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The Rotation Curve and Velocity Dispersions of Dwarf Galaxies

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Title: The Rotation Curve and Velocity Dispersions of Dwarf Galaxies


1
The Rotation Curve and Velocity Dispersions of
Dwarf Galaxies
  • Lei Hao
  • Apr, 25th, 2007
  • Astro 620 Advanced Radio Astronomy

2
Introduction
  • Probe the mass distribution
  • Dark Matter content
  • Dynamics, evolution and formation of galaxies

3
Kinematics -- 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)

4
Kinematics -- 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.

5
Kinematics 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.

6
Kinematics -- 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

7
Kinematics -- Observations
8
Kinematics 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

9
Rotation 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.

10
Rotation 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
11
Rotation 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)

12
Rotation 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

13
Rotation 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
14
Rotation 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
15
Rotation 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
16
Rotation 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)

17
Rotation Curves of Dwarfs-- exceptions
Carignan Puche 1990
18
Rotation Curves of Dwarfs-- exceptions
Ostlin et al. 1999 RC for BCDs
19
Velocity 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

20
Velocity 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)

21
Velocity 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)

22
Velocity 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.

23
Velocity 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.

24
Velocity 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

25
Velocity 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

26
References
  • 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
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