Finding Galactic- halo substructure in the Gaia data Amina Helmi - - PowerPoint PPT Presentation
Finding Galactic- halo substructure in the Gaia data Amina Helmi - - PowerPoint PPT Presentation
Finding Galactic- halo substructure in the Gaia data Amina Helmi Stellar halo: treasure trove of merger relics t = 1 Gyr t = 2 Gyr Cosmological models characteristic: hierarchical growth: mergers Disrupted galaxies/debris naturally in a
t = 1 Gyr t = 2 Gyr t = 3 Gyr t = 4.5 Gyr t = 8 Gyr t = Tnow
today
snapshots: J. Gardner
Stellar halo: treasure trove of merger relics
- Cosmological model’s characteristic: hierarchical
growth: mergers
- Disrupted galaxies/debris naturally in a stellar halo:
!merger signatures: Substructures and tidal streams
- Questions:
- Were mergers important for galaxies like MW?
- How often and when did they happen?
- What were the building blocks?
- Stars are “fossils”
- Motions, ages, chemical composition trace origin
- Substructures pinpoint to merger debris
- Probe force field ! mass (gravity)
Testing the cold dark matter paradigm
Is this “picture” correct?
- Are galaxies like the Milky Way and its nearest neighbours embedded in dark matter halos like
those predicted by the cosmological model?
Credit: V. Springel
Testing the cold dark matter paradigm
Is this “picture” correct?
- Are galaxies like the Milky Way and its nearest neighbours embedded in dark matter halos like
those predicted by the cosmological model?
Testing the cold dark matter paradigm
Is this “picture” correct?
- Are galaxies like the Milky Way and its nearest neighbours embedded in dark matter halos like
those predicted by the cosmological model?
- How much dark matter is there?
– how is it distributed? – what is the dark matter?
- Is Gravity correct?
Credit: V. Springel
A stream in a dark halo with substructure
Granularity: Hundreds of thousands dark clumps if dark matter particle is cold Springel et al. 2008
Belokurov et al. 2006 +
Outer halo: R > 20 kpc
- Clear evidence of substructure
- Limited to high-surface brightness features
(progenitors/time of events)
- Qualitatively consistent with expectations from
ΛCDM (Helmi et al. 2011; Deason et al. 2014)
North Galac?c Cap
Galac?c An?centre
Slater et al. 2014+
The accretion history unveiled so far:
The Galactic halo from SDSS/PanStarrs
PanSTARRS 3π survey
Many narrow streams mapped/discovered. Bernard et al. (2016)
The relevance of kinema?c informa?on
The relevance of kinema?c informa?on
Proper motions from Gaia DR2 (April 2018)
vt=200 km/s ! μ~1 – 5 mas/yr (d ~ 10 – 40 kpc) expected error: σμ ~ 0.1mas/yr (G ~ 17)
! Trace substructures, outlier removal, and map MW potential
Not all substructure is accreted – does pinpoint to interactions and mergers
Li et al 2017 Price-Whelan et al 2015 Deason et al 2014
Gomez et al. (2016, 2017)
angular momentum energy
conserved quantities
Nearby halo
Memory of origin: retained in the motions
" 100s of streams should cross Sun’s vicinity " So far.. not much evidence (small samples) " How to find more? ! Clustering in conserved quantities
Helmi & de Zeeuw 2000
https://www.astro.rug.nl/~ahelmi/research/gaia/movie.html
Construction of a halo sample: TGAS x RAVE
- TGAS dataset is significant improvement, but need full
phase-space information ! cross-match to RAVE survey
- RAVE: spectra for 500k stars in southern sky: vlos, [M/H],
spectrophotometric distance/parallax
(with TGAS priors, McMillan et al. 2017)
! ~ 200,000 stars in common
- Metallicity cut [M/H]cal < -1 dex
to select preferentially halo
- Remove stars with disk-like
kinematics
- 2-Gaussian decomposition
! sample of 1307 genuine halo stars
−600 −400 −200 200 400 600
vx (km/s)
−600 −400 −200 200 400 600
vy (km/s)
−600 −400 −200 200 400 600
vz (km/s)
−600 −400 −200 200 400 600
vy (km/s)
Maarten Breddels Jovan Veljanoski
Helmi, Veljanoski, Breddels et al. (2017), Veljanoski et al. (in prep)
Statistical tests and searches of substructure
Models predict
- several hundred moving groups or
streams in Solar Neighbourhood ! we search for excess clustering in velocity space with a correlation function
- substructure to be more easily apparent
in Integrals of Motion space ! we characterise the distribution, degree of clustering and establish significance
20 10 10 20
100 200 300 400 500 600 700
velocity difference |vi − vj| (km/s)
0.8 0.9 1.0 1.1 1.2 1.3 1.4 1.5
1+<ξ>
Velocity correlation function
- Very significant excess of pairs in data compared to random/smooth
