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Dark Matter shining by Galactic gamma rays and its possible implications for the LHC From EGRET excess of diffuse Galactic gamma rays • Determination of WIMP mass • Determination of WIMP halo (= standard halo + DM ring) Confirmation: • Rotation curve • Canis Major/Monoceros stream • Gas flaring PREDICTIONS • for LHC (if SUSY) • for direct searches • for solar neutrinos Wim de Boer, Karlsruhe Ingredients to this analysis Rotation curve Astronomers Tidal streams Gas flaring Astrophysics Cosmics Gamma rays 23%DM, thermal history of WIMPs Cosmology Annihilation cross section Tidal disruption of dwarfs Gamma ray spectra Particle Physics for BG + DMA HEP2008, Chile, Jan. 8, 2008 1 What is known about Dark Matter? From CMB + SN1a + surveys • 95% of the energy of the Universe is non-baryonic 23% in the form of Cold Dark Matter • Dark Matter enhanced in Galaxies and Clusters of Galaxies but DM widely distributed in halo-> DM must consist of weakly interacting and massive particles -> WIMP’s • If it is not dark It does not matter Annihilation with <σv>=2.10-26 cm3/s, if thermal relic DM halo profile of galaxy cluster from weak lensing Wim de Boer, Karlsruhe HEP2008, Chile, Jan. 8, 2008 2 Colliding Clusters Shed Light on Dark Matter http://www.sciam.com/ August 22, 2006 Observations with bullet cluster: •Chandra X-ray telescope shows distribution of hot gas •Hubble Space Telescope and others show distribution of Dark Matter from gravitational lensing •Distributions are clearly different after collision-> •dark matter is Wim de Boer, Karlsruhe weakly interacting! HEP2008, Chile, Jan. 8, 2008 3 Do we have Dark Matter in our Galaxy? Rotationcurve Solarsystem 1/r Wim de Boer, Karlsruhe HEP2008, Chile, Jan. 8, 2008 rotation curve Milky Way 4 Simple 3-Komponent Galaxy: p+e+Wimps Interactions: p+e <->H p+p -> X p+W -> p+W W+W -> X Wim de Boer, Karlsruhe electromagnetic x-section strong x-section: 10-25 cm2 x-section:<10-43 cm2 (direct DM searches) x-section: 10-33 cm2 (Hubble expansion) HEP2008, Chile, Jan. 8, 2008 5 Expansion rate of universe determines WIMP annihilation cross section Thermal equilibrium abundance Comoving number density Actual abundance T>>M: f+f->M+M; M+M->f+f T<M: M+M->f+f T=M/22: M decoupled, stable density (wenn Annihilationrate Expansionsrate, i.e. =<v>n(xfr) H(xfr) !) WMAP -> h2=0.1130.009 -> <v>=2.10-26 cm3/s DM increases in Galaxies: 1 WIMP/coffee cup 105 <ρ>. DMA (ρ2) restarts again.. Annihilation into lighter particles, like quarks and leptons -> 0’s -> Gammas! T=M/22 x=m/T Gary Steigmann/ Jungmann et al. Wim de Boer, Karlsruhe Only assumption in this analysis: WIMP = THERMAL RELIC! HEP2008, Chile, Jan. 8, 2008 6 Example of DM annihilation (SUSY) f ~ f f f W A f f Z f ≈37 gammas Z 0 W Z Dominant + A b bbar quark pair Sum of diagrams should yield <σv>=2.10-26 cm3/s to get correct relic density Wim de Boer, Karlsruhe Quark fragmentation known! Hence spectra of positrons, gammas and antiprotons known! Relative amount of ,p,e+ known as well. HEP2008, Chile, Jan. 8, 2008 7 Conclusion sofar IF DM particles are thermal relics from early universe they can annihilate with cross section as large as <v>=2.10-26 cm3/s which implies an enormous rate of gamma rays from π0 decays (produced in quark fragmentation) (Galaxy=1040 higher rate than any accelerator) Expect significant fraction of energetic Galactic gamma rays to come from DMA in this case. Remaining ones from pCR+pGAS-> π0+X , π0->2γ (+some IC+brems) This means: Galactic gamma rays have 2 components with a shape KNOWN from the 2 BEST studied reactions in accelerators: background known from fixed target exp. DMA known from e+e- annihilation (LEP) Wim de Boer, Karlsruhe HEP2008, Chile, Jan. 8, 2008 8 Basic principle for indirect dark matter searches From rotation curve: R1 Sun R bulge disc disc Sun Forces: mv2/r=GmM/r2 or M/r=const.for v=cons. and (M/r)/r2 1/r2 for flat rotation curve Expect highest DM density IN CENTRE OF GALAXY Divergent for r=0? NFW profile1/r Isotherm profile const. IF FLUX AND SHAPE MEASURED IN ONE DIRECTION, THEN FLUX AND SHAPE FIXED IN ALL (=180) SKY DIRECTIONS!