CTA as a γ-ray probe for dark matter structures: Searching for the smallest clumps & the largest clusters

Size: px
Start display at page:

Download "CTA as a γ-ray probe for dark matter structures: Searching for the smallest clumps & the largest clusters"

Transcription

1 CTA as a γ-ray probe for dark matter structures: Searching for the smallest clumps & the largest clusters Moritz Hütten (MPP Munich) for the CTA consortium "The extreme Universe viewed in very-highenergy gamma rays 2018, La Palma, Introduction 2. Dark Galactic DM clumps 3. Galaxy clusters mhuetten@mpp.mpg.de

2 1. Introduction 2

3 Gravitational evidence for dark matter on all scales Reticulum II, Dwarf galaxies small scales (pc) baryonic matter Baryonic matter dark matter Dark Matter large scales (Mpc) 3

4 Gravitational evidence for dark matter on all scales Reticulum II, Dwarf galaxies Begemann (1991) small scales (pc) baryonic matter Baryonic matter Milky Way-like galaxies dark matter Dark Matter large scales (Mpc) 3

5 Gravitational evidence for dark matter on all scales Reticulum II, Dwarf galaxies Begemann (1991) small scales (pc) baryonic matter Baryonic matter Milky Way-like galaxies dark matter Dark Matter large scales (Mpc) Galaxy cluster substructure 3

6 Gravitational evidence for dark matter on all scales Reticulum II, Dwarf galaxies Begemann (1991) small scales (pc) baryonic matter Baryonic matter Galaxy clusters dark matter Milky Way-like galaxies Dark Matter large scales (Mpc) Chandra/HST image of Abell 1689 Galaxy cluster substructure 3

7 The dark matter γ-ray connection: indirect detection NASA/G. Dinderman (mass > GeV) 4

8 The dark matter γ-ray connection: indirect detection NASA/G. Dinderman (mass > GeV) 4

9 The dark matter γ-ray connection: indirect detection NASA/G. Dinderman typical astrophysical background γ-rays: (mass > GeV) m = 500 GeV + straight to observer + no absorption in the Galaxy - astrophysical background 4

10 Dark matter structures on all scales 140 Mpc x 100 Mpc 500 Mpc x 375 Mpc 0.8 Mpc x 0.6 Mpc DM d (sim ensity ulat ion) 0.4 Mpc x 0.3 Mpc Springel et al. (2005) Diemand, Kuhlen, Madau (2006) color code: brighter = denser 5

11 Dark matter structures on all scales 140 Mpc x 100 Mpc 500 Mpc x 375 Mpc DM d (sim ensity ulat ion) 0.8 Mpc x 0.6 Mpc Springel et al. (2005) Diemand, Kuhlen, Madau (2006) color code: brighter = denser 5

12 Dark matter structures on all scales 140 Mpc x 100 Mpc 500 Mpc x 375 Mpc DM d (sim ensity ulat ion) 0.8 Mpc x 0.6 Mpc Springel et al. (2005) Diemand, Kuhlen, Madau (2006) color code: brighter = denser 5

13 Dark matter structures on all scales 140 Mpc x 100 Mpc 500 Mpc x 375 Mpc DM d (sim ensity ulat ion) Satellite galaxies 0.8 Mpc x 0.6 Mpc Springel et al. (2005) Diemand, Kuhlen, Madau (2006) color code: brighter = denser 5

14 Dark matter structures on all scales 140 Mpc x 100 Mpc 500 Mpc x 375 Mpc DM d (sim ensity ulat ion) Satellite galaxies Segue I 0.8 Mpc x 0.6 Mpc LMC C Springel et al. (2005) Diemand, Kuhlen, Madau (2006) color code: brighter = denser 5

15 Dark matter structures on all scales 140 Mpc x 100 Mpc 500 Mpc x 375 Mpc Satellite galaxies Segue I Dark 0.8 Mpc x 0.6 Mpc clumps: too light to trigger star formation DM d (sim ensity ulat ion) LMC C Springel et al. (2005) Diemand, Kuhlen, Madau (2006) color code: brighter = denser 5

16 Dark matter structures on all scales 140 Mpc x 100 Mpc 500 Mpc x 375 Mpc 0.8 Mpc x 0.6 Mpc DM d (sim ensity ulat ion) 0.4 Mpc x 0.3 Mpc Springel et al. (2005) Diemand, Kuhlen, Madau (2006) color code: brighter = denser 6

17 Dark matter structures on all scales 500 Mpc x 375 Mpc 0.8 Mpc x 0.6 Mpc DM d (sim ensity ulat ion) 0.4 Mpc x 0.3 Mpc Springel et al. (2005) Diemand, Kuhlen, Madau (2006) color code: brighter = denser 6

18 Dark matter structures on all scales 500 Mpc x 375 Mpc DM d (sim ensity ulat ion) Assuming this was Perseus cluster (d = 80 Mpc) 0.8 Mpc x 0.6 Mpc 0.4 Mpc x 0.3 Mpc Springel et al. (2005) Diemand, Kuhlen, Madau (2006) color code: brighter = denser 6

19 Dark matter structures on all scales 500 Mpc x 375 Mpc DM d (sim ensity ulat ion) Assuming this was Perseus cluster (d = 80 Mpc) CTA field of view 0.8 Mpc x 0.6 Mpc (6 diameter) 0.4 Mpc x 0.3 Mpc Central 1 Mpc of the Perseus cluster (0.7 x 0.7 ) Springel et al. (2005) Diemand, Kuhlen, Madau (2006) color code: brighter = denser 6

20 The dark matter sky seen from Earth (annihilation) log (γ-ray intensity from DM annihilation), Galactic coordinates synthetic map calculated with CLUMPY

21 The dark matter sky seen from Earth (annihilation) Galactic center + strong signal γ-ray backgrounds (Silk and Bloemen, 1987, ) log (γ-ray intensity from DM annihilation), Galactic coordinates synthetic map calculated with CLUMPY

22 The dark matter sky seen from Earth (annihilation) Galactic center Milky Way satellite galaxies + no background lower fluxes , , + strong signal γ-ray backgrounds (Silk and Bloemen, 1987, ) log (γ-ray intensity from DM annihilation), Galactic coordinates synthetic map calculated with CLUMPY

23 The dark matter sky seen from Earth (annihilation) Dark clumps + no background? brighter than satellites unknown position Galactic center Milky Way satellite galaxies + no background lower fluxes , , + strong signal γ-ray backgrounds (Silk and Bloemen, 1987, ) log (γ-ray intensity from DM annihilation), Galactic coordinates synthetic map calculated with CLUMPY

24 The dark matter sky seen from Earth (annihilation) Galaxy clusters + massive DM targets far away γ-ray backgrounds Dark clumps + no background? brighter than satellites unknown position Galactic center Milky Way satellite galaxies + no background lower fluxes , , + strong signal γ-ray backgrounds (Silk and Bloemen, 1987, ) log (γ-ray intensity from DM annihilation), Galactic coordinates synthetic map calculated with CLUMPY

