Title: The Rotation Curve and Velocity Dispersions of Dwarf Galaxies
1The Rotation Curve and Velocity Dispersions of
Dwarf Galaxies
- Lei Hao
- Apr, 25th, 2007
- Astro 620 Advanced Radio Astronomy
2Introduction
- Probe the mass distribution
- Dark Matter content
- Dynamics, evolution and formation of galaxies
3Kinematics -- Observations
- Using optical spectroscopy (star and gas)
- Traditional long-slit spectra
- Fabry-Perot spectrographs and IFU velocity
information for the whole field, but time
consuming - Emission lines H?, NII, SII
- Distant planetary nebulae and satellite galaxies
(large distances) - Individual HII regions (e.g. Rubin Ford, 1970,
83)
4Kinematics -- Observations
- HI line
- Advantage Extends further out than the visible
disk - Disadvantage not good in the central region
poor spatial resolution of the beam - CO line
- Good alternative to H? and HI in the inner disk,
less extinction - Maser Lines SiO, OH, H2O
- Super-massive BH in the center of NGC4258.
5Kinematics of Dwarfs
- Optical (H? and star) and HI
- Pressure-supported systems velocity dispersion
- Rotationally-supported systems rotation velocity
- Methods to measure rotation curve tilted-ring
model (Begeman 1989) - The galaxy can be described by a set of
concentric rings, each ring being characterized
by a fixed value of the HI surface density and
circular velocity, and the inclination angle and
position angle of the major axis. - Fit with the observed velocity along the major
axis.
6Kinematics -- Observations
- Rotation Curve in typical disk galaxies
- Rise rapidly in the central regions and often
reach 200-300km/s within a few hundred parsecs
of the center. - HI disk stay flat until the last point measured ?
dark matter (exceptions exists) - The shape of the RC correlates with the optical
luminosities - Low-luminosity slowly rising and low amplitude
- High-luminosity fast rising and high amplitude
7Kinematics -- Observations
8Kinematics of Dwarfs
- Dwarf galaxies are dark matter dominated. (Mateo
1989) - For a given M/L, the central velocity dispersion
of a self-gravitating system in equilibrium,
scales as (RcS0)1/2 - Globular clusters have central velocity
dispersions of 2-15km/s - Pressure supported dwarf galaxies have Rc 10
times larger, and S0 103times smaller ? vlt2 km/s - All low-luminosity dwarfs have velocity
dispersions of gt7km/s
9Rotation Curves of Dwarfs
- Dwarf spiral galaxies provide excellent probes of
the internal structure of dark haloes. - Dark matter dominate on scales larger than a
kiloparsec - Easy to take out the baryonic mass which is
mostly in the form of HI within the disk. - Early results show slow rotation, with rotation
curves that rise monotonically to the last
measure points.
10Rotation Curves of Dwarfs
- Dwarf spiral galaxies provide excellent probes of
the internal structure of dark haloes. - Dark matter dominate on scales larger than a
kiloparsec - Easy to take the baryonic mass which is mostly in
the form of HI within the disk.
Moore 1994
11Rotation Curves of Dwarfs
- Core or cusp
- Simulation predict the inner part slope of the
mass density ? -1 (Navarro et al. 1997, Power at
al. 2003, Colin et al. 2004) ? -1.2-1.5 (Moore
et al. 1999, Ghigna et al. 2000 klypin et al.
2001 Reed et al. 2003 Tasitsiomi et al. 2004) - Observations ?-0.2 (de Blok et al. 2001a)
12Rotation Curves of Dwarfs-- Uncertainties
- De Blok, Mcgaugh et al. ? HI RC of dwarf galaxies
are in contradiction with the CDM predictions. - Swaters, van den Bosch et al. ? RC of dwarf
galaxies are consistent with cosmological
predictions - Beam smearing, uncertain mass-to-light ratio,
limited spatial sampling of halos density
distribution - Ask for higher resolution, and independent M/L
ratio
13Rotation Curves of Dwarfs-- Uncertainties
- De Blok, Mcgaugh et al. ? RC of dwarf galaxies
are in contradiction with the CDM predictions. - Swaters, van den Bosch et al. ? RC of dwarf
galaxies are consistent with cosmological
predictions - Beam smearing, uncertain mass-to-light ratio,
limited spatial sampling of halos density
distribution - Ask for higher resolution, and independent M/L
ratio
Sofue Rubin 2001
14Rotation Curves of Dwarfs-- Uncertainties
- De Blok, Mcgaugh et al. ? RC of dwarf galaxies
are in contradiction with the CDM predictions. - Swaters, van den Bosch et al. ? RC of dwarf
galaxies are consistent with cosmological
predictions - Beam smearing, uncertain mass-to-light ratio,
limited spatial sampling of halos density
distribution - Ask for higher resolution, and independent M/L
ratio
Swaters et al. 2000
15Rotation Curves of Dwarfs-- Uncertainties
- De Blok, Mcgaugh et al. ? RC of dwarf galaxies
are in contradiction with the CDM predictions. - Swaters, van den Bosch et al. ? RC of dwarf
galaxies are consistent with cosmological
predictions - Beam smearing, uncertain mass-to-light ratio,
limited spatial sampling of halos density
distribution - Ask for higher resolution, and independent M/L
ratio
Swaters et al. 2000
16Rotation Curves of Dwarfs-- Uncertainties
- De Blok, Mcgaugh et al. ? RC of dwarf galaxies
are in contradiction with the CDM predictions. - Swaters, van den Bosch et al. ? RC of dwarf
galaxies are consistent with cosmological
predictions - Beam smearing, uncertain mass-to-light ratio,
limited spatial sampling of halos density
distribution - Ask for higher resolution, and independent M/L
ratio - Mcgaugh et al. 2001 with higher resolution H?
