The Galactic Center and The Fornax Galaxy Cluster IPA 2013 May 13 2013 Sheldon Campbell Center for Cosmology and AstroParticle Physics The Ohio State University Outline 5132013 Sheldon Campbell The Ohio State University ID: 933417
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Slide1
An Indirect Detection Source Comparison Case Study
The Galactic CenterandThe Fornax Galaxy Cluster
IPA 2013May 13, 2013
Sheldon CampbellCenter for Cosmology and AstroParticle PhysicsThe Ohio State University
Slide2Outline
5/13/2013Sheldon Campbell, The Ohio State University
2Motivate indirect detection from the galactic center and nearby galaxy clusters.Constrain the dark matter distribution.
kinematical datacluster X-ray emissionCompare the strength of annihilation signals.The Fornax ClusterThe Galactic CenterConsequences for indirect detection experiments, IceCube in particular.
Slide3Indirect Detection of Dark Matter
5/13/2013Sheldon Campbell, The Ohio State University
3
Annihilating cosmic dark matter detectable astrophysical radiationIntensity
Brightest regions are those that are a combination of
close
, and
dense
over considerable volume.
particle properties
J-factor: astrophysical
distribution
Slide4Where is Dark Matter Annihilation Brightest?
5/13/2013Sheldon Campbell, The Ohio State University
4Galactic Center is a very well-motivated candidate!
Relatively nearby.Expected to be very dark matter dense (based on simulations).Observational evidence for acored halo profile?If so, nearby substructure-rich
galaxy clusters might be as bright.
Slide5The Milky Way Dark Matter Halo
5/13/2013Sheldon Campbell, The Ohio State University
5
Our halo may have a cusp at the core.as seen in dark-matter-only cosmological simulations.
Also plausible are cored profiles.
NFW profile
Einasto profile
Burkert profile
Slide6Constraints from Kinematical Galactic Tracers
5/13/2013Sheldon Campbell, The Ohio State University
6
NFW profile
Catena,
Ullio
,
JCAP 1008 (2010) 004
Nesti, Salucci, arXiv:1304.5127
The solar system velocity strongly constrains
the value of
.
The J-factor goes roughly as
.
Constraints from Kinematical Galactic Tracers
5/13/2013Sheldon Campbell, The Ohio State University
7
Einasto profile
Also consistent with
current data for a
significant range
of parameters.
Slide8Constraints from Kinematical Galactic Tracers
5/13/2013Sheldon Campbell, The Ohio State University
8
Burkert profile
Nesti and Salucci point out
that the cored Burkert profile
has less tension with data
than the cusped profiles.
Slide9Galactic Center J-factor Profile
5/13/2013Sheldon Campbell, The Ohio State University
9
NFW
Einasto
Burkert
In the case that our halo profile is cored, it is advantageous to also consider signals from nearby galaxy clusters…
Slide10The Fornax Galaxy Cluster
5/13/2013Sheldon Campbell, The Ohio State University
10
A good target because: It is BIG.
diameter in the sky.
It is
near
.
20
M
pc
away.
It may have abundant substructure that could make it very bright to us.
WISE Experiment, NASA/JPL-Caltech/UCLA
Slide11X-ray Cluster Intensity Profiles
5/13/2013Sheldon Campbell, The Ohio State University
11
Pressure-supported gas at the
cluster center thermally emits X-rays.
If spherical, and in hydrodynamical equilibrium, the total gravitational potential may be reconstructed.
The X-ray intensity profile is well-described by
the
β
-model.
Reiprich
,
Bohringer
(2007)
This corresponds to a cored dark matter profile.
What would the X-rays look like in an NFW profile?
U
sing X-rays to Constrain the Halo Profile5/13/2013
Sheldon Campbell, The Ohio State University12
A best-fit
b-model fits the X-ray data very well.
Assuming spherically distributed
matter with gas in hydrodynamical
equilibrium:
An NFW profile with same scale
radius is similarly shaped, offset.
Similarly for the Einasto profile
with
a=0.16.
And with
a=0.26.
Slide13The scale radius for each profile is determined from
X-ray data.
5/13/2013Sheldon Campbell, The Ohio State University
13
Surprisingly, all profiles are consistent with the
X-ray data, given
an appropriate
scale radius
.
Cluster d
ensity
profiles
may
also constrained
by:
kinematic data,weak lensing.
Slide14Substructure Models for Galaxy Clusters
5/13/2013Sheldon Campbell, The Ohio State University
14
Three recently published models of substructure were considered:Gao et al. (2011), G11:
Based on the Phoenix and Aquarius simulations.A fitting formula for the angular surface intensity of substructure.Kamionkowski
et al. (2010), K10:
Density Probability Distribution Function profile.
Fit to the Via
Lactea
II simulation.
Suggested scaling for galaxy clusters by Sánchez-
Conde
et al. (2011).
Pinzke
et al. (2011), P11:
Used the Aquarius simulations and scaled up to cluster sized halos.Found a double-power law fit the primary substructure intensity profile.Scaled down to . I also try .
Slide15J-factor Profiles for the Fornax Cluster
5/13/2013Sheldon Campbell, The Ohio State University
15
NFW
Einasto (
Einasto (
The modest substructure models bring the J-factor to levels similar to the
J-factor of the cored galactic center.
We need the X-ray constraint to remain satisfied…
smooth
K10
G11
P11
TeV Gamma-Ray Emitters
and The Fornax Cluster
Fornax
Wiebusch, arXiv:0907.2263
5/13/2013
Sheldon Campbell, The Ohio State University
16
Slide17Conclusions
5/13/2013Sheldon Campbell, The Ohio State University
17The galactic center may be an excellent target for dark matter indirect detection, given its close proximity and bountiful dark matter abundance.
If the galactic dark matter halo profile is cored, the Fornax Cluster may provide an equally suitable target, if its substructure should prove as abundant as simulations suggest.The galactic center dark matter search analysis at IceCube may be extended to include the Fornax Cluster, as it also resides in the southern sky.