25 The dark matter sky seen from Earth (annihilation) Galaxy clusters + massive DM targets far away γ-ray backgrounds Dark clumps + no background? brighter than satellites unknown position Galactic center Milky Way satellite galaxies + no background lower fluxes , , + strong signal γ-ray backgrounds (Silk and Bloemen, 1987, ) log (γ-ray intensity from DM annihilation), Galactic coordinates synthetic map calculated with CLUMPY

26 Dark matter clumpiness matters! Annihilation Decay 8

27 Dark matter clumpiness matters! Flux searched for with γ-ray telescope Annihilation Decay 8

28 Dark matter clumpiness matters! Annihilation Secondary γ-rays after annihilation/decay Decay 8

29 Dark matter clumpiness matters! Annihilation Decay Unknown DM particle mass: parameter 8

30 Dark matter clumpiness matters! Annihilation Annihilation cross section Decay Particle lifetime 8

31 Dark matter clumpiness matters! Annihilation Decay Density distribution 8

32 Dark matter clumpiness matters! Annihilation Decay Density distribution What density targets do we need for CTA? 1. Bright: close and/or massive DM budget 2. Localized ( point-like ) 3. no astrophysical back-/foregrounds 8

33 2. Dark Galactic DM clumps 9

34 Dark clumps annihilation brightness Brightness in γ-rays (J-factor): conservative 10 4 counting all objects flux from annihilation ~ Hütten, Combet, Maier, Maurin (2016) 10 3 optimistic N X( J) Estimated J-factors of known satellite galaxies counting all objects many faint objects J-factor [GeV 2 cm 5 ] few bright objects 10

35 Dark clumps annihilation brightness Brightness in γ-rays (J-factor): conservative 10 4 counting all objects flux from annihilation ~ Close-by dark clumps bright DM targets Hütten, Combet, Maier, Maurin (2016) 10 3 optimistic N X( J) Estimated J-factors of known satellite galaxies counting all objects many faint objects J-factor [GeV 2 cm 5 ] few bright objects 10

36 Dark clumps annihilation profiles half-light radius ~ 0.14 log Intensity conservative l [deg] clumpy code, b [deg] Take advantage of CTA s excellent angular resolution 11

37 Dark clumps annihilation profiles half-light radius ~ 0.14 Point-like emission from dark clumps log Intensity conservative l [deg] clumpy code, b [deg] Take advantage of CTA s excellent angular resolution 11

38 But how to find the dark clumps? In a survey: Observing 25% of the sky with 500 hours (extragalactic survey benchmark): 25% of sky γ-ray brightest subhalo in the field (assume it is a dark clump)

39 But how to find the dark clumps? In a survey: Observing 25% of the sky with 500 hours (extragalactic survey benchmark): Chance detection 22 approximate CTA 236 diameter FOV 24 12

40 Survey sensitivity based on CTA South (prod2-3) 500h, 95% C.L. (Hütten, Combet, Maier, Maurin, 2016) CTA dark subhalos, model HIGH CTA dark subhalos,! b b Di erent targets,! b b h vi [cm 3 s 1 ] %! b b 68% LOW (post-trial) HIGH LOW (post-trial) HIGH (pre-trial) (post-trial) Cosmic variance VERITAS, stacked dsph MAGIC, Segue 1 (158h) H.E.S.S., Gal. halo (254h) Fermi-LAT, stacked dsph CTA dark subhalos (HIGH) thermal relic cross section WIMP mass m [GeV] WIMP mass m [GeV] WIMP mass m [GeV] 13

41 Survey sensitivity based on CTA South (prod2-3) 500h, 95% C.L. (Hütten, Combet, Maier, Maurin, 2016) CTA dark subhalos, model HIGH CTA dark subhalos,! b b Di erent targets,! b b h vi [cm 3 s 1 ] ! b b! b b [cm 2 s 1 sr 1 GeV 1 ] conservative model LOW (post-trial) optimistic HIGH (post-trial) model [cm 2 s 1 sr 1 GeV 1 ] VERITAS, stacked dsph MAGIC, Segue 1 (158h) H.E.S.S., Gal. halo (254h) Fermi-LAT, stacked dsph CTA dark subhalos (HIGH) [cm 2 s 1 sr 1 GeV 1 ] Modeling systematics thermal relic cross section WIMP mass m [GeV] WIMP mass m [GeV] [cm 2 s 1 sr 1 GeV 1 ] WIMP mass m [GeV]

42 Survey sensitivity based on CTA South (prod2-3) 500h, 95% C.L. (Hütten, Combet, Maier, Maurin, 2016) CTA dark subhalos, model HIGH CTA dark subhalos,! b b Di erent targets,! b b h vi [cm 3 s 1 ] ! b b! b b + conservative model LOW (post-trial) optimistic HIGH (post-trial) model VERITAS, stacked dsph MAGIC, Segue 1 (158h) H.E.S.S., Gal. halo (254h) Fermi-LAT, stacked dsph CTA dark subhalos (HIGH) thermal relic cross section WIMP mass m [GeV] WIMP mass m [GeV] WIMP mass m [GeV] 15

43 Survey sensitivity based on CTA South (prod2-3) 500h, 95% C.L. (Hütten, Combet, Maier, Maurin, 2016) h vi [cm 3 s 1 ] CTA dark subhalos, model HIGH! b b! b b + CTA dark subhalos, LOW (post-trial) conservative model LOW HIGH (post-trial) optimistic HIGH (post-trial) (pre-trial) model! b b Di erent targets,! b b CTA Segue 1 (500h) CTA Gal. halo (500h, Einasto) VERITAS, stacked dsph MAGIC, Segue 1 (158h) H.E.S.S., Gal. halo (254h) Fermi-LAT, stacked dsph CTA dark subhalos (HIGH) thermal relic cross section WIMP mass m [GeV] WIMP mass m [GeV] WIMP mass m [GeV] 16

44 Chance detection probability: Subhalo algebra 1. Number of detectable objects rises linearly with ΔΩ : geometry + isotropy 2. Number of detectable objects rises with sqrt(t obs ): instrument background 3. Number of detectable objects rises inversely with sensitivity threshold N objects ( F sens ) ~ 1/F sens : subhalo source count distribution See Hütten et al. (2016), App. E, for details ΔΩ N FOV T obs /FOV <σv> N spots ( 2σ) π min cm 3 s min cm 3 s min cm 3 s min cm 3 s

45 3. Galaxy clusters 18

46 The case of galaxy clusters: DM annihilation Recall: All Galactic clumps N X( J) dwarf galaxies J-factor [GeV 2 cm 5 ] 19

47 The case of galaxy clusters: DM annihilation Recall: All Galactic clumps N X( J) dwarf galaxies J-factor [GeV 2 cm 5 ] DM-annihilation brightness comparable to satellite galaxies 19

48 The case of galaxy clusters: DM annihilation DM-annihilation brightness comparable to satellite galaxies Emission profiles more extended (typical half-light radii > 0.5 ) 19

49 The case of galaxy clusters: DM annihilation DM-annihilation brightness comparable to satellite galaxies Emission profiles more extended (typical half-light radii > 0.5 ) Astrophysical backgrounds: γ-ray emitting galaxies (AGN, star-forming galaxies, CR interaction) Also expect diffuse emission from the inter-cluster medium (ICM) 19

