Dark Matter searches with astrophysics

Similar documents
Dark Matter searches with radio observations

Spectra of Cosmic Rays

Natural explanation for 130 GeV photon line within vector boson dark matter model

Cosmic ray electrons from here and there (the Galactic scale)

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

Astrophysical issues in the cosmic ray e spectra: Have we seen dark matter annihilation?

Fundamental Physics with GeV Gamma Rays

The High-Energy Interstellar Medium

The positron and antiproton fluxes in Cosmic Rays

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

Indirect dark matter detection and the Galactic Center GeV Excess

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

Fermi: Highlights of GeV Gamma-ray Astronomy

arxiv: v1 [astro-ph.he] 29 Jan 2015

GALACTIC CENTER GEV GAMMA- RAY EXCESS FROM DARK MATTER WITH GAUGED LEPTON NUMBERS. Jongkuk Kim (SKKU) Based on Physics Letters B.

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

CMB constraints on dark matter annihilation

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

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

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

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

Interstellar gamma rays. New insights from Fermi. Andy Strong. on behalf of Fermi-LAT collaboration. COSPAR Scientific Assembly, Bremen, July 2010

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

Neutrinos and DM (Galactic)

Project Paper May 13, A Selection of Dark Matter Candidates

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

Observational Prospects for Quark Nugget Dark Matter

Annihilation Phenomenology. Christoph Weniger. GRAPPA, University of Amsterdam

Astrophysical issues in indirect DM detection

Dark Matter in the Galactic Center

Instituto de Fisica Teórica, IFT-CSIC Madrid. Marco Taoso. Sommerfeld enhancement and Bound State formation. DM from aev to ZeV. Durham

Dark Matter Models. Stephen West. and. Fellow\Lecturer. RHUL and RAL

Lecture 14. Dark Matter. Part IV Indirect Detection Methods

DARK MATTER. Martti Raidal NICPB & University of Helsinki Tvärminne summer school 1

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

Indirect Dark Matter constraints with radio observations

OVERVIEW: Dark Matter

Dark Matter in the Universe

PHY326/426 Dark Matter and the Universe. Dr. Vitaly Kudryavtsev F9b, Tel.:

Anisotropy signatures of dark matter annihilation

Resolving the Extragalactic γ-ray Background

PERSPECTIVES of HIGH ENERGY NEUTRINO ASTRONOMY. Paolo Lipari Vulcano 27 may 2006

Cosmic rays and the diffuse gamma-ray emission

Understanding High Energy Neutrinos

Astroparticle Anomalies

Cosmic Positron Signature from Dark Matter in the Littlest Higgs Model with T-parity

Particle Acceleration in the Universe

Structure of Dark Matter Halos

Dark Matter Decay and Cosmic Rays

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

Indirect detection of decaying dark matter

Wino dark matter breaks the siege

Impact of substructures on predictions of dark matter annihilation signals

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

Exploring the Ends of the Rainbow: Cosmic Rays in Star-Forming Galaxies

Dark matter in split extended supersymmetry

Kaluza-Klein Dark Matter

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

Signal Model vs. Observed γ-ray Sky

The Mystery of Dark Matter

Chern-Simons portal Dark Matter

Cristiano Alpigiani Shanghai Jiao Tong University Shanghai, 18 May 2017

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

99 Years from Discovery : What is our current picture on Cosmic Rays? #6 How cosmic rays travel to Earth? Presented by Nahee Park

The Characterization of the Gamma-Ray Excess from the Central Milky Way

Constraints on Light WIMPs from Isotropic Diffuse γ-ray Emission

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

Fermi-Large Area Telescope Observations of Pulsar Wind Nebulae and their associated pulsars

Prospects for indirect dark matter detection with Fermi and IACTs

Gamma-ray Astrophysics

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

Astro2020 Science White Paper Prospects for the detection of synchrotron halos around middle-age pulsars

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

THE STATUS OF NEUTRALINO DARK MATTER

DM subhalos: The obser vational challenge

An Auger Observatory View of Centaurus A

Neutralino Dark Matter as the Source of the WMAP Haze

The Cherenkov Telescope Array (CTA)

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

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

LHC searches for dark matter.! Uli Haisch

Dark-matter bound states

Dark Matter - II. Workshop Freudenstadt shedding (Cherenkov) light on dark matter. September 30, 2015

Dark Matter Annihilation, Cosmic Rays and Big-Bang Nucleosynthesis

Signatures of clumpy dark matter in the global 21 cm background signal D.T. Cumberland, M. Lattanzi, and J.Silk arxiv:

Constraints on cosmic-ray origin from gamma-ray observations of supernova remnants

Dark Matter ASTR 2120 Sarazin. Bullet Cluster of Galaxies - Dark Matter Lab

Propagation in the Galaxy 2: electrons, positrons, antiprotons

Indirect Search for Dark Matter with AMS-02

Dynamical Dark Matter and the Positron Excess in Light of AMS

Remnants and Pulsar Wind

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

LATE DECAYING TWO-COMPONENT DARK MATTER (LD2DM) CAN EXPLAIN THE AMS-02 POSITRON EXCESS

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

Cosmological Constraint on the Minimal Universal Extra Dimension Model

Ultra- high energy cosmic rays

Gamma-ray emission at the base of the Fermi bubbles. Dmitry Malyshev, Laura Herold Erlangen Center for Astroparticle Physics

