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Comparing RAVE with theoretical models of the Milky Way Sanjib Sharma Joss Bland Hawthorn University of Sydney

Comparing RAVE with theoretical models of the Milky Way Sanjib Sharma Joss Bland Hawthorn University of Sydney

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Page 1: Comparing RAVE with theoretical models of the Milky Way Sanjib Sharma Joss Bland Hawthorn University of Sydney

Comparing RAVE with theoretical models of the Milky Way

Sanjib Sharma

Joss Bland HawthornUniversity of Sydney

Page 2: Comparing RAVE with theoretical models of the Milky Way Sanjib Sharma Joss Bland Hawthorn University of Sydney

Outline

• Galaxia a code for generating a synthetic/mock survey according to a given galaxy evolution model

• A mock RAVE survey with Galaxia

• What matches and what does not.

• What can we learn with RAVE, constraining models with observations.

Page 3: Comparing RAVE with theoretical models of the Milky Way Sanjib Sharma Joss Bland Hawthorn University of Sydney

Motivation• A framework to compare theoretical

models of our Galaxy with observations.

Theoretical model

Observed Catalog

Theory of Stellar Evolution (Isochrones) Galaxia

Synthetic Catalog

Analytical N-body

Comparison

Monte Carlo Markov Chain,

Chi square, etc

(Extinction, Measurement Errors)

),,vx,,( mZf

Observational Space

l, b, r, μl, μb, vr, B, V, log(g)

(Age,Pos,Vel,Metallicity,Mass)

Page 4: Comparing RAVE with theoretical models of the Milky Way Sanjib Sharma Joss Bland Hawthorn University of Sydney

Drawbacks of current schemes

• Besancon Model- state of the art (Robin et al 2003)• Also Trilegal, (Girardi et al, Padova group)• Designed for simulating a particular line of sight

– at max 25 line of sights• Discrete (l,b,r) step sizes to be supplied by user• Not suitable for wide area surveys, or large catalog of stars

– takes too much time • No possibility to simulate substructures or incorporate N-

body models– Sagittarius dwarf galaxy, simulation of tidally disrupted

galaxies

Page 5: Comparing RAVE with theoretical models of the Milky Way Sanjib Sharma Joss Bland Hawthorn University of Sydney

Theoretical Model-Analytical Models

),,vx,,( mZf

),x,()vx,,()()(

Zffmm Zxv

Star Formation Rate SFR

Initial Mass Function IMF

2)(log

)(/))(log(log log

Z

ZZ Ze

Age Metallicity Relation AMR

Phase space distribution

Page 6: Comparing RAVE with theoretical models of the Milky Way Sanjib Sharma Joss Bland Hawthorn University of Sydney

Sampling Analytical Model(Von Neumann rejection sampling)

Page 7: Comparing RAVE with theoretical models of the Milky Way Sanjib Sharma Joss Bland Hawthorn University of Sydney

Adaptive Mesh (Barnes Hut Tree)

Page 8: Comparing RAVE with theoretical models of the Milky Way Sanjib Sharma Joss Bland Hawthorn University of Sydney

Optimization• To generate a patch do not need to

generate the full galaxy– If a survey is not all sky, first check

if a node intersects with survey geometry.

• Faint stars which dominate in number are visible only for nearby nodes.

• For far away nodes there is a minimum mass above which stars are visible– Sort nodes according to distance.

Calculate appropriate m’ – Generate only those stars that are

visible.

r

x

yz

mmin m’ mmax

r

Page 9: Comparing RAVE with theoretical models of the Milky Way Sanjib Sharma Joss Bland Hawthorn University of Sydney

Galaxia summary

• Analytical model for disc, with warp– Robin et al 2003 (Besancon model)

• Padova Isochrones – m >0.15 , Marigo et al 2008, Bertilli et al 1994– 0.07<m<0.15 Chabrier et al 2000

• 3d extinction model – double exponential disc with warp and flare, hR=4.4

kpc, hz=0.088 kpc –

E(B-V) at infinity match Schlegel et al 1998 or– 0.54 mag/kpc in solar neighborhood