50 DM annihilation profile of the Perseus cluster 3 orders of magnitude 0.5 Intensity proportional to without substructure random triaxiality 20

51 DM annihilation profile of the Perseus cluster 3 orders of magnitude 0.5 NCG 1275 MAGIC, E > 250 GeV IC 310 Intensity proportional to without substructure random triaxiality 20

52 DM decay profile of the Perseus cluster 3 orders of magnitude 0.5 NCG 1275 MAGIC, E > 250 GeV See MAGIC result : τ DM s IC 310 Intensity proportional to random triaxiality (substructure irrelevant) 21

53 Cosmic-ray induced emission in the inter-cluster medium Spatial profile Spectral profile Expectation Expectation CTA s excellent angular resolution and energy range: disentangle the signals DM substructure extends annihilation profile 22

54 The CTA galaxy cluster working group (wg-phys-clusters) CTA galaxy cluster key science project: 300 hours allocated for CTA North Coordination: Moritz Hütten (MPP Munich) Judit Pérez-Romero, Miguel Sánchez-Conde (UAM Madrid) The team: R. Alfaro, G. Brunetti, S. Colafrancesco, C. Delgado, M. Doro, E. Fedorova, E. de Gouveia Dal Pino, S. Hernandez Cadena, M. Hütten, M. Lallena, S. Nuza, J. Pérez, O. Reimer, M. Sánchez-Conde, S. Zimmer Updated performance study on galaxy clusters in progress 23

55 Conclusions Hierarchical DM clustering: γ-ray clumps from annihilation/decay at various scales and distances Search for the smallest clumps in a TeV γ-ray survey with CTA (extragalactic key science project by-catch) Watch out for unidentified sources in the FOV: may be a Galactic DM clump Study the closest galaxy clusters: Perseus and Coma: Excellent observation conditions with CTA North Clusters: Constrain DM particle life times beyond τ DM > s = t Universe CTA excellent probe for TeV dark matter particle physics in various complementary targets 24

56 BACK UP 25

57 Perseus cluster also optimal target for DM decay Perseus = Perseus region already extensively studied by MAGIC telescopes: , , , , , : τ DM s 26

58 Astrophysical merits of Perseus cluster observations

59 Brightest Galactic DM clumps: Properties Average mass and distance (from 10 4 runs): Fermi-LAT scenario CTA scenario Median properties of (f sky = 82.6%) (f sky = 25%) brightest subhalo within int =0.1 int =0.8 int =0.05 int =0.1  ÂD ı obs [kpc]  1 2  log 10 ( Âm ı vir /M ) log  10 J ı /GeV 2 cm optimistic Fermi-LAT scenario CTA scenario Median properties of (f sky = 82.6%) (f sky = 25%) brightest subhalo within int =0.1 int =0.8 int =0.05 int =0.1 ÂD ı obs [kpc] log 10 ( Âm ı vir /M ) log  10 J ı /GeV 2 cm conservative 28

60 Dark clumps decay brightness Number of subhalos brighter than a given flux/ J-factor: # of subhalos brighter than J Nsub( D) flux > 100 GeV in Crab units for! b b, =10 26 s, m = 500 GeV % of the sky, dwarf-like objects included Sculptor dsphg Astrophysical D-factor in log 10 (D/GeV cm 2 ) CTA survey sensitivity model 1 model 2 model 3 model 4 model 5 model 6 model 4 parameters 7 model 168 models model dashed 9 lines: model higher 10 c(m) model 11 model 12 model 13 model 14 model 15 model 16 work done by Rungployphan Kieokaew, 2015!29

Dark matter annihilation and decay factors in the Milky Way s dwarf spheroidal galaxies

Dark matter annihilation and decay factors in the Milky Way s dwarf spheroidal galaxies Dark matter annihilation and decay factors in the Milky Way s dwarf spheroidal galaxies Vincent Bonnivard bonnivard@lpsc.in2p3.fr TAUP 2015 07/09/15 Collaborators: D. Maurin, C. Combet, M. G. Walker, A.

More information

Indirect dark matter searches with the Cherenkov Telescope Array

Indirect dark matter searches with the Cherenkov Telescope Array Indirect dark matter searches with the Cherenkov Telescope Array Jennifer Gaskins GRAPPA, University of Amsterdam for the CTA Consortium For more details, please see: arxiv:1508.06128 Carr et al. 2015

More information

Emmanuel Moulin! on behalf of the CTA Consortium!!! Rencontres de Moriond 2013! Very High Energy Phenomena in the Universe! March 9-16, La Thuile,

Emmanuel Moulin! on behalf of the CTA Consortium!!! Rencontres de Moriond 2013! Very High Energy Phenomena in the Universe! March 9-16, La Thuile, Emmanuel Moulin! on behalf of the CTA Consortium!!! Rencontres de Moriond 2013! Very High Energy Phenomena in the Universe! March 9-16, La Thuile, Italy Emmanuel Moulin CTA meeting, Zürich 2009 1 Core-energy

More information

CLUMPY: A public code for γ-ray and ν signals from dark matter structures.

CLUMPY: A public code for γ-ray and ν signals from dark matter structures. CLUMPY: A public code for γ-ray and ν signals from dark matter structures. Moritz Hütten, DESY Zeuthen for the CLUMPY developers: Vincent Bonnivard, Moritz Hütten, Emmanuel Nezri, Aldée Charbonnier, Céline

More information

the CTA Consortium represented by Aldo Morselli

the CTA Consortium represented by Aldo Morselli The Dark Matter Programme of the Cherenkov Telescope Array the CTA Consortium represented by Aldo Morselli INFN Roma Tor Vergata 1 CTA PROJECT Next generation ground based Gamma-ray observatory Open observatory

More information

THE MAGIC TELESCOPES. Major Atmospheric Gamma Imaging Cherenkov Telescopes

THE MAGIC TELESCOPES. Major Atmospheric Gamma Imaging Cherenkov Telescopes THE MAGIC TELESCOPES Observatorio del Roque de los Muchachos, La Palma (2200 m a.s.l.) System of two 17 m Cherenkov Telescopes for VHE γ-ray astronomy MAGIC-I operational since 2004, Stereo system since

More information

A New View of the High-Energy γ-ray Sky with the Fermi Telescope

A New View of the High-Energy γ-ray Sky with the Fermi Telescope A New View of the High-Energy γ-ray Sky with the Fermi Telescope Aurelien Bouvier KIPAC/SLAC, Stanford University On behalf of the Fermi collaboration SNOWPAC, 2010 The Fermi observatory Launch: June 11

More information

Gamma-ray background anisotropy from Galactic dark matter substructure

Gamma-ray background anisotropy from Galactic dark matter substructure Gamma-ray background anisotropy from Galactic dark matter substructure Shin ichiro Ando (TAPIR, Caltech) Ando, arxiv:0903.4685 [astro-ph.co] 1. Introduction Dark matter annihilation and substructure Dark

