STELLAR TO HALO MASS RELATION 2 LOUIS LEGRAND - OXFORD SCLSS - - PowerPoint PPT Presentation

stellar to halo mass relation
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STELLAR TO HALO MASS RELATION 2 LOUIS LEGRAND - OXFORD SCLSS - - PowerPoint PPT Presentation

LOUIS LEGRAND H. J. McCRACKEN, M. DOUSPIS, N. AGHANIM STELLAR TO HALO MASS RELATION 2 LOUIS LEGRAND - OXFORD SCLSS GALAXIES AND DARK MATTER Deficit for small and big masses. Silk & Mamon 2012 3 LOUIS LEGRAND - OXFORD SCLSS


slide-1
SLIDE 1

STELLAR TO HALO MASS RELATION

LOUIS LEGRAND

  • H. J. McCRACKEN, M. DOUSPIS, N. AGHANIM
slide-2
SLIDE 2

LOUIS LEGRAND - OXFORD SCLSS 2

Silk & Mamon 2012

Deficit for small and big masses.

GALAXIES AND DARK MATTER

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SLIDE 3

LOUIS LEGRAND - OXFORD SCLSS

STELLAR TO HALO MASS RELATION

3

▸What is the link between the stellar content

and the dark matter halo of galaxies ?

▸How is the galaxy stellar mass related to

the dark matter halo mass ?

▸Did the stellar-to-halo mass relation evolve

with time ?

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SLIDE 4

LOUIS LEGRAND - OXFORD SCLSS

MASS FUNCTIONS

4

Davidzon et al. 2017 Behroozi, 2013b

Stellar mass function: COSMOS Field Halo mass function: Bolshoï DM only simulation

slide-5
SLIDE 5

LOUIS LEGRAND - OXFORD SCLSS

ABUNDANCE MATCHING TECHNIQUE

5

▸ Hypotheses : ▸ Halos contain only

  • ne galaxy.

▸ The most massive

galaxies are in most massive halos, etc.

slide-6
SLIDE 6

LOUIS LEGRAND - OXFORD SCLSS

ABUNDANCE MATCHING TECHNIQUE

5

▸ Hypotheses : ▸ Halos contain only

  • ne galaxy.

▸ The most massive

galaxies are in most massive halos, etc.

slide-7
SLIDE 7

LOUIS LEGRAND - OXFORD SCLSS

ABUNDANCE MATCHING TECHNIQUE

5

▸ Hypotheses : ▸ Halos contain only

  • ne galaxy.

▸ The most massive

galaxies are in most massive halos, etc.

slide-8
SLIDE 8

LOUIS LEGRAND - OXFORD SCLSS

ABUNDANCE MATCHING TECHNIQUE

5

Stellar mass ▸ Hypotheses : ▸ Halos contain only

  • ne galaxy.

▸ The most massive

galaxies are in most massive halos, etc.

slide-9
SLIDE 9

LOUIS LEGRAND - OXFORD SCLSS

ABUNDANCE MATCHING TECHNIQUE

5

Stellar mass ▸ Hypotheses : ▸ Halos contain only

  • ne galaxy.

▸ The most massive

galaxies are in most massive halos, etc.

slide-10
SLIDE 10

LOUIS LEGRAND - OXFORD SCLSS

ABUNDANCE MATCHING TECHNIQUE

5

Stellar mass Dark matter mass ▸ Hypotheses : ▸ Halos contain only

  • ne galaxy.

▸ The most massive

galaxies are in most massive halos, etc.

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SLIDE 11

LOUIS LEGRAND - OXFORD SCLSS

STELLAR TO HALO MASS RELATION

6

Abundance matching hypotheses give :

Behroozi et al. 2010

φ∗ = φh dlog10(Mh) dlog10(M∗)

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MCMC with :

  • 5 free parameters
  • 10 bins in redshift
  • 2 HMF (Bolshoï simulation and Tinker et al. 2008)

log10(Mh) = log10(M1) + βlog10 ✓ M∗ M∗,0 ◆ + ⇣

M∗ M∗,0

⌘δ 1 + ⇣

M∗ M∗,0

⌘−γ − 1 2

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slide-12
SLIDE 12

LOUIS LEGRAND - OXFORD SCLSS

STELLAR TO HALO MASS RELATION

6

Abundance matching hypotheses give :