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!! THIS IS AN INCREDIBLE CONSTRAINT, LIKE SAYING I VERIFY THE EXCESS AND WIMP MASS WITH 180 INDEPENDENT MEAS. Wim de Boer, Karlsruhe HEP2008, Chile, Jan. 8, 2008 9 EGRET on CGRO (Compton Gamma Ray Observ.) Data publicly available from NASA archive Instrumental parameters: Energy range: 0.02-30 GeV Energy resolution: ~20% Effective area: 1500 cm2 Angular resol.: <0.50 Data taking: 1991-1994 Main results: Catalogue of point sources Excess in diffuse gamma rays Wim de Boer, Karlsruhe HEP2008, Chile, Jan. 8, 2008 10 Two results from EGRET paper Called “Cosmic enhancement Factor” Excess Enhancement in ringlike structure at 13-16 kpc 1 Wim de Boer, Karlsruhe 10 Eγ GeV HEP2008, Chile, Jan. 8, 2008 11 Background + signal describe EGRET data! Background + DMA signal describe EGRET data! 50 GeV PS IM 0 Blue: background uncertainty Wim de Boer, Karlsruhe IC HEP2008, Chile, Jan. 8, 2008 IC s. em Br s. em Br IC W IM 0 PS W 70 Blue: WIMP mass uncertainty 12 Analysis of EGRET Data in 6 sky directions A: inner Galaxy B: outer disc C: outer Galaxy Total 2 for all regions :28/36 Prob.= 0.8 Excess above background > 10σ. E: intermediate lat. D: low latitude A: inner Galaxy (l=±300, |b|<50) B: Galactic plane avoiding A C: Outer Galaxy Wim de Boer, Karlsruhe F: galactic poles D: low latitude (10-200) E: intermediate lat. (20-600) F: Galactic poles (60-900) HEP2008, Chile, Jan. 8, 2008 13 Fits for 180 instead of 6 regions 180 regions: 80 in longitude 45 bins 4 bins in latitude 00<|b|<50 50<|b|<100 100<|b|<200 200<|b|<900 4x45=180 bins >1400 data points. Reduced 2≈1 with 7% errors BUT NEEDED IN ADDITION to 1/r2 profile, substructure in the form of 2 doughnut-like rings in the Galactic disc! ONE RING COINCIDES WITH ORBIT FROM CANIS MAJOR DWARF GALAXY which looses mass along orbit by tidal forces OTHER RING coincides with H2 ring Wim de Boer, Karlsruhe HEP2008, Chile, Jan. 8, 2008 14 Dark Matter distribution Expected Profile Observed Profile 2M/r=cons. vxy and (M/r)/r2 1/r2 for const. xzrotation curve Divergent for r=0? NFW1/r Isotherm const. xy xz Halo profile Wim de Boer, Karlsruhe Rotation Curve 2002,Newberg et al. Ibata et disk al, Crane et al. Yanny et al. bulge Inner Ring Outer Ring 1/r2 profile and rings determined fromto inde-pendent directions Normalize solar velocity of 220 km/s HEP2008, Chile, Jan. 8, 2008 15 Halo density on scale of 300 kpc Sideview Topview Cored isothermal profile with scale 4 kpc Total mass: O(1012) solar masses Wim de Boer, Karlsruhe HEP2008, Chile, Jan. 8, 2008 16 Halo density on scale of 30 kpc Sideview Topview Enhancement of inner (outer) ring over 1/r2 profile 6 (8). Mass in rings 0.3 (3)% of total DM Wim de Boer, Karlsruhe HEP2008, Chile, Jan. 8, 2008 17 How does DM substructure form from tidal disruption of dwarf galaxies? Wim de Boer, Karlsruhe HEP2008, Chile, Jan. 8, 2008 18 The Milky Way and its satellite galaxies Canis Major Tidal force ΔFG 1/r3 Wim de Boer, Karlsruhe HEP2008, Chile, Jan. 8, 2008 19 Tidal streams of dark matter from CM and Sgt CM Sun Sgt From David Law, Caltech Wim de Boer, Karlsruhe HEP2008, Chile, Jan. 8, 2008 20 Canis Major Dwarf orbits from N-body simulations to fit visible ring of stars at 13 and 18 kpc Movie from Nicolas Martin, Rodrigo Ibata http://astro.u-strasbg.fr/images_ri/canm-e.html Canis Major leaves at 13 kpc tidal stream of gas(106 M☉ from 21 cm line), stars (108 M☉ ,visible), Wim dark de Boer, matter Karlsruhe (1010 HEP2008, M☉, EGRET) Chile, Jan. 8, 2008 21 N-body simulation from Canis-Major dwarf galaxy Observed stars R=13 kpc,φ=-200,ε=0.8 Canis Major (b=-150) prograde Wim de Boer, Karlsruhe HEP2008, Chile, Jan. 8, 2008 retrograde 22 Gas flaring in the Milky Way P M W Kalberla, L Dedes, J Kerp and U Haud, http://arxiv.org/abs/0704.3925 no ring with ring Gas flaring needs EGRET ring with mass of 2.1010M☉! Wim de Boer, Karlsruhe HEP2008, Chile, Jan. 8, 2008 23 Inner Ring coincides with ring of dust and H2 -> gravitational potential well! H2 Enhancement of inner (outer) ring over 1/r2 profile 6 (8). Mass in rings 0.3 (3)% of total DM Wim de Boer, Karlsruhe 4 kpc coincides with ring of neutral hydrogen molecules! H+H->H2 in presence of dust-> grav. potential well at 4-5 kpc. HEP2008, Chile, Jan. 8, 2008 24 Objections against DMA interpretation Rotation curves in outer galaxy measured with different method than inner rotation curve. Can you combine? Also it depends on R0. Answer: first points of outer RC have same negative slope as inner RC so no problem with method. Change of slope seen for every R0. Sofue &Honma v Inner rotation curve R0=8.3 kpc R0=7.0 Outer RC Black hole at centre: R0=8.00.4 kpc R/R0 Wim de Boer, Karlsruhe HEP2008, Chile, Jan. 8, 2008 25 Do antiproton data exclude interpretation of EGRET data? Bergstrom et al. astro-ph/0603632, Abstract: we investigate the viability of the model using the DarkSUSY package to compute the gamma-ray and antiproton fluxes. We are able to show that their (=WdB et al) model is excluded by a wide margin from the measured flux of antiprotons. Problem with DarkSUSY (DS): 1) Flux of antiprotons/gamma in DarkSUSY: O(1) from DMA. However, O(10-2) from LEP data Reason: DS has diffusion box with isotropic diffusion -> DMA fills up box with high density of antiprotons 2) Priors of DARKSUSY.(and other propagation models as well): a) static galactic magnetic fields are negligible b) gas is smoothly distributed c) propagation in halo and disk are the same ALL priors likely wrong and can change predictions for DM searches by ORDER OF MAGNITUDE (and still ok with all observations!) Wim de Boer, Karlsruhe HEP2008, Chile, Jan. 8, 2008 26 Another propagation model including static magnetic fields and gas clouds and anisotropic diffusion it is shown that Galactic cosmic rays can be effectively confined through magnetic reflection by molecular clouds, Chandran, 1999 Galactic magnetic field (A0) Fast propagation along regular field lines will reduce antiproton flux from DMA, while grammage and lifetime are determined by trapping in magnetic fields Wim de Boer, Karlsruhe HEP2008, Chile, Jan. 8, 2008 27 Escape time of cosmic rays and grammage (distance x density) B/C determines grammage 10Be/9Be B/C=secondary/prim.determines grammage (smaller than disc!) In GALPROP: by large halo In CHANDRAN: by reflecting molecular clouds Wim de Boer, Karlsruhe determines escape time 10Be (t1/2 = 1.51 Myr) is cosmic clock: lifetime of cosmics 107 yrs. In GALPROP: by large halo In CHANDRAN: by long trapping. HEP2008, Chile, Jan. 8, 2008 28 Preliminary results from GALPROP with isotropic and anisotropic propagation CHANDRAN model GALPROP model Summary: with fast propagation perp. to disc (e.g. by convection, fast diffusion or static magnetic fields) one reduces contribution of charged particles from DMA by large factor and can be consistent with B/C and 10Be/9Be Wim de Boer, Karlsruhe HEP2008, Chile, Jan. 8, 2008 29 What about Supersymmetry? Simplest model: mSUGRA with 5 parameters: m0, m1/2, tan β, A0, sign µ Wim de Boer, Karlsruhe HEP2008, Chile, Jan. 8, 2008 30 EGRET excess interpreted as DM consistent with WMAP, Supergravity and electroweak constraints Stau