More information

Constraints on dark matter annihilation cross section with the Fornax cluster

Constraints on dark matter annihilation cross section with the Fornax cluster DM Workshop@UT Austin May 7, 2012 Constraints on dark matter annihilation cross section with the Fornax cluster Shin ichiro Ando University of Amsterdam Ando & Nagai, arxiv:1201.0753 [astro-ph.he] Galaxy

More information

DM subhalos: The obser vational challenge

DM subhalos: The obser vational challenge DM subhalos: The obser vational challenge Hannes-S. Zechlin and Dieter Horns Inst. f. Experimentalphysik, Universität Hamburg, Germany July 26th, 2012 DM subhalos in the Milky Way concordance cosmology

More information

Indirect Dark Matter Detection with Dwarf Galaxies

Indirect Dark Matter Detection with Dwarf Galaxies Indirect Dark Matter Detection with Dwarf Galaxies Neelima Sehgal KIPAC-SLAC/Stanford SnowPAC, Utah 2010 Rouven Essig, NS, Louis Strigari, arxiv: 0902.4750, PRD 80, 023506 (2009) Rouven Essig, NS, Louis

More information

The Inner Region of the Milky Way Galaxy in High Energy Gamma Rays

The Inner Region of the Milky Way Galaxy in High Energy Gamma Rays The Inner Region of the Milky Way Galaxy in High Energy Gamma Rays Simona Murgia, SLAC-KIPAC for the Fermi LAT Collaboration Dark Matter Signatures in the Gamma-ray Sky Austin, Texas 7-8 May 2012 arxiv:0908.0195

More information

The Cherenkov Telescope Array (CTA)

The Cherenkov Telescope Array (CTA) The Cherenkov Telescope Array (CTA) The CTA Consortium1, represented by Andreas Reisenegger2 1 2 see http://www.cta observatory.org/consortium_authors/authors_2018_01.html for full author list Instituto

More information

Tesla Jeltema. Assistant Professor, Department of Physics. Observational Cosmology and Astroparticle Physics

Tesla Jeltema. Assistant Professor, Department of Physics. Observational Cosmology and Astroparticle Physics Tesla Jeltema Assistant Professor, Department of Physics Observational Cosmology and Astroparticle Physics Research Program Research theme: using the evolution of large-scale structure to reveal the fundamental

More information

The Inner Region of the Milky Way Galaxy in High Energy Gamma Rays

The Inner Region of the Milky Way Galaxy in High Energy Gamma Rays The Inner Region of the Milky Way Galaxy in High Energy Gamma Rays Simona Murgia, SLAC-KIPAC for the Fermi LAT Collaboration UCLA Dark Matter 2012 Marina del Rey 22-24 February 2012 arxiv:0908.0195 Gamma

More information

Signal Model vs. Observed γ-ray Sky

Signal Model vs. Observed γ-ray Sky Signal Model vs. Observed γ-ray Sky Springel+, Nature (2008) Two main dark matter signal components: 1. galactocentric diffuse 2. small structures Observed sky modeled with bremsstrahlung π 0 decay up-scattered

More information

Using the Fermi-LAT to Search for Indirect Signals from Dark Matter Annihilation

Using the Fermi-LAT to Search for Indirect Signals from Dark Matter Annihilation Using the Fermi-LAT to Search for Indirect Signals from Dark Matter Annihilation Tim Linden UC - Santa Cruz Representing the Fermi-LAT Collaboration with acknowledgements to: Brandon Anderson, Elliott

More information

Search Results and Prospects from Atmospheric Cherenkov Telescopes. Andrew W Smith University of Marland, College Park / NASA GSFC

Search Results and Prospects from Atmospheric Cherenkov Telescopes. Andrew W Smith University of Marland, College Park / NASA GSFC Search Results and Prospects from Atmospheric Cherenkov Telescopes Andrew W Smith University of Marland, College Park / NASA GSFC From P5 report (Cosmic Frontier) Arrenberg et al. Indirect Detection probes

More information

Recent highlights from VERITAS

Recent highlights from VERITAS Recent highlights from VERITAS K. Ragan McGill University RICAP 2011, Rome, 26-May-2011 K. Ragan VERITAS RICAP '11 1 Outline Very high-energy (VHE) gamma-ray astrophysics Ground-based observations with

More information

Hunting for Dark Matter in Anisotropies of Gamma-ray Sky: Theory and First Observational Results from Fermi-LAT

Hunting for Dark Matter in Anisotropies of Gamma-ray Sky: Theory and First Observational Results from Fermi-LAT Hunting for Dark Matter in Anisotropies of Gamma-ray Sky: Theory and First Observational Results from Fermi-LAT Eiichiro Komatsu (Texas Cosmology Center, Univ. of Texas at Austin) MPA Seminar, September

More information

Searching for Dark Matter in the Galactic Center with Fermi LAT: Challenges

Searching for Dark Matter in the Galactic Center with Fermi LAT: Challenges Searching for Dark Matter in the Galactic Center with Fermi LAT: Challenges Simona Murgia University of California, Irvine Debates on the Nature of Dark Matter Sackler 2014 19-22 May 2014 arxiv:0908.0195

More information

Structure of Dark Matter Halos

Structure of Dark Matter Halos Structure of Dark Matter Halos Dark matter halos profiles: DM only: NFW vs. Einasto Halo concentration: evolution with time Dark matter halos profiles: Effects of baryons Adiabatic contraction Cusps and

More information

Miguel A. Sánchez Conde (Instituto de Astrofísica de Canarias)

Miguel A. Sánchez Conde (Instituto de Astrofísica de Canarias) Miguel A. Sánchez Conde (Instituto de Astrofísica de Canarias) In collaboration with: F. Prada, A. Cuesta, A. Domínguez, M. Fornasa, F. Zandanel (IAA/CSIC) E. Bloom, D. Paneque (KIPAC/SLAC) M. Gómez, M.

More information

Very High-Energy Gamma- Ray Astrophysics

Very High-Energy Gamma- Ray Astrophysics Very High-Energy Gamma- Ray Astrophysics David A. Williams Santa Cruz Institute for Particle Physics UC Santa Cruz Quarknet July 12, 2013 Detecting High Energy Gamma Rays High Sensitivity HESS, MAGIC,

More information

The VERITAS Dark M atter and Astroparticle Programs. Benjamin Zitzer For The VERITAS Collaboration

The VERITAS Dark M atter and Astroparticle Programs. Benjamin Zitzer For The VERITAS Collaboration The VERITAS Dark M atter and Astroparticle Programs Benjamin Zitzer For The VERITAS Collaboration Introduction to VERITAS Array of four IACTs in Southern AZ, USA Employs ~100 Scientists in five countries

More information

Enhancement of Antimatter Signals from Dark Matter Annihilation

Enhancement of Antimatter Signals from Dark Matter Annihilation Enhancement of Antimatter Signals from Dark Matter Annihilation around Intermediate Mass Black Holes Pierre Brun Laboratoire d Annecy-le-vieux de Physique des Particules CNRS/IN2P3/Université de Savoie

More information

Constraining Galactic dark matter in the Fermi-LAT sky with photon counts statistics

Constraining Galactic dark matter in the Fermi-LAT sky with photon counts statistics Constraining Galactic dark matter in the Fermi-LAT sky with photon counts statistics Moriond Cosmology 2018 Silvia Manconi (University of Turin & INFN) March 20, 2018 In collaboration with: Hannes Zechlin,

