Koji Ichikawa. Prospects on the indirect dark matter detection and a future spectroscopic survey of dwarf spheroidal galaxies.

Similar documents
Koji Ichikawa In collaboration with Kohei Hayashi, Masahiro Ibe, Miho N. Ishigaki, Shigeki Matsumoto and Hajime Sugai.

Koji Ichikawa. (In preparation) TAUP, Torino, Sep. 7-11, 2015

Future DM indirect detection in dwarf spheroidal galaxies and Foreground effect on the J-factor estimation Koji Ichikawa

Robust estimate of the dark matter halo of the Milky-way's dwarf spheroidal galaxies

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

Shigeki Matsumoto (Kavli IPMU)

Wino dark matter breaks the siege

Sommerfeld-Enhanced J-Factors for Dwarf Spheroidal Galaxies

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

Milky Way Satellite Galaxy Kinematics and Scaling Relations for Dark Matter Searches. Andrew B. Pace. Texas A&M University. Louie Strigari (TAMU)

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

Mass modelling of dwarf spheroidals. Jorge Peñarrubia

Structure and substructure in dark matter halos

Indirect Dark Matter Detection with Dwarf Galaxies

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

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

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

Chap.6 Formation and evolution of Local Group galaxies

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

Dark Matter Halos of M31. Joe Wolf

Indirect dark matter searches with the Cherenkov Telescope Array

JINA Observations, Now and in the Near Future

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

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

The Milky Way s rotation curve out to 100 kpc and its constraint on the Galactic mass distribution

Recent Searches for Dark Matter with the Fermi-LAT

MAMPOSSt modeling of true & mock dwarf spheroidal galaxies

Instituto de Fisica Teórica, IFT-CSIC Madrid. Marco Taoso. DM and the Galactic Center GeV excess

Separating Signal from Background

Searching for WIMPs in deep radio observations of Gl Galactic dsphs

Galaxy formation and evolution. Astro 850

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

Two-halo Galactic Conformity as a Test of Assembly Bias

Constraints on dark matter annihilation cross section with the Fornax cluster

Future prospects for finding Milky Way satellites. Amit and Carl 31 March 2010

Connecting observations to simulations arxiv: Joe Wolf (UC Irvine)

A tool to test galaxy formation theories. Joe Wolf (UC Irvine)

THE MAGIC TELESCOPES. Major Atmospheric Gamma Imaging Cherenkov Telescopes

the CTA Consortium represented by Aldo Morselli

Dark Matter Dominated Objects. Louie Strigari Stanford

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

Milky Way Satellite Galaxies with DES

Spatial distribution of stars in the Milky Way

(Present and) Future Surveys for Metal-Poor Stars

The Milky Way, Hubble Law, the expansion of the Universe and Dark Matter Chapter 14 and 15 The Milky Way Galaxy and the two Magellanic Clouds.

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

Precision kinematics Demonstration on Bootes dsph. Sergey Koposov Matt Walker, Vasily Belokurov, Gerry Gilmore, Jorge Pennarubia and others

Galaxy Life Stories: Sheila Kannappan UNC Chapel Hill

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

Dark Matter in Galaxies

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

A tool to test galaxy formation arxiv: Joe Wolf (UC Irvine)

Connecting observations to simulations arxiv: Joe Wolf (UC Irvine)

Overview of Dynamical Modeling. Glenn van de Ven

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

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

The Los Cabos Lectures

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

Highlights from the Fermi Symposium

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

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

Sho IWAMOTO. 15 Sep Osaka University. Based on [ ] in collaboration with M. Abdullah, J. L. Feng, and B. Lillard (UC Irvine)

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

Connecting the small and large scales

Determination of [α/fe] and its Application to SEGUE F/G Stars. Young Sun Lee

Whither WIMP Dark Matter Search? Pijushpani Bhattacharjee AstroParticle Physics & Cosmology Division Saha Institute of Nuclear Physics Kolkata

Sep. 13, JPS meeting

Sho IWAMOTO. 7 Nov HEP phenomenology joint Cavendish DAMTP U. Cambridge

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

Halo Tidal Star Streams with DECAM. Brian Yanny Fermilab. DECam Community Workshop NOAO Tucson Aug

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

Reionization. High-Redshift Galaxy UV Luminosity Function. Axion Dark Matter. Rosemary Wyse