data for inner region ? similar RC as before,
still in contradiction with the CDM predictions - Rhee et al. 2004 ? many systematic biases to
consider. Each bias can be small, but all add up
to produce significant effects. (Inclination
bar bulge) titled-ring model produces an
underestimate of the central rotational
velocities. (typically 20)
17Rotation Curves of Dwarfs-- exceptions
Carignan Puche 1990
18Rotation Curves of Dwarfs-- exceptions
Ostlin et al. 1999 RC for BCDs
19Velocity Dispersion of Dwarfs
- How low-mass dwarf galaxies supported
- Rotation velocities become comparable to
disordered motions (intrinsic gas dispersions,
bulk motions by SN and stellar winds) - A 107-108M? galaxy with a radius 2kpc has
circular rotation speed of 5-15km/s, while warm
diffuse HI gas with T6000K has velocity
dispersion of 7km/s. - DsphdIrr LGS3 and Phoenix
- Optically similar to dwarf spheroidals
- Retain a substantial amount of interstellar gas
20Velocity Dispersion of Dwarfs
- Young Lo 1997
- HI studies of Sag DIG (dIrr), LGS3 (dIrr/dsph)
and phoenix (dIrr/dsph) - Sag DIG and LGS3 have extended HI, phoenix
unsure. - They are random motion supported. (only within
local group do we have dIrr that are not rotation
supported)
21Velocity Dispersion of Dwarfs
- Young Lo 1997
- HI studies of Sag DIG (dIrr), LGS3 (dIrr/dsph)
and phoenix (dIrr/dsph) - Sag DIG and LGS3 have extended HI, phoenix
unsure. - They are random motion supported. (only within
local group do we have dIrr that are not rotation
supported)
22Velocity Dispersion of Dwarfs
- Young Lo 1997
- HI studies of Sag DIG (dIrr), LGS3 (dIrr/dsph)
and phoenix (dIrr/dsph) - Sag DIG and LGS3 have extended HI, phoenix
unsure. - They are random motion supported. (only within
local group do we have dIrr that are not rotation
supported) - Sag DIG is decomposed into broad (?10km/s) and
narrow (?5km/s) components. Broad component
distributed throughout the galaxy and the narrow
component concentrated into a small number of
prominent clumps.
23Velocity Dispersion of Dwarfs
- Young Lo 1997
- HI studies of Sag DIG (dIrr), LGS3 (dIrr/dsph)
and phoenix (dIrr/dsph) - Sag DIG and LGS3 have extended HI, phoenix
unsure. - They are random motion supported. (only within
local group do we have dIrr that are not rotation
supported) - Sag DIG is decomposed into broad (?10km/s) and
narrow (?5km/s) components. Broad component
distributed throughout the galaxy and the narrow
component concentrated into a small number of
prominent clumps.
24Velocity Dispersion of Dwarfs
- Young Lo 1997
- HI studies of Sag DIG (dIrr), LGS3 (dIrr/dsph)
and phoenix (dIrr/dsph) - Sag DIG and LGS3 have extended HI, phoenix
unsure. - They are random motion supported. (only within
local group do we have dIrr that are not rotation
supported) - Sag DIG is decomposed into broad (?10km/s) and
narrow (?5km/s) components. Broad component
distributed throughout the galaxy and the narrow
component concentrated into a small number of
prominent clumps. - LGS3 do not have narrow component the lack of
cold component may be the reason for the lack of
starformation in LGS3
25Velocity Dispersion of Dwarfs
- Young Lo 1997
- HI studies of Sag DIG (dIrr), LGS3 (dIrr/dsph)
and phoenix (dIrr/dsph) - Sag DIG and LGS3 have extended HI, phoenix
unsure. - They are random motion supported. (only within
local group do we have dIrr that are not rotation
supported) - Sag DIG is decomposed into broad (?10km/s) and
narrow (?5km/s) components. Broad component
distributed throughout the galaxy and the narrow
component concentrated into a small number of
prominent clumps. - LGS3 do not have narrow component the lack of
cold component may be the reason for the lack of
starformation in LGS3
26References
- Sofue Rubin ARAA, 2001, 39, 137
- Rhee et al. 2004, ApJ, 617, 1059
- Young Lo, 1997, ApJ, 490, 710
- Moore, 1994, Nature, 370, 629
- Noordermeer, et al. 2007, MNRAS,/0701731
- McGaugh et al. 2001, AJ, 122, 2381
- Begeman 1989, AA, 223, 47
- Swaters et al 2000, ApJ, 531, 107
- De Blok McGaugh 1997 MNRAS, 290, 533