Page 10: Comparing RAVE with theoretical models of the Milky Way Sanjib Sharma Joss Bland Hawthorn University of Sydney

Computational Performance

• Run time nearly linear with mass of the galaxy being simulated– Due to the use of adaptive mesh or node

• Speed- 0.16 million stars per second (2.44 GHz proc)– For shallower surveys a factor of 3 less

• V<20, 10,000 sq degrees towards NGP, 35 ×106 stars, 220 secs

• V<20 GAIA like survey 4 billion stars can be generated in 6 hours on a single CPU

Page 11: Comparing RAVE with theoretical models of the Milky Way Sanjib Sharma Joss Bland Hawthorn University of Sydney

A synthetic RAVE survey

• RAVE_internalA (S/N>20 , July, VDR3)• For each RAVE field match the number

distribution of stars in IDENIS magnitude (9-12).– Assumption RAVE is a magnitude limited survey– Number counts were matched per 0.25 mag bin– Proper sampling required about 50 million stars in

9<IDENIS<12• Add extinction, add observational errors

– Photometric errors for the time being only added for 2MASS J and K not IDENIS

– Stellar parameter errors taken from Siebert et al 2011• σ= σ(log(g),Teff)

Page 12: Comparing RAVE with theoretical models of the Milky Way Sanjib Sharma Joss Bland Hawthorn University of Sydney

All stars

Page 13: Comparing RAVE with theoretical models of the Milky Way Sanjib Sharma Joss Bland Hawthorn University of Sydney

Dwarfs

Page 14: Comparing RAVE with theoretical models of the Milky Way Sanjib Sharma Joss Bland Hawthorn University of Sydney

Giants

Page 15: Comparing RAVE with theoretical models of the Milky Way Sanjib Sharma Joss Bland Hawthorn University of Sydney

Red Clumps (Siebert et al 2011 criteria)

Page 16: Comparing RAVE with theoretical models of the Milky Way Sanjib Sharma Joss Bland Hawthorn University of Sydney

(NRAVE-Nmodel)/√(NRAVE+Nmodel)

Page 17: Comparing RAVE with theoretical models of the Milky Way Sanjib Sharma Joss Bland Hawthorn University of Sydney

• Log(g) Vs Teff

Page 18: Comparing RAVE with theoretical models of the Milky Way Sanjib Sharma Joss Bland Hawthorn University of Sydney

Checking the kinematics

• Let us assume we have faithfully reproduced the RAVE catalog in color magnitude space.

• For the time being let us take radial velocities only.

• Convert to U V W components and check the distribution.

• Contains information about USun, VSun,

WSun,, σv(R,τ), τ being age

Page 19: Comparing RAVE with theoretical models of the Milky Way Sanjib Sharma Joss Bland Hawthorn University of Sydney

X

y

Page 20: Comparing RAVE with theoretical models of the Milky Way Sanjib Sharma Joss Bland Hawthorn University of Sydney

•Values of USun VSun sensitive to weights used, range used to fit. Inner and outer regions cannot be matched simultaneously

Page 21: Comparing RAVE with theoretical models of the Milky Way Sanjib Sharma Joss Bland Hawthorn University of Sydney
Page 22: Comparing RAVE with theoretical models of the Milky Way Sanjib Sharma Joss Bland Hawthorn University of Sydney

This is a good match

which means σvz(τ) is approximately correct.

Page 23: Comparing RAVE with theoretical models of the Milky Way Sanjib Sharma Joss Bland Hawthorn University of Sydney

What needs to be done

• Need to move beyond simple one dimensional fits. Multidimensional parameter search. A model fitting machinery .

• Need to use distance information also.

• Simultaneous constraints from different surveys SDSS, 2MASS, Hipparcos etc.

Page 24: Comparing RAVE with theoretical models of the Milky Way Sanjib Sharma Joss Bland Hawthorn University of Sydney

Hunting for structures

• Multi-dimensional group finder EnLinK. – Density based hierarchical group finder – Uses nearest neighbor links to search for peaks and

valleys in density distribution.– Gives a statistical significance of a group

• Develop a similar scheme for finding groups where we look for differences between a given data and an expected smooth model.

• Exploit all the multidimensional information that RAVE provides.