More information

The Cherenkov Telescope Array

The Cherenkov Telescope Array The Cherenkov Telescope Array Gamma-ray particle astrophysics Dark Matter Space time Cosmic rays...? Gamma-ray particle astrophysics Dark Matter Space time Cosmic rays...? Particle Dark Matter Direct Detection

More information

Probing Dark Matter in Galaxy Clusters using Neutrinos

Probing Dark Matter in Galaxy Clusters using Neutrinos Indirect Detection - Parallel Session I IDM 2012, Chicago Probing Dark Matter in Galaxy Clusters using Neutrinos In Collaboration with Ranjan Laha, arxiv/1206.1322 + PRD Basudeb Dasgupta CCAPP, Ohio State

More information

Cross-Correlation of Cosmic Shear and Extragalactic Gamma-ray Background

Cross-Correlation of Cosmic Shear and Extragalactic Gamma-ray Background Cross-Correlation of Cosmic Shear and Extragalactic Gamma-ray Background Masato Shirasaki (Univ. of Tokyo) with Shunsaku Horiuchi (UCI), Naoki Yoshida (Univ. of Tokyo, IPMU) Extragalactic Gamma-Ray Background

More information

Indirect Detection of Dark Matter with Gamma Rays

Indirect Detection of Dark Matter with Gamma Rays Indirect Detection of Dark Matter with Gamma Rays Simona Murgia SLAC-KIPAC University of California, Irvine on behalf of the Fermi LAT Collaboration Dark Attack 212 Ascona, Switzerland 15-2 July 212 WIMP

More information

Princeton December 2009 The fine-scale structure of dark matter halos

Princeton December 2009 The fine-scale structure of dark matter halos Princeton December 2009 The fine-scale structure of dark matter halos Simon White Max Planck Institute for Astrophysics The dark matter structure of CDM halos A rich galaxy cluster halo Springel et al

More information

Gamma-ray Observations of Galaxy Clusters!

Gamma-ray Observations of Galaxy Clusters! Gamma-ray Observations of Galaxy Clusters! a! Fabio Zandanel! (GRAPPA Institute University of Amsterdam)! f.zandanel@uva.nl! SnowCluster 2015 The Physics Of Galaxy Clusters! Snowbird (Utah, US) March 15-20,

More information

Cherenkov Telescope Array

Cherenkov Telescope Array Cherenkov Telescope Array Giovanni Lamanna (on behalf of the CTA consortium) LAPP - Laboratoire d'annecy-le-vieux de Physique des Particules, Université de Savoie, CNRS/IN2P3, Annecy-le-Vieux, France Rencontres

More information

Constraining Dark Matter annihilation with the Fermi-LAT isotropic gamma-ray background

Constraining Dark Matter annihilation with the Fermi-LAT isotropic gamma-ray background Constraining Dark Matter annihilation with the Fermi-LAT isotropic gamma-ray background Fiorenza Donato @ Physics Dept., Un. Torino The gamma-ray sky - Minneapolis, October 10, 2013 Plan of my talk What

More information

Searching for spectral features in the g-ray sky. Alejandro Ibarra Technische Universität München

Searching for spectral features in the g-ray sky. Alejandro Ibarra Technische Universität München Searching for spectral features in the g-ray sky Alejandro Ibarra Technische Universität München Oslo 5 November 2014 Outline Motivation Indirect dark matter searches with gamma-rays. Overcoming backgrounds

More information

The Galactic diffuse gamma ray emission in the energy range 30 TeV 3 PeV

The Galactic diffuse gamma ray emission in the energy range 30 TeV 3 PeV The Galactic diffuse gamma ray emission in the energy range 30 TeV 3 PeV Mount Rainier by Will Christiansen Silvia Vernetto & Paolo Lipari 35th ICRC 12-20 July 2017 - Busan - South Korea Gamma ray astronomy

More information

Indirect dark matter detection and the Galactic Center GeV Excess

Indirect dark matter detection and the Galactic Center GeV Excess Image Credit: Springel et al. 2008 Indirect dark matter detection and the Galactic Center GeV Excess Jennifer Siegal-Gaskins Caltech Image Credit: Springel et al. 2008 Jennifer Siegal-Gaskins Caltech Image

More information

VERITAS Observations of Starburst Galaxies. The Discovery of VHE Gamma Rays from a Starburst Galaxy

VERITAS Observations of Starburst Galaxies. The Discovery of VHE Gamma Rays from a Starburst Galaxy VERITAS Observations of Starburst Galaxies The Discovery of VHE Gamma Rays from a Starburst Galaxy Wystan Benbow for the VERITAS Collaboration 1 Harvard-Smithsonian Center for Astrophysics 1 see R.A. Ong

More information

Impact of substructures on predictions of dark matter annihilation signals

Impact of substructures on predictions of dark matter annihilation signals Impact of substructures on predictions of dark matter annihilation signals Julien Lavalle Institute & Dept. of Theoretical Physics, Madrid Aut. Univ. & CSIC DESY Theory Astroparticle, Hamburg 16 V 2011

More information

Searching for Dark Matter Annihilation from Milky Way Dwarf Spheroidal Galaxies. Present status and future prospects

Searching for Dark Matter Annihilation from Milky Way Dwarf Spheroidal Galaxies. Present status and future prospects Searching for Dark Matter Annihilation from Milky Way Dwarf Spheroidal Galaxies. Present status and future prospects Aldo Morselli INFN Roma Tor Vergata CTA in the quest for Dark Matter and exotic phenomena

More information

Andrea Albert (The Ohio State University) on behalf of The Fermi LAT Collaboration. HEP Seminar University of Virginia 12/05/12

Andrea Albert (The Ohio State University) on behalf of The Fermi LAT Collaboration. HEP Seminar University of Virginia 12/05/12 Indirect Searches for Dark Matter with the Fermi Large Area Telescope Andrea Albert (The Ohio State University) on behalf of The Fermi LAT Collaboration HEP Seminar University of Virginia 12/05/12 Outline

More information

Cherenkov Telescope Array Status Report. Salvatore Mangano (CIEMAT) On behalf of the CTA consortium

Cherenkov Telescope Array Status Report. Salvatore Mangano (CIEMAT) On behalf of the CTA consortium Cherenkov Telescope Array Status Report Salvatore Mangano (CIEMAT) On behalf of the CTA consortium Outline Very-High-Energy Gamma-Ray Astronomy Cherenkov Telescope Array (CTA) Expected Performance of CTA

More information

Fundamental Physics with GeV Gamma Rays

Fundamental Physics with GeV Gamma Rays Stefano Profumo UC Santa Cruz Santa Cruz Institute for Particle Physics T.A.S.C. [Theoretical Astrophysics, Santa Cruz] Fundamental Physics with GeV Gamma Rays Based on: Kamionkowski & SP, 0810.3233 (subm.