Beyond Simplified Models

Collider Searches for Dark Matter

Transcription:

Marco Taoso IPhT CEA-Saclay Dark Matter searches with astrophysics IAP 24 February 2013

The cosmological pie Non baryonic Dark Matter dominates the matter content of the Universe Motivation to search for new physics beyond the Standard Model

Weakly Interacting Massive Particles WIMPs annihilate in the early Universe and decouple from thermal bath when they are non relativistic Relic density with standard cosmology: Electroweak cross-sections are in the correct range WIMPs arises in many extensions of the Standard Model at the EW scale

Hunting WIMPs Colliders Missing energy signature at LHC Direct Detection DM scattering off detectors in underground laboratories Indirect detection Signature of DM annihilations in space

Hunting WIMPs with astrophysics WIMPs inside halos annihilate into Standard Model particles. Generically these processes lead to fluxes of photons Typically gamma-rays since WIMPs masses lie in the GeV-TeV range Antimatter antiproton, positrons, antideuterium neutrinos

Plan of the talk Searches of DM with gamma-rays Brief discussion about recent results on gamma-ray lines Implications for models of DM Radio Bounds from radio data and searches of extragalactic sources

Annihilation spectra DM annihilates into SM particle which eventually hadronize/decay and produce photons, neutrinos, anti-protons, positrons... Continuum featureless photon spectrum Difficult to distinguish from astrophysical background

Where to look for DM Dwarf galaxies Extragalactic emission Galactic center clumps Cluster of galaxies Diffuse Halo

Dwarf galaxies From Drlica-Wagner, Fermi Symposium 2012 Thermal cross-section DM dominated objects, large M/L ratios Nearby DM density distribution from stellar velocity distribution Strong bounds on DM annihilations

Spectral features Bringmann, Weniger 2012 Gamma-ray lines are induced at loop-level : O(α2) suppression Hard spectrum can arise from radiative corrections Internal Bremsstrahlung

Fermi Lines Weniger 2012 Optimized target region around the galactic center & excluding most of the disk Sliding energy window : search in a small energy range around the line. Astro bkg as a power law Line at 130 GeV with Local significance of 4.6 sigma (Global significance 3.2 sigma)

Fermi Lines Su, Finkbeiner arxiv:1206.1616 Talk by A. Albert, Fermi Symposium 2012

News from Fermi-Collaboration Results from Fermi Collaboration with reprocessed data + improved energy resolution The peak move to 135 GeV and the significance drops below 2 sigma Search for systematics effects. Look at control regions away from GC Feature detected in the Earth Limb photons Maybe also in other control regions, see Finkbeiner,Su,Weniger 2012, Whiteson 2013

Limits on gamma-rays Lines Hess collaboration 2013, arxiv:1301.1173

Implications for models DM DM DM DM

Implications for models Sensitivity of FERMI-LAT to lines around 100 GeV From dwarfs for hadronic channels & M around 100 GeV From the shape of the spectrum bounds Cohen, Lisanti,Slatyer, Wacker 2012 on the continuum Loop suppression is typically larger! Summarizing: not straightforward to accommodate such signal in DM models

Forbidden channel scenario DM Mediator DM DM has large couplings to new charged particles via a mediator annihilations kinematically forbidden today since DM has small velocities Annihilations can occur in the early Universe

Simple recipe The dark sector contains SM gauge group DM + scalar + charged fermions

1-loop annihilations More than 1 line!

1-loop annihilations Jackson, Servant, Shaughnessy, Tait, MT. 2013

Relic density

Top connection The charged particle might be the SM top quark Jackson, Servant, Shaughnessy, Tait, MT. 2010 It is the only one SM fermion with a mass in right ballpark Dark sector which couples more to large particles with heavier particles are motivated in models of composite Higgs and fermions and & Randall Sundrum extra-dimensions

Simple UV completion SM top mass mass new fermion Mixing Top quark (t) and extra fermion (T) are superposition of initial fermions Mixing angle functions of initial parameters

Electroweak Precision Tests The mixing between the top quark and the new fermion is constrained by precision measurements at colliders

Higgs Physics Like SM! EXCLUDED EWPT

1-loop diagrams

1-loop x-sections

Lines EXCLUDED EWPT Large Line signals with small continuum is possible! Jackson, Servant, Shaughnessy, Tait, MT. In preparation EXCLUDED EWPT

Summary Large line signals can arise in models where annihilations are enhanced by resonant effects and the continuum emission is forbidden/depressed These features can be captured by simple models with vector/scalar mediators & possibly with mass mixing with the SM top Gamma-ray line signals are precious probes of DM annihilations We need to single out the DM theories which can be tested

Other wavelengths Gamma-rays are primary messengers of WIMPs annihilations Can we look for DM signals at other wave-lengths? Radio Bounds from radio and searches of extragalactic sources

