STAR FORMATION HISTORIES FROM Z=0 TO Z=8 Peter Behroozi, Stanford - - PowerPoint PPT Presentation

star formation histories from z 0 to z 8
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STAR FORMATION HISTORIES FROM Z=0 TO Z=8 Peter Behroozi, Stanford - - PowerPoint PPT Presentation

STAR FORMATION HISTORIES FROM Z=0 TO Z=8 Peter Behroozi, Stanford University Risa W echsler, Stanford University Charlie Conroy, Harvard / UCSC Santa Cruz Galaxy W orkshop 2011 Wednesday, August 10, 11 Major Questions When did galaxies


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SLIDE 1

STAR FORMATION HISTORIES FROM Z=0 TO Z=8

Peter Behroozi, Stanford University Santa Cruz Galaxy W

  • rkshop 2011

Risa W echsler, Stanford University Charlie Conroy, Harvard / UCSC

Wednesday, August 10, 11

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SLIDE 2

Major Questions

When did galaxies form their stars, as a function of their mass today? (Or their mass at an earlier redshift?)

LMC; Hubble Heritage Team

Wednesday, August 10, 11

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SLIDE 3

Major Questions

What’s the solution to the discrepancy between the cosmic SFR and the cosmic SM density? 0 1 2 3 4 z

Wilkins et al. 2008

Wednesday, August 10, 11

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SLIDE 4

Approach

Parametrize the evolution of the stellar mass function; Constrain using ALL available data, currently including observations of the stellar mass function, specific star formation rates, and the cosmic star formation rate (all from z=0-8). Include nuisance parameters for all conceivable systematic effects.*

*see Behroozi, Conroy, & W echsler 2010

Wednesday, August 10, 11

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SLIDE 5

Approach

(∆t) · SFRmd(tnow) = SMmd(tnow) −

  • MMPmp,md + SUBSmp,md · (1 − ICL(mp, md))
  • × SFHmp,t(tnow)(1 − SLt(tnow))

(new stars) (expected stellar mass) (number of contributing progenitors, corrected for ICL losses) (stellar population of progenitors, corrected for stellar death)

In equations:

Talk to me about details!

Wednesday, August 10, 11

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SLIDE 6

Approach

Include parametrized models for all conceivable systematic effects: Many have suggested that high-redshift galaxies have bursty/dusty star formation,* but no-one’s done a self-consistent check. Let’s try out a simple model! *Stark et al. 2009, K.S. Lee et al. 2009, Schaerer & Barros 2010

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SLIDE 7

SFR / SM Tension

λ(z) = A 1 + exp(B − z) Incompleteness/burstiness:

1 2 3 4 5 z 0.4 0.5 0.6 0.7 0.8 0.9 Completeness

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SLIDE 8

SFR / SM Tension

1 2 3 4 5 6 Redshift 0.001 0.01 0.1 Cosmic SFR [MO

  • yr
  • 1 Mpc
  • 3]

Without including CSFR constraint Face Value Bursty/Dust Obscured Bursty/Dust Obscured w/o SSFR scaling

W e can immediately better match the cosmic SFR.

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SLIDE 9

SFR / SM Tension

1 2 3 4 5 z 0.4 0.5 0.6 0.7 0.8 0.9 1 Completeness

And we can constrain the incompleteness (in this model):

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SLIDE 10

SFR / SM Tension

Burstiness / dust obscuration helps, but does not completely explain the cosmic SFR / SM tension at z>4. Result: W e have an extremely powerful framework for testing models to resolve the cosmic SFR / SM tension.

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SLIDE 11

W e’ve run our models to z=0, and found the same trends: strongly decreasing SFRs at fixed halo mass with redshift:

Star Formation Rates

Preliminary

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SLIDE 12

Star Formation Histories

But, if we ask the complementary question about galaxy star formation histories, there’s no single trend!

Preliminary

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SLIDE 13

Star Formation Histories

The rate at which the stellar population grew in low-mass galaxies has always been increasing; whereas for high-mass galaxies, the rate peaked at an early redshift and then declined.

Preliminary

0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 Scale Factor 0.2 0.4 0.6 0.8 1 SF History [MO

  • yr
  • 1]

Mh = 10

11.0 MO

  • h
  • 1

0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 Scale Factor 10 20 30 40 50 60 70 80 SF History [MO

  • yr
  • 1]

Mh = 10

13.0 MO

  • h
  • 1

Wednesday, August 10, 11

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SLIDE 14

Star Formation Histories

Best-fit model: Even better in detail: V alid across a wide range of redshifts (0<z<4 at least).

0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 Scale Factor 0.2 0.4 0.6 0.8 1 SF History [MO

  • yr
  • 1]

Mh = 10

11.0 MO

  • h
  • 1

0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 Scale Factor 10 20 30 40 50 60 70 80 SF History [MO

  • yr
  • 1]

Mh = 10

13.0 MO

  • h
  • 1

SFH(a) = AaB exp[C(1 − a)] SFH(a) = AaB exp[C(1 −

3

√a)]

Wednesday, August 10, 11

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SLIDE 15

Final Words

Still preliminary work, but: Our approach combines constraints from the observed stellar mass function at all times, as well as the observed clustering of galaxies (through the galaxy-halo connection), as well as the cosmic SFR and specific SFRs.

Wednesday, August 10, 11

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SLIDE 16

Final Words

Still preliminary work, but: W e can also start to constrain models for resolving the discrepancy between cosmic SFRs and SMs. Our approach combines constraints from the observed stellar mass function at all times, as well as the observed clustering of galaxies (through the galaxy-halo connection), as well as the cosmic SFR and specific SFRs.

Wednesday, August 10, 11

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SLIDE 17

Final Words

Still preliminary work, but: W e can also start to constrain models for resolving the discrepancy between cosmic SFRs and SMs. Our approach combines constraints from the observed stellar mass function at all times, as well as the observed clustering of galaxies (through the galaxy-halo connection), as well as the cosmic SFR and specific SFRs. W e’ve already obtained constraints on the functional form of both the star formation history and the star formation rate for galaxies.

Wednesday, August 10, 11

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SLIDE 18

Image Credits

http://spacefellowship.com/news/ art15504/picture-of-the-day-the- birth-of-stars.html http://www.williamsclass.com/ EighthScienceW

  • rk/

ImagesEighth/ SuperNovaReminant.jpg

Wednesday, August 10, 11