– for Δ < 20 km/s, 5.5σ (120 pairs of stars in excess) – for 20 < Δ < 40 km/s: 8.8σ (328 pairs in excess)
- Also for very large separations, there is a significant excess
Helmi et al. (2017) Helmi, Veljanoski et al. (2017)
The amount of substructure: comparison to cosmological simulations
- Simulations of halos purely built via accretion show excess on small and large separations
- f similar amplitude
– some variation from halo to halo ! Milky Way halo consistent with being fully built via accretion
Cooper et al. (2010)
Helmi et al. (2017)
−4000 −3000 −2000 −1000 1000 2000 3000 4000
Lz (km/s kpc)
−200000 −175000 −150000 −125000 −100000 −75000 −50000 −25000
E (km2/s2)
! very retrograde motions: 73% of all stars (for E > -1.3x105 km2/s2)
In randomised (re-shuffled) smooth distributions the probability of having so many loosely bound
counter-rotating stars is < 0.1% retrograde less-bound
Helmi, Veljanoski et al. (2017)
Integrals of motion - space
Integrals of motion – space
- Statistical comparison to smooth
distributions allows identification of
- verdensities in E vs Lz
- Structures at Lz ~-500 km/s kpc
could be related to OmegaCen debris (Dinescu 2002)
- VelHel-6: stars with disk-like
kinematics but counter-rotating
−3 −2 −1 1 2 3 scaled Lz −10 −9 −8 −7 −6 scaled E
3 6 7 9 13 14 18 21
−200000 −180000 −160000 −140000 −120000 −100000 E (km2/s2) −2000 −1000 1000 2000 Lz (km/s kpc)
Helmi, Veljanoski, Breddels et al. (2017), Veljanoski et al. (in prep)
see also Myuoung et al. (2017)
The retrograde halo in context
- Not common in cosmological
simulations
(e.g. Illustris; Vogelsberger et al. 2014)
- Less than 1% of MW-mass
galaxies have more than 60% of the less bound stars on retrograde orbits (here defined as r > 15 kpc)
Helmi et al. (2017)
Chemical abundances
Helmi et al. (2017)
- C. Boeche chemical pipeline, not all stars have detailed abundances (SNR > 20, McMillan sample)
- Stars with Lz < 0 on average lower metallicity, both [M/H] and [Fe/H]
- May be some clumpiness (?)
−2000 −1000 1000 2000
Lz (km/s kpc)
−210000 −200000 −190000 −180000 −170000 −160000 −150000 −140000 −130000
E (km2/s2)
−2.4 −2.2 −2.0 −1.8 −1.6 −1.4 −1.2 −1.0 −0.8
[Fe/H] (dex)
−4000 −3000 −2000 −1000 1000 2000
Lz (km/s kpc)
−200000 −175000 −150000 −125000 −100000 −75000 −50000 −25000
E (km2/s2)
−2.4 −2.2 −2.0 −1.8 −1.6 −1.4 −1.2 −1.0 −0.8
[M/H] (dex) Veljanoski (in prep)
Chemical abundances: substructures
Helmi et al. (2017)
−1.0 −0.5 0.0 0.5 1.0
[Mg/Fe] (dex)
Retrograde halo Stars not in substructures Substructure 3 Substructure 6 Substructure 7
−3 −2 −1
[Fe] (dex)
−1.0 −0.5 0.0 0.5 1.0
[Mg/Fe] (dex)
Substructure 9
−3 −2 −1
[Fe] (dex)
Substructure 13
−3 −2 −1
[Fe] (dex)
Substructure 14
−3 −2 −1
[Fe] (dex)
Substructure 18
−3 −2 −1
[Fe] (dex)
Substructure 21 2 4 6 8
Number of stars
Retrograde halo
20 40 60 80 100
Stars not in substructures
2 4 6 8
Substructure 3
0.0 0.5 1.0 1.5 2.0 2.5 3.0
Substructure 6
1 2 3 4 5 6
Substructure 7
−2 −1
[Fe/H] (dex)
1 2 3 4 5 6
Number of stars
Substructure 9
−2 −1
[Fe/H] (dex)
0.0 0.5 1.0 1.5 2.0 2.5 3.0
Substructure 13
−2 −1
[Fe/H] (dex)
1 2 3 4 5 6
Substructure 14
−2 −1
[Fe/H] (dex)
0.0 0.5 1.0 1.5 2.0
Substructure 18
−2 −1
[Fe/H] (dex)
0.0 0.2 0.4 0.6 0.8 1.0
Substructure 21
p < 0.1% p < 1% p < 0.1% p < 1% p < 6% p < 1%
Veljanoski (in prep) Probabilities drawn from
- verall population can be
relatively small Similar behaviour in e.g. [Mg/Fe] Generally limited by number of stars
PI – GA surveys: Vanessa Hill
Clustering in integrals of motion (e.g. actions) maximal for right gravitational potential (DR2)
Sanderson et al. (2014, 2016)
Summary
- Halo substructure is useful for dynamics (dark matter) and merger history
- Photometric surveys mapped large structures in the outer halo
- TGAS x RAVE: excess of close velocity pairs and IoM space rich in substructure
– at level consistent with cosmological simulations of halos purely built via accretion – Less-bound halo stars predominantly retrograde (significance > 99.9%) – Many overdensities for more bound halo
- What’s coming:
– DR2 (April 2018) will be fantastic: proper motions and parallaxes for 1 billion stars! – 4MOST and WEAVE: spectroscopic follow – Characterization of the stars in the structures found, e.g. chemical abundances, ages – Numerical simulations for orbits, infall times, link to other structures in the halo – constraints on characteristic mass and scale of Milky Way