, you can determine the mass enclosed by
that radius.
23
Obtaining rotation curves
24
Obtaining rotation curves
Dark Matter
Gas
Stars
25
What is Dark Matter?
Obtaining rotation curves
26
An AsideDark Matter and Missing Mass
Obtaining rotation curves
  • Nucleosynthesis Big Bang predictions 60-80
    of the predicted baryonic matter in
  • the universe is not visible
  • Assuming Newton Einstein are right,
  • gravitational constraints
  • An additional 90 of non-baryonic matter
  • is not visible
  • Result
  • What we actually study is only 2-4 of the
  • stuff in the Universe!!!

27
What is Dark Matter?
Obtaining rotation curves
Option 1 - Baryons
Recall that baryons are the stuff of everyday
life protons and neutrons
In fact, baryons are the heavyweight particle,
each having 3 quarks, and includes p,n,?, ?,S,
O,L
28
What is Dark Matter?
Obtaining rotation curves
Option 1 - Baryons
Possibilities include
  • Cold molecular gas in the form of dense clumps
  • T3K, d1024 cm-2,D30 A.U., M10-3Msun
  • Stellar remnants, brown/low mass stars dwarfs,
  • black holes

Problems
  • No evidence for sufficient quantities

29
What is Dark Matter?
Obtaining rotation curves
Option 2 Supersymmetric particles
Neutralinos, gravitinos, axinos
  • Neutral particles (uncharged)
  • Very light, but containing mass
  • Made up of neutrons, gravitons, or axions
  • Created in the early Universe

Problems
  • Extremely difficult to detect
  • Existence not yet proven

30
What is Dark Matter?
Obtaining rotation curves
Option 3 New particles/ Particle Physics
Gives lots of freedom in constraints No proof
available
31
What is Dark Matter?
Obtaining rotation curves
Option 4 MOND Modified Newtonian Dynamics
  • Current version proposed by Milgrom, 1983
  • (but originally seen back in the 1950s)
  • Attempts to bypass the need for dark matter in
  • galaxies galaxy clusters

32
What is Dark Matter?
Obtaining rotation curves
Option 4 MOND Modified Newtonian Dynamics
  • Newtonian Physics

Fma
  • MOND

Fma f(a/a0) a0constant f(x) 1 if xgtgt1 f(x)
x if xltlt1
gn g f(g/a0) In low acceleration g
v(gna0) v4 GMa0
MOND changes the force of gravity only when
acceleration (density) is low.
33
What is Dark Matter?
Obtaining rotation curves
Option 4 MOND Modified Newtonian Dynamics
MOND Surface-Density Prediction
  • At high density (Smatter gt a0/G ) Newtonian
    Physics dominates
  • At low density (Smatter lt a0/G ) MOND dominates

34
Modified Newtonian Dynamics
Obtaining rotation curves
Smatter gt a0/G
Smatter lt a0/G
Sm lt a0/G
High Density Galaxies
Low Density Galaxies
35
Without MOND
Obtaining rotation curves
Smatter gt a0/G
Smatter lt a0/G
Sm lt a0/G
High Density Galaxies
Low Density Galaxies
NGC 2903
DM
gas
stars
36
Modified Newtonian Dynamics
Obtaining rotation curves
Smatter gt a0/G
Smatter lt a0/G
Sm lt a0/G
High Density Galaxies
Low Density Galaxies
NGC 2903
MOND
stars
gas
a01.2X10-8 cm/s2
37
Modified Newtonian Dynamics
Obtaining rotation curves
MOND and Newtonian fits to high and low density
galaxies
Sm lt a0/G
38
Modified Newtonian Dynamics
Obtaining rotation curves
Sm lt a0/G
MOND accurately predicts rotation curves
observed for high and low density galaxies!!!
39
Modified Newtonian Dynamics
Obtaining rotation curves
Sm lt a0/G
Should we toss out Newton and embrace MOND?
  • YES!
  • Accurate prediction of many rotation curves
  • Eliminates need for mysterious Dark Matter in
    galaxies
  • Also explains surface density limits in galaxies
  • formation of bars in HSB galaxies
  • NO!
  • Needless change in fundamental physics
  • Does not work 100 of the time

40
Modified Newtonian Dynamics
Obtaining rotation curves
Why should we continue to investigate MOND?
  • At this point, we still do not know what the
    mysterious
  • Dark Matter (or Dark Force) is
  • Understanding when and why MOND works for
    galaxies
  • can give us considerable insight into Dark
    Matter
  • Trial and error technique is how many scientific
    theories
  • are realized

41
Using a Single Dish Telescope
One last thought..
42
Using a single dish telescope
  • Results shown have information on radius vs.
    HI/velocity
  • This requires imaging of galaxies (more than 1
    pixel)
  • GBT is only one telescope (one pixel)

43
Images Pixels
44
Images Pixels
45
Images Pixels
46
Using a single dish telescope
  • Results shown have information on radius vs.
    HI/velocity
  • This requires imaging of galaxies (more than 1
    pixel)
  • GBT is only one telescope (one pixel)
  • Can we use the GBT to study galaxy structure and
    DM
  • in galaxies smaller than the beam?

YES
47
Using a single dish telescope
More than one telescope (e.g. VLA)
One telescope (e.g. GBT)
48
Using a single dish telescope
Determining the Distribution
49
Using a single dish telescope
Determining the Dark Matter Content
W202vrot
  • Measure vrotation
  • Assume a radius for gas
  • Determine Mdynamical
  • Measure Mgas
  • Determine Mdark matter

Less accurate, but it takes (far!) less
telescope time for higher sensitivity
50
The End
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