coannihilation Stau LSP Charginos, neutralinos and gluinos light Too large boostfactor for EGRET data WMAP h<114 Bulk Wim de Boer, Karlsruhe EGRET LSP largely Bino DM may be supersymmetric partner of CMB HEP2008, Chile, Jan. 8, 2008 31 mSUGRA cross sections Main production channels: MET+ Njets+ Nleptons Contributions of different production channels normalized to the total SUSY cross section tot [pb] tan=50 A0=0 Total mSUGRA cross section(LO) Wim de Boer, Karlsruhe KNLO =1.3-1.7 HEP2008, Chile, Jan. 8, 2008 32 mSUGRA topologies Different event topology in different regions according to masses and couplings.. mSUGRA averaged observables in m0-m1/2 plane <Njets> ET>30 GeV <MET> Heff= MET+ET jets +ETleptons <N>muons PT>10 GeV/c <PT> highest muon Wim de Boer, Karlsruhe CMS FAMOS <ET > highest jet tan=50 A0=0 HEP2008, Chile, Jan. 8, 2008 33 Detector performance Main trigger streams for SUSY L1 Stream LL thresholds, GeV 1 14 2 3 29 e 2e 17 Jet+MET 88+45 Jets1(1,2,3,4) 177,86,70 Inclusive trigger efficiencies in mSUGRA plane HLT with respect to L1 L1 with respect to MC ....... HLT Stream LL thresholds, GeV 1 19 2 7 29 e 2e 17 Jet+MET 180+123 Jets1(1,2,3,4) 657,247,113 ......... Wim de Boer, Karlsruhe HEP2008, Chile, Jan. 8, 2008 34 Indirect DM detection from solar neutrinos Celestial bodies collect DM in their cores by their high density. Annihilation can result in flux of HIGH energy neutrinos from sun (from b-decays or from Z-decays). EGRET SUN Neutrinos can be detected by large detectors,like Super-Kamiokande, Amanda, Ice-Cube, Baksan by the charged current interactions with nuclei,which yields muons in the detectors. Wim de Boer, Karlsruhe HEP2008, Chile, Jan. 8, 2008 35 Direct Detection of WIMPs WIMPs elastically scatter off nuclei => nuclear recoils Measure recoil energy spectrum in target 0 H,Z EGRET? 0 If SUSY particle spectrum known, elastic scattering X-section can be calculated Wim de Boer, Karlsruhe HEP2008, Chile, Jan. 8, 2008 36 Clustering of DM An artist picture of what we should see if our eyes were sensitive to 3 GeV gamma rays and we were flying with 220 km/s through the DM halo Wim de Boer, Karlsruhe HEP2008, Chile, Jan. 8, 2008 37 8 physics questions answered SIMULTANEOUSLY if WIMP = thermal relic • Astrophysicists: What is the origin of “GeV excess” of diffuse Galactic Gamma Rays? A: DM annihilation • Astronomers: Why a change of slope in the galactic rotation curve at R0 ≈ 11 kpc? A: DM substructure Why ring of stars at 13 kpc? Why ring of molecular hydrogen at 4 kpc? Why S-shape in gas flaring? • Cosmologists: How is DM annihilating?A: into quark pairs How is Cold Dark Matter distributed?A: standard profile + substructure • Particle physicists: Is DM annihilating as expected in Supersymmetry? A: Cross sections perfectly consistent with mSUGRA for light gauginos, heavy squarks/sleptons Wim de Boer, Karlsruhe HEP2008, Chile, Jan. 8, 2008 38 Summary >>10σ EGRET excess shows intriguing hint that: WIMP is thermal relic with expected annihilation into quark pairs DM becomes visible by gamma rays from fragmentation (30-40 gamma rays of few GeV pro annihilation from π0 decays) Results rather model independent, since only KNOWN spectral shapes of signal and background used, NO model dependent calculations of abs.fluxes. Different shapes or unknown experimental problems may change the gamma ray flux and/or WIMP mass, BUT NOT the distribution in the sky. SPATIAL DISTRIBUTION of annihilation signal is signature for DMA which clearly shows that EGRET excess is tracer of DM by fact that one can construct rotation curve and tidal streams from gamma rays. DM interpretation strongly supported independently by gas flaring DM interpretation perfectly consistent with Supersymmetry Wim de Boer, Karlsruhe HEP2008, Chile, Jan. 8, 2008 39