dark matter annihilation in and around the first galaxy halos · first order energy transfer!11 •...

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Dark Matter Annihilation in and around the First Galaxy Halos Sarah Schon, University of Melbourne supervised by Katherine Mack and Stuart Wyithe TAUP 2015, Torino 1

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Page 1: Dark Matter Annihilation in and around the First Galaxy Halos · First Order Energy Transfer!11 • High energy injected particles’ interactions with gas is non-trivial and dependent

Dark Matter Annihilation in and around the First

Galaxy Halos

Sarah Schon, University of Melbourne supervised by Katherine Mack and Stuart Wyithe

TAUP 2015, Torino

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Page 2: Dark Matter Annihilation in and around the First Galaxy Halos · First Order Energy Transfer!11 • High energy injected particles’ interactions with gas is non-trivial and dependent

Indirect Dark Matter Searches

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Col

lider

Exp

erim

ents

Direct Detection

Indirect Detection!

• Look for effects from standard model annihilation products

• i.e. particle excess from high DM density regions or cumulative, global signals

DM

SM

Page 3: Dark Matter Annihilation in and around the First Galaxy Halos · First Order Energy Transfer!11 • High energy injected particles’ interactions with gas is non-trivial and dependent

High Redshift Searches• Heating and ionisation from DM annihilation products

may alter the evolution of the IGM which could subsequently be detectable through measurements of the 21-cm line emission

• Search during the Cosmic Dark Ages* and Era of Reionisation

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* See poster by Cassandra Avram “Dark Matter Annihilation During Early Cosmic Times”

Page 4: Dark Matter Annihilation in and around the First Galaxy Halos · First Order Energy Transfer!11 • High energy injected particles’ interactions with gas is non-trivial and dependent

DM Annihilation and the IGM

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DM annihilates

IGM is modified through additional heating and

ionising component from DM

Change in 21-cm global signal and power spectrum

Page 5: Dark Matter Annihilation in and around the First Galaxy Halos · First Order Energy Transfer!11 • High energy injected particles’ interactions with gas is non-trivial and dependent

DM Annihilation and the IGM

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DM annihilates

IGM is modified through additional heating and

ionising component from DM

Change in 21-cm global signal and power spectrum

Astrophysical uncertainties can create degeneracies between

a possible DM signal and standard phenomenology.

Energy from DM annihilation may also change early structure

formation though “self-heating” halos

Page 6: Dark Matter Annihilation in and around the First Galaxy Halos · First Order Energy Transfer!11 • High energy injected particles’ interactions with gas is non-trivial and dependent

…with Modification of Structure Formation

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DM annihilates

Change in 21-cm global signal and power spectrum

IGM is modified through additional heating and

ionising component from DM

Halo self-heat, leading to possible delay or suppression

of structure formation

Page 7: Dark Matter Annihilation in and around the First Galaxy Halos · First Order Energy Transfer!11 • High energy injected particles’ interactions with gas is non-trivial and dependent

Self-heating HalosRequires:

• Dark Matter halo model

• Dark Matter particle model

• Energy Transfer scheme

• Compare gravitational binding energy of the gas of the halo to the energy transferred from DM annihilation over the Hubble time

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also see Schon et al MNRAS, 2015

Page 8: Dark Matter Annihilation in and around the First Galaxy Halos · First Order Energy Transfer!11 • High energy injected particles’ interactions with gas is non-trivial and dependent

DM Particle Model• Consider a SUSY neutralino type candidate, self-

annihilating to standard model particles.

!

• Assume weak-interaction cross-section

• Use an electron/positron proxy in PYTHIA to simulate annihilation to either muon, quark, W or tau

• Annihilation products are allowed to decay until only electrons, positron and photons remain

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Pdm =c2

mdm< v̄� > ⇢2dm

Page 9: Dark Matter Annihilation in and around the First Galaxy Halos · First Order Energy Transfer!11 • High energy injected particles’ interactions with gas is non-trivial and dependent

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Injected Particles

Page 10: Dark Matter Annihilation in and around the First Galaxy Halos · First Order Energy Transfer!11 • High energy injected particles’ interactions with gas is non-trivial and dependent

DM Halo Model

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Compare cusp (NFW, Einasto) and core (Burkert) density profiles, with different mass-concentration relations.

Central density paramount to total energy produced through annihilation

c sets profile turn-over

Page 11: Dark Matter Annihilation in and around the First Galaxy Halos · First Order Energy Transfer!11 • High energy injected particles’ interactions with gas is non-trivial and dependent

First Order Energy Transfer

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• High energy injected particles’ interactions with gas is non-trivial and dependent on the density, ionisation, temperature and species of the gas

• Create electromagnetic cascades with numerous secondary particles

• As a first order approach we calculate the energy loss of the primary particle as it travel through the halo and consider an absorption fraction of the secondary particles.

Feff =Udm(M, z)

Ug(M, z)T (M, z)fabs

Page 12: Dark Matter Annihilation in and around the First Galaxy Halos · First Order Energy Transfer!11 • High energy injected particles’ interactions with gas is non-trivial and dependent

New Code for Energy Transfer

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Update code for future work, to allow full realisation of electro-magnetic cascades in non-uniform gas density fields.

Page 13: Dark Matter Annihilation in and around the First Galaxy Halos · First Order Energy Transfer!11 • High energy injected particles’ interactions with gas is non-trivial and dependent

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Self-heating Halos

Page 14: Dark Matter Annihilation in and around the First Galaxy Halos · First Order Energy Transfer!11 • High energy injected particles’ interactions with gas is non-trivial and dependent

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Self-heating Halos

Page 15: Dark Matter Annihilation in and around the First Galaxy Halos · First Order Energy Transfer!11 • High energy injected particles’ interactions with gas is non-trivial and dependent

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Self-heating Halos

For most models, majority of annihilation

energy escapes the halo

For gas to be evacuated from halo, we require

light mass DM particles and high density halos

Page 16: Dark Matter Annihilation in and around the First Galaxy Halos · First Order Energy Transfer!11 • High energy injected particles’ interactions with gas is non-trivial and dependent

Future Work

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As the halo cools, gas becomes denser and heating from DM annihilation increases in efficiency

Energy from DM annihilation escapes halo into circum- galactic medium.

Self-heating in- efficient in Halo

Self-heating efficient in Halo, star-formation is

suppressed

Use updated energy transfer code to model gas in CGM and evolving halo with DM heating to look for further potential modification in standard structure formation

Page 17: Dark Matter Annihilation in and around the First Galaxy Halos · First Order Energy Transfer!11 • High energy injected particles’ interactions with gas is non-trivial and dependent

Conclusions• There exists a parameter space for which DM

annihilation may suppress star formation at high redshift in small halos

• Direct observation at these high redshifts is difficult but modification of star-formation maybe detectable through the 21-cm signal

• Follow up calculations (using an updated energy transfer code) of the energy deposited into the CGM and modification of the gas during the evolution of the halo are planned

• Thank you for your time!

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