Chapter 14 The Milky Way Galaxy

The cosmic distance scale

Using Globular Clusters to. Study Elliptical Galaxies. The View Isn t Bad... Omega Centauri. Terry Bridges Australian Gemini Office M13

Spiral Structure. m ( Ω Ω gp ) = n κ. Closed orbits in non-inertial frames can explain the spiral pattern

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

Masses of Dwarf Satellites of the Milky Way

Galaxy classification

WEAVE Galactic Surveys

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

The Structural Properties of Milky Way Dwarf Galaxies. Ricardo Muñoz (Universidad de Chile) Collaborators:

Distinguishing Between Warm and Cold Dark Matter

Tentative observation of a gamma-ray line at the Fermi Large Area Telescope

Exploring the structure and evolu4on of the Milky Way disk

From quasars to dark energy Adventures with the clustering of luminous red galaxies

Update on the Two Smoking Gun" Fermi LAT Searches for Dark Matter- Milky Way Dwarfs and Lines

Astroparticle Anomalies

Mario Juric Institute for Advanced Study, Princeton

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

Dark Matter searches with astrophysics

The tidal stirring model and its application to the Sagittarius dwarf

Annihilation Phenomenology. Christoph Weniger. GRAPPA, University of Amsterdam

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

Dark Forces in the Sky: Signals from Z and the Dark Higgs

Testing Cosmology with Phase-Space Correlations in Systems of Satellite Galaxies. Current Studies and Future Prospects

Techniques for measuring astronomical distances generally come in two variates, absolute and relative.

Indirect Detection of Dark Matter with Gamma Rays

Introduction to SDSS -instruments, survey strategy, etc

ROSAT Roentgen Satellite. Chandra X-ray Observatory

Transcription:

Prospects on the indirect dark matter detection and a future spectroscopic survey of dwarf spheroidal galaxies Koji Ichikawa (In preparation) In collaboration with Kohei Hayashi, Masahiro Ibe, Miho N. Ishigaki, Shigeki Matsumoto and Hajime Sugai. TeVPa2015, Kashiwa, Oct. 26-30, 1 2015

Direct Detection Dark Matter Search Indirect Detection DM SM DM SM Collider Production 2

Signal Target Milky-Way Galaxy dsphs 100 kpc 10 Mpc Extra Galaxy/ Cluster 8.5 kpc Charged CRs 3

dsphs: Dwarf spheroidal galaxies = Clean & DM Rich Target 1. Neighbor galaxies: 10~100kpc 2. Large Mass to Luminosity ratio = DM rich 3. Clean (no strong gamma-ray source) arxiv:0908.2995v6 [astro-ph.co]

Current(slightly old) obs limit (ex. Wino) Collider Wino DM annihilation cross section 5

Current(slightly old) obs limit (ex. Wino) Collider Wino DM annihilation cross section 6

We Should Precisely Determine The dsph DM Halo Shape Dwarf galaxy γ-rays Observed γ-ray Flux DM Property Halo Profile (J-factor)

J-Factor DM Density profile ( r / r s s ) (1 r / r s 1 s (1 r / r ) 1 s ) (1 r / r 2 s ) 2 Cusp Cored Stellar Density Profile: ν(r) Jeans equation for stars 2 (Theory) l.o.s Fit 2 (obs) l.o.s Geringer-Sameth et al., arxiv:1408.0002 8

Astrophysical Factor DM Density profile ( r / r s s ) (1 r / r s 1 s (1 r / r ) 1 s ) (1 r / r 2 s ) 2 Cusp Cored Stellar Density Profile: ν(r) Jeans equation for stars 2 (Theory) l.o.s 2 (obs) l.o.s Fit Classical: Well-determined Ultra-faint: Not well-determined. Prior dependence Factor 1.6 ~ 2 unc. :Conservative? 9

Hidden Systematics Non Spherical? => 0.2 0.4 uncertainty Axisymmetric: Hayasi and Chiba., arxiv: 1206.3888 Foreground Contamination? N < 100: O(1) uncertainty N 1000: < 0.4 By K. Hayashi-san (Preliminary) Prior Bias?/Cut? N < 100: > O(1) uncertainty Bonnivard et al., arxiv: 1407.7822

