Title: HI in Galaxies
1HI in Galaxies
Karen ONeil NRAO - GB
2Atmospheric opacity has governed our view onto
the sky
A Brief Introduction
3The most common transition of neutral
Hydrogen (HI) is at 21-cm (1420.4058 MHz)
A Brief Introduction
4The 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
-
5The 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
6The 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!
7The 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!
8So what?
What do you with do with it?
9Tracing the structureand star formation
potential in galaxies
10Tracing 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/
11Tracing 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/
12Tracing the structureand star formation
potential in galaxies
Neutral Hydrogen around Cass A
Image from CGPS www.ras.ucalgary.ca/CGPS/
13Tracing the structureand star formation
potential in galaxies
Atomic Hydrogen Mushroom Cloud
Image from CGPS www.ras.ucalgary.ca/CGPS/
14Tracing the structureand star formation
potential in galaxies
M101
15Tracing the structureand star formation
potential in galaxies
UGC 12695
16Tracing the structureand star formation
potential in galaxies
From the HI Rogues Gallery - http//www.nrao.edu/
astrores/HIrogues/
17Tracing the structureand star formation
potential in galaxies
From the HI Rogues Gallery - http//www.nrao.edu/
astrores/HIrogues/
18Tracing the structureand star formation
potential in galaxies
From the HI Rogues Gallery - http//www.nrao.edu/
astrores/HIrogues/
19Tracing the structureand star formation
potential in galaxies
and even discovering new galaxies!
Kilborn, et. Al 2000
20What else can you do?
21Obtaining rotation curves
22Obtaining rotation curves
If you know an objects velocity at a given
radius, you can determine the mass enclosed by
that radius.
23Obtaining rotation curves
24Obtaining rotation curves
Dark Matter
Gas
Stars
25What is Dark Matter?
Obtaining rotation curves
26An 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!!!
27What 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
28What 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
29What 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
30What is Dark Matter?
Obtaining rotation curves
Option 3 New particles/ Particle Physics
Gives lots of freedom in constraints No proof
available
31What 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
32What is Dark Matter?
Obtaining rotation curves
Option 4 MOND Modified Newtonian Dynamics
Fma
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.
33What 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
34Modified Newtonian Dynamics
Obtaining rotation curves
Smatter gt a0/G
Smatter lt a0/G
Sm lt a0/G
High Density Galaxies
Low Density Galaxies
35Without 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
36Modified 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
37Modified Newtonian Dynamics
Obtaining rotation curves
MOND and Newtonian fits to high and low density
galaxies
Sm lt a0/G
38Modified Newtonian Dynamics
Obtaining rotation curves
Sm lt a0/G
MOND accurately predicts rotation curves
observed for high and low density galaxies!!!
39Modified 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
40Modified 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
41Using a Single Dish Telescope
One last thought..
42Using 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)
43Images Pixels
44Images Pixels
45Images Pixels
46Using 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
47Using a single dish telescope
More than one telescope (e.g. VLA)
One telescope (e.g. GBT)
48Using a single dish telescope
Determining the Distribution
49Using 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
50The End