More information

EGRET Excess of diffuse Galactic Gamma Rays as a Trace of the Dark Matter Halo

EGRET Excess of diffuse Galactic Gamma Rays as a Trace of the Dark Matter Halo EGRET Excess of diffuse Galactic Gamma Rays as a Trace of the Dark Matter Halo Indirect Search for Dark Matter W. de Boer 1, I. Gebauer 1, A.V. Gladyshev 2, D. Kazakov 2, C. Sander 1, V. Zhukov 1 1 Institut

More information

Status of the MAGIC telescopes

Status of the MAGIC telescopes SNOWPAC 2010 Status of the MAGIC telescopes Pierre Colin for the MAGIC collaboration Max-Planck-Institut für physik (Munich) Status of the MAGIC telescopes MAGIC-1 MAGIC-2 Outline: Recent results of the

More information

Probing Dark Matter with Cosmic Messengers

Probing Dark Matter with Cosmic Messengers Probing Dark Matter with Cosmic Messengers Andrea Albert Los Alamos National Lab 3rd KMI International Symposium January 6, 2017 Outline Indirect Detection Overview evidence for dark matter dark matter

More information

Non-detection of the 3.55 kev line from M31/ Galactic center/limiting Window with Chandra

Non-detection of the 3.55 kev line from M31/ Galactic center/limiting Window with Chandra Non-detection of the 3.55 kev line from M31/ Galactic center/limiting Window with Chandra Meng Su (MIT)! Pappalardo/Einstein fellow!! In Collaboration with Zhiyuan Li (NJU)!! 15 Years of Science with Chandra!

More information

Latest Results on Dark Matter and New Physics Searches with Fermi. Simona Murgia, SLAC-KIPAC on behalf of the Fermi-LAT Collaboration

Latest Results on Dark Matter and New Physics Searches with Fermi. Simona Murgia, SLAC-KIPAC on behalf of the Fermi-LAT Collaboration Latest Results on Dark Matter and New Physics Searches with Fermi Simona Murgia, SLAC-KIPAC on behalf of the Fermi-LAT Collaboration TeV Particle Astrophysics 2009 SLAC, July 13-16 2009 DM and New Physics

More information

Prospects for indirect dark matter detection with Fermi and IACTs

Prospects for indirect dark matter detection with Fermi and IACTs Prospects for indirect dark matter detection with Fermi and IACTs Francesc Ferrer Washington University in St. Louis TeV Particle Astrophysics, SLAC, July 2009 Signals of Dark Matter (DM) at γ ray telescopes

More information

Nikolay Topchiev for the GAMMA-400 Collaboration High-energy gamma-ray studying with GAMMA-400

Nikolay Topchiev for the GAMMA-400 Collaboration High-energy gamma-ray studying with GAMMA-400 Nikolay Topchiev for the GAMMA-400 Collaboration High-energy gamma-ray studying with GAMMA-400 July 12-20, 2017, ICRC2017, Busan, Korea High-energy gamma-ray studying Distribution of 3033 discrete sources

More information

arxiv: v1 [astro-ph.im] 27 Aug 2012

arxiv: v1 [astro-ph.im] 27 Aug 2012 Dark Matter and Fundamental Physics with the Cherenkov Telescope Array M. Doro j,1, J. Conrad g,h,1, D. Emmanoulopoulos k, M. A. Sànchez-Conde q, J.A. Barrio a, E. Birsin b, J. Bolmont c, P. Brun d, S.

More information

Astroparticle Physics with IceCube

Astroparticle Physics with IceCube Astroparticle Physics with IceCube Nick van Eijndhoven nickve.nl@gmail.com http://w3.iihe.ac.be f or the IceCube collaboration Vrije Universiteit Brussel - IIHE(ULB-VUB) Pleinlaan 2, B-1050 Brussel, Belgium

More information

Indirect searches for dark matter with the Fermi LAT instrument

Indirect searches for dark matter with the Fermi LAT instrument Indirect searches for dark matter with the Fermi LAT instrument M. Nicola Mazziotta INFN-Bari mazziotta@ba.infn.it 2nd international workshop on HERD Beijing Dec 2-3, 2013 Indirect Dark Matter Search +

More information

M. Lattanzi. 12 th Marcel Grossmann Meeting Paris, 17 July 2009

M. Lattanzi. 12 th Marcel Grossmann Meeting Paris, 17 July 2009 M. Lattanzi ICRA and Dip. di Fisica - Università di Roma La Sapienza In collaboration with L. Pieri (IAP, Paris) and J. Silk (Oxford) Based on ML, Silk, PRD 79, 083523 (2009) and Pieri, ML, Silk, MNRAS

More information

The Cherenkov Telescope Array. Kevin Meagher Georgia Institute of Technology

The Cherenkov Telescope Array. Kevin Meagher Georgia Institute of Technology The Cherenkov Telescope Array Kevin Meagher Georgia Institute of Technology Outline VHE Gamma Ray Astronomy CTA Overview Science Goals for CTA Schwarzschild-Couder Telescope Extension 2 Gamma-ray Astronomy

More information

Searches for WIMP annihilation with GLAST

Searches for WIMP annihilation with GLAST SLAC-PUB-11289 Searches for WIMP annihilation with GLAST Larry Wai Stanford Linear Accelerator Center, Stanford, California representing the GLAST LAT Collaboration Abstract We describe signatures for

More information

On the scientific motivation for a wide field-of-view TeV gamma-ray observatory in the Southern Hemisphere

On the scientific motivation for a wide field-of-view TeV gamma-ray observatory in the Southern Hemisphere On the scientific motivation for a wide field-of-view TeV gamma-ray observatory in the Southern Hemisphere for the HAWC collaboration E-mail: miguel@psu.edu Observations of high energy gamma rays are an

More information

Astrometric Microlensing by Local Dark Matter Subhalos

Astrometric Microlensing by Local Dark Matter Subhalos Astrometric Microlensing by Local Dark Matter Subhalos Adrienne Erickcek CITA & Perimeter Institute with Nicholas Law University of Toronto Dunlap Institute arxiv: 17.4228 ApJ in press Dark Matter Halos

More information

Selecting Interesting Unidentified Sources

Selecting Interesting Unidentified Sources Selecting Interesting Unidentified Sources Robert Wagner Max-Planck-Institut für Physik, München and Excellence Cluster Origin and Structure of the Universe, Garching b. München Standard origin of TeV

More information

Astroparticle Physics

Astroparticle Physics Astroparticle Physics 43 (013) 189 14 Contents lists available at SciVerse ScienceDirect Astroparticle Physics journal homepage: www.elsevier.com/locate/astropart Dark matter and fundamental physics with

More information

Measuring Dark Matter Properties with High-Energy Colliders

Measuring Dark Matter Properties with High-Energy Colliders Measuring Dark Matter Properties with High-Energy Colliders The Dark Matter Problem The energy density of the universe is mostly unidentified Baryons: 5% Dark Matter: 20% Dark Energy: 75% The dark matter

More information

Sep. 13, JPS meeting

Sep. 13, JPS meeting Recent Results on Cosmic-Rays by Fermi-LAT Sep. 13, 2010 @ JPS meeting Tsunefumi Mizuno (Hiroshima Univ.) On behalf of the Fermi-LAT collaboration 1 Outline Introduction Direct measurement of CRs CRs in

More information

Constraining dark matter signal from a combined analysis of Milky Way satellites using the Fermi-LAT arxiv: v1 [astro-ph.