Secondary emissions Synchrotron Radio - Microwave IC FSR X-rays Gamma-rays Final state radiation Inverse Compton Synchrotron emission from interactions of electrons with magnetic fields

Synchrotron radiation Synchrotron emission from interactions of electrons with magnetic fields Typical values for the synchrotron peak:

Propagation of charged particles Propagation of charged cosmic-rays described by transport equation which describes energy losses, diffusion accelerations, convection diffusion energy losses distribution of sources

Local cosmic-rays Delahaye et al. 2010 Di Bernardo et al. 2012 Astrophysical sources can explain data under reasonable assumptions Sources of leptonic CRs: 1) primary electrons from sources (Supernova Remnants) 2) secondaries electrons and positrons from hadronic CRs interactions 3) extra population of electrons and positrons (likely pulsars). Propagation models tuned against data, notably B/C, radioactive isotopes, protons This leaves degeneracies among the propagation parameters Additional info should be used

Constrain CRs and B with radio Strong, Orlando, Jaffe 2011 Magnetic fields are constrained by Faraday rotation measurements of sources Radio surveys constrain the synchrotron emission from CR electrons Low/high frequency surveys probe different parts of the interstellar electron

Constrain CRs and B with radio Bringmann, Donato, Lineros 2011 Morphology and normalization of synchrotron emission (+ info on Magnetic fields) constrain the parameter of propagation models Models with small scale-height of the diffusion regions are disfavored Similar conclusions arises from analysis of the diffuse gamma-ray emission from Fermi-LAT Gamma-ray diffuse from interactions of protons with gas and IC and Brem. of electrons

Synchrotron from DM MAX MED MIN Propagation models allowed by cosmic-rays data MIN MED MAX bracket the uncertainties. However extreme modes (MIN) are disfavored from shape of diffuse radio and gamma emissions!

Synchrotron from DM Low radio frequencies particularly suitable to constrain light DM

Radio surveys from 22 MHz to 1420 MHz

Constraints on DM N.Fornengo, R.Lineros, M.Regis, M.T. 2011 Bounds are better/worst than those from gamma-rays for leptonic/hadronic channels The dependence on the scale-height and on the propagation parameters is not dramatic Bounds depend somewhat on the dark matter density profile

Constraints on DM Bounds are better/worst than those from gamma-rays for leptonic/hadronic channels The dependence on the scale-height and on the propagation parameters is not dramatic Bounds depend somewhat on the dark matter density profile

Isotropic radio background Isotropic radio background emission can be extracted from radio maps looking at high latitude and after subtraction of a galactic model. Delicate jobs!!! Used to study populations of radio sources. Can be useful to look for dark matter signals?

ARCADE-II excess Data from low frequency surveys 22 MHz 45 MHz 408 MHz 1420 MHz + ARCADE-2 3.2 GHz 90 GHz Fixen et al. 2009 Galactic emission estimated with 2 methods: plane parallel model & correlation of radio maps with CII map (tracer of galactic emission) After CMB monopole is removed data an isotropic background is detected <10 GHz Fixen et al. 2009

Number counts of sources Radio Loud AGN Star Forming Galaxies Vernstron, Scott, Wall 2012

ARCADE-II excess Isotropic extra galactic radio background inferred by ARCADE is 480 mk! Vernstron, Scott, Wall 2012 Expected contribution of radio sources Vernstron et al. 2011 Excess confirmed at other frequencies

Possible explanations? The excess calls for an undetected population of radio sources at fluxes below micro-jy Interpretations in terms of known astro- sources are challenged by multi-wavelength constraints: gamma-rays, X-rays (diffuse intragalactic emission), IR (star forming galaxies). Singal et al. 2010, Lacki 2010, Ponente 2010,...

Can DM explain these data? N.Fornengo, R.Lineros, M.Regis, M.T. 2011 Synchrotron emission in extra-galactic halos can explain the excess Only leptonic channels are viable Constraints from gamma and X rays are ok for lepto-philic and light DM DM is in principle a viable option but there isn't any striking signature of DM into the signal!!!

Options 1) The radio background estimated by ARCADE-2 collaboration is off because it is contaminated by galactic foreground. Different methods to test the robustness of this estimation 2) There is an undetected small population of faint and numerous radio sources with faint emissions at other wavelengths.

Forecast for future experiments N.Fornengo, R.Lineros, M.Regis, M.T. 2012 DM sources can dominate the number counts of sources at sub micro-jy fluxes These fluxes are at the reach of future radio telescopes: EVLA and ASKAP soon, SKA (long term project) Redshift evolution of DM sources different from that of Star Forming galaxies

Forecast for future experiments Present data on angular correlations are not relevant: too large fluxes They can becomes relevant probes for DM sources at low fluxes Caution: predictions are affected by large astro-uncertainties See N.Fornengo, R.Lineros, M.Regis, M.T. 2012for more details

Summary Gamma-ray line signals are precious probes of DM annihilations We need to single out the DM theories which can be tested DM annihilations typically produce a multi-wavelength spectrum From Radio data we can constrain the dark properties Future surveys might say something about extragalactic DM radio sources

THANKS