interactions and cosmic reionization JCAP 1808 (2018) no.08, 045 - - PowerPoint PPT Presentation

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interactions and cosmic reionization JCAP 1808 (2018) no.08, 045 - - PowerPoint PPT Presentation

Dark matter-DARK RadiAtion interactions and cosmic reionization JCAP 1808 (2018) no.08, 045 Vikram Rentala Indian Institute of Technology Bombay (w Subinoy Das, Rajesh Mondal and Srikanth Suresh) Observational constraints on reionization


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SLIDE 1

Dark matter-DARK RadiAtion interactions and cosmic reionization

Vikram Rentala Indian Institute of Technology Bombay

(w Subinoy Das, Rajesh Mondal and Srikanth Suresh)

JCAP 1808 (2018) no.08, 045

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SLIDE 2

Observational constraints on reionization

  • Quasar absorption spectra traces neutral hydrogen
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SLIDE 3

Observational constraints on reionization

  • Gunn-Peterson trough
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SLIDE 4

Observational constraints on reionization

  • Optical depth to CMB
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SLIDE 5

When does reionization happen?

Seiler, Jacob et al. astro-ph/1902.01611

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SLIDE 6

Can we constrain dark matter particle physics models with these

  • bservations?
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SLIDE 7

Outline

  • Self-interacting dark matter
  • ETHOS framework
  • Structure formation
  • Constraints from Cosmic Reionization
  • Future observables
  • Conclusions
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SLIDE 8

Astrophysical and cosmological evidence for dark matter

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SLIDE 9

Problems with the standard LCDM

Small scales

  • Missing satellite problem (Klypin et al, Moore et al, 1999)
  • Too big to fail problem (Boylan-Kolchin et al, 2011)
  • Core cusp problem (Oh et al, 2010)

Baryonic feedback or dark matter self interactions?

(Bullock et al 2000, Benson et al 2002, Governato et al 2010)

Large scales

  • Hubble tension (Zhang et al, 2017)
  • σ8 tension (Battye et al 2014)
  • Effective number of neutrinos (Mangano et al 2005, Lesgourges et al

2016)

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SLIDE 10

Self-interacting dark matter

c c c c

Spergel, Steinhardt PRL, 1999 Harvey et al, Science, 2015

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SLIDE 11

Dark matter and dark radiation

Visible Hidden Mediator Light particles are generic:

Goldstone bosons, chiral fermions, gauge bosons

CMB:

Mass/Energy

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SLIDE 12

Evolution of cosmological perturbations Metric

Photons Electrons Protons Dark Matter Neutrinos

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SLIDE 13

Evolution of cosmological perturbations Metric

Photons Electrons Protons Dark Matter Dark Radiation Neutrinos

?

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Wh What at is the is the impact impact of D

  • f Dark

ark Matter Matter-Dar Dark k Radiatio Radiation n inte interactions ractions on reio

  • n reioniza

nization? tion?

  • Impact on structure formation
  • Impact on reionization
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SLIDE 15

Impact on structure formation

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SLIDE 16

ETHOS framework

(Cyr-Racine et al 2016)

Particle physics -> Cosmology Basic idea: Map all the particle physics parameters to coefficients of a red-shift series expansion of the collision term

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ETHOS model 1

(Cyr-Racine et al, Binder et al 2016) Dark matter particle Dark radiation Mediator

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Decoupling of DM and DR

  • Comoving Hubble scale
  • Scattering length

Early times Late times DM and DR are tightly coupled (dark acoustic oscillations) DM and DR are decoupled (DM free streams) * We will assume that this transition takes place in the radiation dominated universe

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Decoupling of dark matter and dark radiation

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Jeans scale (pre-decoupling)

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Jeans scale (post-decoupling)

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Evolution of Jeans scale in ETHOS 1

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Evolution of Jeans scale in ETHOS 1

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Evolution of Jeans scale in WDM models

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Evolution of Jeans scale in WDM models

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Linear Power Spectrum (z=124)

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Non-Linear power spectrum (z=8)

from N-body simulation Lyman-alpha constraints rule out mx < 3.5 keV

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SLIDE 28

Halo mass distribution (z=8)

from Halo finding algorithm

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Halo mass distribution (z=8)

from Halo finding algorithm

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Impact on reionization

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From structure to reionization

Halos in ΛCDM

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From structure to reionization

Halos in ΛCDM

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From structure to reionization

With suppressed small scale structure we need higher values of Nion in order to achieve reionization!

Halos in self-interacting DM model

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What value of Niondo we need for successful reionization?

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HI brightness temperature (z = 8)

Nion Nion 100 321 721 23 23 57 225 861

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Can we estimate Nion?

can be safely assumed

Depends on metallicity, IMF, SF efficiency, escape fraction

Large systematic uncertainties! However,

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Our Results

  • Constraint on a4 from demanding consistency

with global history of reionization

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Future: HI brightness power spectrum

Future 21 cm surveys could measure this difference

GMRT, LOFAR, MWA, PAPER, SKA, HERA …

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Other future observations

How can we reduce systematic uncertainties on Nion?

  • Direct observations of early galaxies that reionized

the universe (using near IR observations)

  • Pop III stars (JWST)
  • Improved galaxy formation simulations matched to

data

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SLIDE 40

Conclusions

  • Dark Matter - Dark radiation interactions can

lead to suppression of the small scale matter power spectrum

  • Global history of reionization can set strong

constraints on DM-DR interactions

  • Need to have a realistic understanding of the

astrophysical uncertainties

  • 21 cm surveys could potentially detect the

impact of DM-DR interactions on cosmological perturbations

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QUESTIONS, COMMENTS, SUGGESTIONS?

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Backup Slides

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Robustness check

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Global history of reionization

EDGES, SARAS, DARE … Pritchard (2011)

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Abundance Matching

The Current Status of Galaxy Formation - Silk, Joe et al. arXiv:1207.3080