Constraining dark matter signal from a combined analysis of Milky Way satellites using the Fermi-LAT arxiv: v1 [astro-ph. Constraining dark matter signal from a combined analysis of Milky Way satellites using the Fermi-LAT arxiv:1102.5701v1 [astro-ph.he] 28 Feb 2011 Stockholm University E-mail: maja.garde@fysik.su.se On behalf

More information

Searching for dark matter annihilation lines with HESS II. Knut Dundas Morå for the HESS collaboration

Searching for dark matter annihilation lines with HESS II. Knut Dundas Morå for the HESS collaboration Searching for dark matter annihilation lines with HESS II Knut Dundas Morå for the HESS collaboration Outline Indirect Dark Matter detection Dark Matter signatures Dark Matter distributions Fermi Line

More information

Measurement of the CR e+/e- ratio with ground-based instruments

Measurement of the CR e+/e- ratio with ground-based instruments Measurement of the CR e+/e- ratio with ground-based instruments Pierre Colin Max-Planck-Institut für Physik CR Moon shadow MPP retreat - 21 January 2014 Cosmic ray electrons Observation: Above the atmosphere:

More information

Ruling out thermal dark matter with a black hole induced spiky profile in the M87 galaxy

Ruling out thermal dark matter with a black hole induced spiky profile in the M87 galaxy Ruling out thermal dark matter with a black hole induced spiky profile in the M87 galaxy Based on arxiv:1505.00785 (IAP, Paris) in collaboration with Joseph Silk (IAP) & Céline Bœhm (IPPP, Durham) PACIFIC

More information

Resolving the Extragalactic γ-ray Background

Resolving the Extragalactic γ-ray Background Resolving the Extragalactic γ-ray Background Marco Ajello Clemson University On behalf of the Fermi-LAT collab. (with a few additions by Jack) Ackermann+2015, ApJ, 799, 86 Ajello+2015, ApJL, 800,27 Ackermann+2016,

More information

Indirect Dark Matter Searches: a Review Eric Charles SLAC National Lab.

Indirect Dark Matter Searches: a Review Eric Charles SLAC National Lab. Indirect Dark Matter Searches: a Review Eric Charles SLAC National Lab. 13 eme Recontres de Vietnam: Exploring the Dark Universe 24 July 2017, Quy Nhon, Vietnam Outline 2 I. Review / Context: indirect

More information

Fermi-LAT Analysis of the Coma Cluster

Fermi-LAT Analysis of the Coma Cluster Fermi-LAT Analysis of the Coma Cluster a Fabio Zandanel GRAPPA Institute University of Amsterdam f.zandanel@uva.nl In collaboration with S. Ando (GRAPPA) 18 th Symposium on Astroparticle Physics in the

More information

EBL Studies with the Fermi Gamma-ray Space Telescope

EBL Studies with the Fermi Gamma-ray Space Telescope EBL Studies with the Fermi Gamma-ray Space Telescope Luis C. Reyes KICP The Extragalactic Background Light (EBL) What is it? Accumulation of all energy releases in the form of electromagnetic radiation.

More information

Indirect Dark Matter Searches in the Milky Way Center with the LAT on board Fermi

Indirect Dark Matter Searches in the Milky Way Center with the LAT on board Fermi Indirect Dark Matter Searches in the Milky Way Center with the LAT on board Fermi B. Cañadas, A. Morselli and V. Vitale on behalf of the Fermi LAT Collaboration Outline Gamma rays from Dark Matter Dark

More information

Formation and evolution of CDM halos and their substructure

Formation and evolution of CDM halos and their substructure Formation and evolution of CDM halos and their substructure 1) cold dark matter and structures on all scales 2) via lactea, z=0 results 3) subhalo evolution Jürg Diemand UC Santa Cruz 4) DM annihilation

More information

Searching for dark matter. with gamma-ray anisotropies

Searching for dark matter. with gamma-ray anisotropies Image Credit: NASA/DOE/International LAT Team Searching for dark matter with gamma-ray anisotropies Jennifer Siegal-Gaskins CCAPP, Ohio State University with Brandon Hensley (Caltech!Princeton) Eiichiro

More information

Highlights from the Fermi Symposium

Highlights from the Fermi Symposium Highlights from the Fermi Symposium Aldo Morselli INFN Roma Tor Vergata 1 The LAT at 2 Years and 17 days from the 3 rd!!! 11 June 2008 2 Fermi is Making a Major Impact Science, December 2009 Breakthrough

More information

Gamma-ray Astrophysics

Gamma-ray Astrophysics Gamma-ray Astrophysics AGN Pulsar SNR GRB Radio Galaxy The very high energy -ray sky NEPPSR 25 Aug. 2004 Many thanks to Rene Ong at UCLA Guy Blaylock U. of Massachusetts Why gamma rays? Extragalactic Background

More information

Masses of Dwarf Satellites of the Milky Way

Masses of Dwarf Satellites of the Milky Way Masses of Dwarf Satellites of the Milky Way Manoj Kaplinghat Center for Cosmology UC Irvine Collaborators: Greg Martinez Quinn Minor Joe Wolf James Bullock Evan Kirby Marla Geha Josh Simon Louie Strigari

More information

Searching for WIMPs in deep radio observations of Gl Galactic dsphs

Searching for WIMPs in deep radio observations of Gl Galactic dsphs Searching for WIMPs in deep radio observations of Gl Galactic dsphs m x = 10 GV GeV XX e+/e D o = 0.1*MW Excluded d( (2σ) 05deg 0.5 th Kristine Spekkens (RMC) Brian Mason (NRAO), James Aguirre (UPenn),

More information

4. Structure of Dark Matter halos. Hence the halo mass, virial radius, and virial velocity are related by

4. Structure of Dark Matter halos. Hence the halo mass, virial radius, and virial velocity are related by 13-4-12see http://www.strw.leidenuniv.nl/ franx/college/galaxies12 12-c04-1 13-4-12see http://www.strw.leidenuniv.nl/ franx/college/galaxies12 12-c04-2 4. Structure of Dark Matter halos Obviously, we cannot

More information

VERITAS Performance Gernot Maier

VERITAS Performance Gernot Maier VERITAS Performance Gernot Maier Alliance for Astroparticle Physics What scientific impact will VERITAS have in the next 3-5 years? Galactic long-term plan Performance Operations LTP & Performance May

More information

arxiv: v1 [astro-ph.he] 10 Jul 2009

arxiv: v1 [astro-ph.he] 10 Jul 2009 July, 2009 7:46 WSPC - Proceedings Trim Size: 9in x 6in DMsearches IACTs 1 arxiv:0907.1747v1 [astro-ph.he] Jul 2009 DARK MATTER SEARCHES WITH IMAGING ATMOSPHERIC CHERENKOV TELESCOPES E. MOULIN CEA -Saclay,

More information

ElisaBete de Gouveia Dal Pino (IAG-USP) On behalf of the CTA Collaboration

ElisaBete de Gouveia Dal Pino (IAG-USP) On behalf of the CTA Collaboration ElisaBete de Gouveia Dal Pino (IAG-USP) On behalf of the CTA Collaboration UFES,Vitoria, 8 de Outubro, 2018 TeV sky today (~212 sources, 62 unidentified) tevcat.uchicago.edu/ Supernovae Pulsar wind neb.