Behroozi et al. 2010

φ∗ = φh dlog10(Mh) dlog10(M∗)

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φCOSMOS

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Fit

MCMC with :

  • 5 free parameters
  • 10 bins in redshift
  • 2 HMF (Bolshoï simulation and Tinker et al. 2008)

log10(Mh) = log10(M1) + βlog10 ✓ M∗ M∗,0 ◆ + ⇣

M∗ M∗,0

⌘δ 1 + ⇣

M∗ M∗,0

⌘−γ − 1 2

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slide-13
SLIDE 13

LOUIS LEGRAND - OXFORD SCLSS

STELLAR TO HALO MASS RELATION

6

Abundance matching hypotheses give :

Behroozi et al. 2010

φ∗ = φh dlog10(Mh) dlog10(M∗)

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Bolshoï Tinker

φCOSMOS

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Fit

MCMC with :

  • 5 free parameters
  • 10 bins in redshift
  • 2 HMF (Bolshoï simulation and Tinker et al. 2008)

log10(Mh) = log10(M1) + βlog10 ✓ M∗ M∗,0 ◆ + ⇣

M∗ M∗,0

⌘δ 1 + ⇣

M∗ M∗,0

⌘−γ − 1 2

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slide-14
SLIDE 14

LOUIS LEGRAND - OXFORD SCLSS

RESULTS

7

z=0.2 z=3.5 Legrand, McCracken et al. in prep.

slide-15
SLIDE 15

LOUIS LEGRAND - OXFORD SCLSS

RESULTS

7

z=0.2 z=3.5 Legrand, McCracken et al. in prep.

slide-16
SLIDE 16

LOUIS LEGRAND - OXFORD SCLSS

EVOLUTION OF PEAK HALO MASS

8

  • First study using only one

survey from z~0 to 5.

  • No peak for z > 3.
  • Vary with the HMF.
  • Halo downsizing : Peak Halo

Mass decreases with time.

This work

Legrand, McCracken et al. in prep.

slide-17
SLIDE 17

THANK YOU FOR YOUR ATTENTION

slide-18
SLIDE 18

BACKUP SLIDES

slide-19
SLIDE 19

LOUIS LEGRAND 11

▸ The Cosmos field :

  • 2 deg2
  • +500 000 galaxies
  • 0<z<6
  • 2. OBSERVATIONS - THE COSMOS FIELD

Davidzon et al. 2017

▸ Stellar mass function

NASA, ESA

slide-20
SLIDE 20

LOUIS LEGRAND 12

▸ The Bolshoï simulation :

▸ Dark matter only

  • (250 Mpc/h)3
  • 8.109 particules
  • Resolution 5.1010 h-1 M☉
  • 2. SIMULATIONS - BOLSHOÏ

Kyplin et al. 2011 Behroozi, priv. comm.

▸ Halo mass function

Dashed lines for central halos and solid lines are for both satellite and central halos

slide-21
SLIDE 21

LOUIS LEGRAND - OXFORD SCLSS

TINKER AND BOLSHOI HMF

13

  • Tinker et al. 2008

HMF computed from simulations and then rescaled to the Planck Cosmology.

  • Bolshoï HMF is a fit
  • f Tinker HMF on a

DM only simulation with Planck parameters.

slide-22
SLIDE 22

LOUIS LEGRAND - OXFORD SCLSS

RESULTS

14

slide-23
SLIDE 23

LOUIS LEGRAND - OXFORD SCLSS

SHMR

15

SHMR Cosmos / Bolshoi

slide-24
SLIDE 24

LOUIS LEGRAND - OXFORD SCLSS 16

DAVIDZON ET AL. 2017

slide-25
SLIDE 25

LOUIS LEGRAND - OXFORD SCLSS

SCATTER IN STELLAR MASS

17

log10(φconv) ≈ log10(φth) + ξ2 2 ln(10) ✓dlog10(φth(M∗)) dlog10(M∗) ◆

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