the halo of the milky
DESCRIPTION
The Halo of the Milky. Heidi Jo Newberg Rensselaer Polytechnic Institute. In search of a halo model that fits the data. Brief background on the stellar Milky Way We tried to measure the halo shape and found the Sagittarius dwarf tidal stream. - PowerPoint PPT PresentationTRANSCRIPT
In search of a halo model that fits the data
Brief background on the stellar Milky WayWe tried to measure the halo shape and found
the Sagittarius dwarf tidal stream.We improved our technique and found
another tidal stream.Argument that the spheroid is triaxialChi-squared triaxial spheroid fits to the data
and the problem with lumps.
The Standard Galactic ModelRadial scale length (kpc)
0.22.94-53.5-52-3
BulgeSpheroidThick DiskThin DiskDark Halo
Vertical scale height or c/a
0.40.6-11.3 kpc325 pc1?
Density near Sun (Msol/pc3)
0.000260.0260.1240.009
Metallicity [Fe/H]
0.3-1.5-0.6-0.1
Vrot at Rsol (km/s)
0-501802200?
Allen’s Astrophysical Quantities, 2000
The first attempt to measure the shape of the Galactic halo
using the Sloan Digital Sky Survey
It was 1998. We had the first scan of data from the Sloan Digital Sky Survey. I had been writing software for 6 years.
Brian Yanny and I thought we would try to measure the flattening parameter of the Galactic spheroid:
222 )/(,5.3, qzyxrr
Yanny et al. 2000L
og(l
umin
osit
y in
wav
elen
gth
rang
e of
g f
ilte
r)
Log(ratio of lum. in λ range of g filter to lum. in λ range of r filter)
A tremendous number of papers exist studying the Sgr dwarf tidal stream
Measurements of density, position, and stellar velocities of stream stars.
Models of dwarf disruption, that depend on the Galactic potential (various papers claim that q=1, q>1, q<1)
Models that show the Sgr dwarf interacted with the LMC several billion years ago, which threw it into this destructive orbit.
Possibility that the Sgr dwarf tidal stream goes through the solar position, and that it could contribute ~1% to the dark matter density at the Earth.
Theoretical limits on the lumpiness of the Galactic dark matter halo.
Claim that a Galactic globular cluster was stripped from the Sgr dwarf and is currently in the tidal stream.
Current controversiesTurf war over name: Monoceros stream, stream in the Galactic
plane, Galactic Anticenter Stellar Structure (GASS), One Ring or “Ring,” Canis Major dwarf galaxy, Argo structure.
Is the entire structure due to the Galactic warp?How many times does the stream wrap the Galaxy?Has the Canis Major dwarf galaxy been discovered, and is it the
progenitor of the tidal stream?Did this merger puff up, or even create the Galactic thick disk?Is it related to the “metal-weak thick disk?”Is the purported Canis Major dwarf galaxy really an artifact of the
Galactic warp?Is the purported Canis Major structure really an artifact of a hole
in the Galactic extinction – and the real center of the structure in the Argo Navis Constellation?
Is the Argo structure the Galactic warp?
Density of spheroid stars in Galactic coordinates from DR3
Galactic longitude
Gal
actic
latit
ude
1,857,142 stars
θgLong
For close stars, the maximum density is in quadrant IV and the minimum is is quadrant II.
For distances larger than the Sun-GC dist., the max. is in quadrant I and the min. is in quadrant II.
For large distances, the minimum is perpendicular to the major axis of the spheroid.
Finding a modelNo model of the commonly
used form will work.
The triaxial power law still puts too many stars in the Galactic center.
The Hernquist profile fits better, but leaves excess counts in the south.
222 )/(,1
qzyxrr
222 )/()/(,1
qzpyxrr
2223
)/()/(,)(
1qzpyxr
Rrr core
).,,( angles by the rotated then and center, Galactic thefrom
by shifted are axes thewhere
)/'()/'(',)(
1 222
z)(dx, dy, d')(x', y', z
qzpyxrRrr core
Minimum Chi-squared modelFull model
R0 8.0 kpcp 0.73q 0.67θ 48°Rcore 15.0 kpcdx 0.1 kpcdy 3.5 kpcdz 0.1 kpcφ -8.0°ξ 12°α 1δ 3Mf 4.2Nsolar 1081 kpc-3
χ2 1.37
Minimum Chi-squared model
Full model GC power law GC power law standard model
R0 8.0 kpc 8.5 kpc 8.0 kpc 8.5 kpc 10.7 kpcp 0.73 0.73 0.74 0.72 1.0q 0.67 0.60 0.66 0.59 0.63θ 48° 70 52 72 -Rcore 15.0 kpc 14.0 kpc - - -dx 0.1 kpc - 0.2 kpc - -dy 3.5 kpc - 3.0 kpc - -dz 0.1 kpc - 0.0 kpc - -φ -8.0° -4.5 -6.5 -4.0 -ξ 12° 14 16 14 -α 1 1 2.9 3.0 3.1δ 3 3 0 0 0Mf 4.2 4.2 4.2 4.2 4.2Nsolar 1081 kpc-3 1096 kpc-3 1412 kpc-3 1341 kpc-3 1539 kpc-3
χ2 1.37 1.42 1.49 1.51 1.92
Local density of stellar halo
0.00026 Msol/pc3 (Allen’s Astrophysical Quantities, 2000)
1100-1500 F stars/kpc3 at the solar position (this talk)
In Pal 5, the ratio Msol/F stars ~ 5, therefore, we estimate a local density of:
5.5x10-6-7.5x10-6 Msol/pc3
(30-50 times smaller than Allen)
Conclusions
A large part of the Galactic halo is inhabited by lumps and tidal streams with size scales of the order of 10 kpc.
The smoothest component we can find is biased towards a non-axisymmetric shape and a Hernquist rather than a power-law profile.
One cannot measure q from a pencil-beam survey or even a strip of the sky 100 degrees long.
SEGUE as of September 30, 2004 Black= completed stripe or plate pair
Imaging: 3900 sq deg, mostly low |b|; 750/3900 sq deg 19% complete Spectra: 240,000 stellar spectra; 29/400 plates 7% complete (17K stars)