More information

A search for dark matter annihilation in the newly discovered dwarf galaxy Reticulum II

A search for dark matter annihilation in the newly discovered dwarf galaxy Reticulum II Note. Best-fit parameters from the maximum-likelihood fit assuming the composite isochrone described in Section 3.2. Uncertainties are calculated from the the highest density interval containing 90% of

More information

4. Structure of Dark Matter halos. Hence the halo mass, virial radius, and virial velocity are related by

4. Structure of Dark Matter halos. Hence the halo mass, virial radius, and virial velocity are related by 6-4-10see http://www.strw.leidenuniv.nl/ franx/college/galaxies10 10-c04-1 6-4-10see http://www.strw.leidenuniv.nl/ franx/college/galaxies10 10-c04-2 4. Structure of Dark Matter halos Obviously, we cannot

More information

Dark matter indirect searches: Multi-wavelength and anisotropies

Dark matter indirect searches: Multi-wavelength and anisotropies Journal of Physics: Conference Series PAPER OPEN ACCESS Dark matter indirect searches: Multi-wavelength and anisotropies To cite this article: Shin ichiro Ando 2016 J. Phys.: Conf. Ser. 718 022002 Related

More information

Positron Annihilation in the Milky Way and beyond

Positron Annihilation in the Milky Way and beyond Positron Annihilation in the Milky Way and beyond Thomas Siegert, MPE Garching R. Diehl, A. C. Vincent, F. Guglielmetti, M. G. H. Krause, C. Boehm Research Area G Science Day, October 20 th 2016 Positron

More information

Gamma-Ray Astronomy from the Ground

Gamma-Ray Astronomy from the Ground Gamma-Ray Astronomy from the Ground Dieter Horns University of Hamburg Introduction - summary Many new Results from ICRC 2015 No we haven't discovered dark matter, yet Yes we have discovered sources of

More information

Dark Matter Distributions of the Milky Way Satellites and Implications for Indirect Detection

Dark Matter Distributions of the Milky Way Satellites and Implications for Indirect Detection Dark Matter Distributions of the Milky Way Satellites and Implications for Indirect Detection Kavli Institue for Particle Astrophysics and Cosmology, Physics Department, Stanford University, Stanford,

More information

PoS(ICRC2017)904. The VERITAS Dark Matter Program. Benjamin Zitzer. for the VERITAS Collaboration Affiliation

PoS(ICRC2017)904. The VERITAS Dark Matter Program. Benjamin Zitzer. for the VERITAS Collaboration Affiliation The VERITAS Dark Matter Program McGill University E-mail: bzitzer@physics.mcgill.ca for the VERITAS Collaboration Affiliation E-mail: bzitzer@physics.mcgill.ca In the cosmological paradigm, cold dark matter

More information

Astrophysical issues in indirect DM detection

Astrophysical issues in indirect DM detection Astrophysical issues in indirect DM detection Julien Lavalle CNRS Lab. Univers & Particules de Montpellier (LUPM), France Université Montpellier II CNRS-IN2P3 (UMR 5299) Service de Physique Théorique Université

More information

DARK MATTER ANNIHILATION AT THE GALACTIC CENTER?

DARK MATTER ANNIHILATION AT THE GALACTIC CENTER? Complementarity Between Dark Matter Searches and Collider Experiments, UC Irvine, June 11, 2006 DARK MATTER ANNIHILATION AT THE GALACTIC CENTER? Joel Primack University of California, Santa Cruz The Milky

More information

Recent Results on Dark Matter Searches with Fermi. Simona Murgia, SLAC-KIPAC on behalf of the Fermi-LAT Collaboration

Recent Results on Dark Matter Searches with Fermi. Simona Murgia, SLAC-KIPAC on behalf of the Fermi-LAT Collaboration Recent Results on Dark Matter Searches with Fermi Simona Murgia, SLAC-KIPAC on behalf of the Fermi-LAT Collaboration KITP-UCSB 8 December 2009 The Observatory Observe the gamma-ray sky in the 20 MeV to

More information

Ruling out dark matter interpretation of the galactic GeV excess by gamma-ray data of galaxy clusters

Ruling out dark matter interpretation of the galactic GeV excess by gamma-ray data of galaxy clusters www.nature.com/scientificreports Received: 3 August 07 Accepted: 8 October 07 Published: xx xx xxxx OPEN Ruling out dark matter interpretation of the galactic GeV excess by gamma-ray data of galaxy clusters

More information

Fossils of the First Galaxies in the Local Group: True Fossils and Ghost Halos

Fossils of the First Galaxies in the Local Group: True Fossils and Ghost Halos Fossils of the First Galaxies in the Local Group: True Fossils and Ghost Halos Mia S. Bovill with Massimo Ricotti University of Maryland The Smallest Galaxies Minihalos DO NOT initiate gas condensation

More information

TeV Future: APS White Paper

TeV Future: APS White Paper TeV Future: APS White Paper APS commissioned a white paper on the "Status and Future of very high energy gamma ray astronomy. For preliminary information, see http://cherenkov.physics.iastate.edu/wp Working

More information

Particle Acceleration in the Universe

Particle Acceleration in the Universe Particle Acceleration in the Universe Hiroyasu Tajima Stanford Linear Accelerator Center Kavli Institute for Particle Astrophysics and Cosmology on behalf of SLAC GLAST team June 7, 2006 SLAC DOE HEP Program

More information

Testing a DM explanation of the positron excess with the Inverse Compton scattering

Testing a DM explanation of the positron excess with the Inverse Compton scattering Testing a DM explanation of the positron excess with the Inverse Compton scattering Gabrijela Zaharijaš Oskar Klein Center, Stockholm University Work with A. Sellerholm, L. Bergstrom, J. Edsjo on behalf

More information

Determining the Nature of Dark Matter with Astrometry

Determining the Nature of Dark Matter with Astrometry Determining the Nature of Dark Matter with Astrometry Louie Strigari UC Irvine Center for Cosmology Fermilab, 4.16.2007 Collaborators: James Bullock, Juerg Diemand, Manoj Kaplinghat, Michael Kuhlen, Piero

More information

Fermi measurements of diffuse gamma-ray emission: results at the first-year milestone

Fermi measurements of diffuse gamma-ray emission: results at the first-year milestone SciNeGHE 2009 Assisi, October 7th Fermi measurements of diffuse gamma-ray emission: results at the first-year milestone Luigi Tibaldo luigi.tibaldo@pd.infn.it INFN Sezione di Padova Dip. di Fisica G. Galilei,

More information

Dark Matter in the Galactic Center

Dark Matter in the Galactic Center Dark Matter in the Galactic Center Tim Linden University of Chicago along with: Eric Carlson, Ilias Cholis, Dan Hooper, Manoj Kaplinghat, Stefano Profumo, Jennifer Siegal-Gaskins, Tracy Slatyer, Hai-Bo

More information