Hidden Systematics Non Spherical? => 0.2 0.4 uncertainty Axisymmetric: Hayasi and Chiba., arxiv: 1206.3888 Foreground Contamination? N < 100: O(1) uncertainty N 1000: < 0.4 Bonnivard et al., arxiv:1506.08209 30 < NMem < 100 Prior Bias?/Cut? N < 100: > O(1) uncertainty Bonnivard et al., arxiv:1504.02048 Nmem 1000

Hidden Systematics Non Spherical? => 0.2 0.4 uncertainty Axisymmetric: Hayasi and Chiba., arxiv: 1206.3888 Foreground Contamination? N < 100: O(1) uncertainty N 1000: < 0.4 Draco Segue1 Prior Bias?/Cut? N < 100: > O(1) uncertainty Martinez et al., arxiv: 0902.4715

Hidden Systematics Non Spherical? => 0.2 0.4 uncertainty Axisymmetric: Hayasi and Chiba., arxiv: 1206.3888 Foreground Contamination? N < 100: O(1) uncertainty N 1000: < 0.4 Prior Bias?/Cut? (For Ultra faint dsphs) N < 100: > O(1) uncertainty How to Reduce Them? -> Increase #NMem!

Prime Focus Spectrograph FoV 1.3 deg (diam) with 2394 Fiber MMFS (M. G. Walker et al,. (2007)) 14

Prime Focus Spectrograph FoV 1.3 deg (diam) with 2394 Fiber MMFS (M. G. Walker et al,. (2007)) 15

#Obs Star (<V) #Obs Star (<V) by M. Ishigaki Prime Focus Spectrograph More accurate DM profile estimation More Robust constraints

#Obs Star (<V) #Obs Star (<V) by M. Ishigaki Prime Focus Spectrograph More accurate DM profile estimation More Robust constraints

Strategy 1. Mock Observable: dsph Stellar + Foreground dsph Stellar Mock Boltzmann Equation under DM profile Foreground Mock Besancon Model (Robin+ (2003)) Member Star Mock Preliminary 2. Detector Convolution: 1. fix: dv = 3.0km/s 3. Fit: by (v, r) probability density. (unbinned) Foreground Mock Preliminary Obs 18

Strategy Fit without Foreground Star 1. Mock Observable: dsph Stellar + Foreground dsph Stellar Mock Boltzmann Equation under DM profile Foreground Mock Besancon Model (Robin+ (2003)) Member Star Mock Preliminary 2. Detector Convolution: 1. fix: dv = 3.0km/s 3. Fit: by (v, r) probability density. (unbinned) Foreground Mock Preliminary Obs 19

Foreground Contamination Outer Region = FG dominant Preliminary How to reduce the FG? => Cut ~ 10 % Contamination How to include the FG effect? => Model the FG dist. 30 < NMem < 100 20 Bonnivard et al., arxiv:1506.08209

Cut Strategy ROI Cut: 1.3 deg radius for 4 pointing Color Magnitude Cut Gravity Cut velocity Cut Teff, Chemical Cut do not so efficient Current (i ~ 20.) Member 420 FG 30 (w/o vcut: 130) PFS (i < 21) Member 700 FG 80 (w/o vcut: 550) This contamination is ignored = Biases dlogj~ 0.1 Member FG Chem. -> degenerate PFS (i < 21.5) Member 900 FG 100 (w/o vcut: 650)

Fit including FG model Member Fraction Prob. Dist. Of FG Member Parameter = halo information FG Parameter Can be considered to be Gaussian after several cuts. 22

FG func Parameters Outer Region Stars (Data w/o v cut can be used) => FG func parameter inc. its errors can be determined (errors => prior) FG Dominate dsph Dominate 1.3 deg radisu (4 pointings) ROI Preliminary Large ROI =Large FG sample = Small error of ffg params

Results Current Data (inc. FG contami) dlog(j) ~ 0.25? PFS (inc. FG contami) dlog(j) < 0.15? Preliminary Sum FG Mem Optimization is on-going

Summary Indirect detection is essential for DM search. Gamma-ray observation of dsph can give robust constraints on the DM annihilation cross section. Investigation of stellar kinematics (PFS) will play a crucial role. Reduction of foreground stars is important 25

Thank You! Koji Ichikawa In collaboration with Kohei Hayashi, Masahiro Ibe, Miho N. Ishigaki, Shigeki Matsumoto and Hajime Sugai. TeVPa2015, Kashiwa, Oct. 26-30, 2015