Transcript Folie 1

The dark connection between Canis Major, Monoceros Stream, gas flaring, the rotation curve and the EGRET excess From EGRET excess of diffuse Galactic gamma rays

Determination of WIMP massDetermination of WIMP halo

(= standard halo + DM ring) Ingredients to this analysis Astronomers Rotation curve Tidal streams Gas flaring Confirmation:

Rotation curve

Canis Major/Monoceros streamGas flaring

PREDICTIONS

for LHC (if SUSY)for direct searchesfor solar neutrinos

Astrophysics Cosmics Gamma rays Cosmology 23%DM, thermal history of WIMPs Annihilation cross section Tidal disruption of dwarfs Particle Physics Gamma ray spectra for BG + DMA Wim de Boer, Karlsruhe DARK2007, Sydney, September 24, 2007 1

What is known about Dark Matter?

From CMB + SN1a + surveys

95% non-baryonic 23% of the energy of the Universe is 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 if thermal relic cm 3 /s , Wim de Boer, Karlsruhe DARK2007, Sydney, September 24, 2007 DM halo profile of galaxy cluster from weak lensing 2

Expansion rate of universe determines WIMP annihilation cross section Thermal equilibrium abundance Actual abundance T>>M: f+f->M+M; M+M->f+f Tf+f T=M/22: M decoupled , stable density ( wenn Annihilationrate

rate, i.e.

=<

v>n

(x fr Expansions )

H(x fr ) !) WMAP ->

h 2 =0.113

0.009 -> <

v>=2.10

-26 cm 3 /s DM increases in Galaxies:

1 WIMP/coffee cup

10 5 DMA (

ρ 2 ) restarts again..

<ρ>.

T=M/22 Gary Steigmann ( Wim de Boer, Karlsruhe x=m/T Annihilation into lighter particles, like quarks and leptons ->

0 ’s -> Gammas!

Only assumption in this analysis: WIMP = THERMAL RELIC!

DARK2007, Sydney, September 24, 2007 3

Conclusion sofar

IF DM particles are thermal relics from early universe they can annihilate with cross section as large as from π 0 <

(Galaxy=10 v>=2.10

40 -26 cm 3 /s which implies an enormous rate of gamma rays decays (produced in quark fragmentation) higher rate than any accelerator) Expect significant fraction of energetic Galactic gamma rays to come from DMA in this case.

Remaining ones from p CR +p GAS -> π 0 +X , π 0 ->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 DARK2007, Sydney, September 24, 2007 4

 

Example of DM annihilation (SUSY)

f

f

f

A f

Z f f

   

W W

  

0 Z Z

≈37 gammas

Dominant

+

 

A <σv>=2.10

Sum of diagrams should yield -26 b bbar quark pair cm 3 /s to get correct relic density Wim de Boer, Karlsruhe Quark fragmentation known!

Hence spectra of positrons, gammas and antiprotons known!

Relative amount of as well.

DARK2007, Sydney, September 24, 2007

,p,e+ known 5

Basic principle for indirect dark matter searches From rotation curve: R 1 Forces: mv and

 

(M/r)/r 1/r 2 2 2 /r=GmM/r for flat rotation curve 2 or M/r=const.for v=cons.

Sun Sun R bulge disc disc Expect highest DM density IN CENTRE OF GALAXY Divergent for r=0?

NFW profile

1/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 DARK2007, Sydney, September 24, 2007 6

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 cm 2 Angular resol.: <0.5

0 Data taking: 1991-1994 Main results: Catalogue of point sources Excess in diffuse gamma rays Wim de Boer, Karlsruhe DARK2007, Sydney, September 24, 2007 7

Two results from EGRET paper

Excess Called “Cosmic enhancement Factor” Wim de Boer, Karlsruhe 1 10 Enhancement in ringlike structure at 13-16 kpc Eγ GeV DARK2007, Sydney, September 24, 2007 8

Background + signal describe EGRET data!

Background + DMA signal describe EGRET data!

IC 0

WIMPS .

Blue: background uncertainty 50 GeV IC

0 WIMPS IC 70 Brems .

Blue: WIMP mass uncertainty Wim de Boer, Karlsruhe DARK2007, Sydney, September 24, 2007 9

What about background shape?

No SM No SM Quarks from WIMPS Electrons Protons Quarks in protons Background from nuclear interactions (mainly p+p-> π inverse Compton scattering (e-+

0 + X ->

-> e- +

) + X Bremsstrahlung (e- + N -> e- +

+ N) Shape of background KNOWN if Cosmic Ray spectra of p and e- known Wim de Boer, Karlsruhe DARK2007, Sydney, September 24, 2007 10

Energy loss times of electrons and nuclei

t -1 = 1/E dE/dt t

univ Protons diffuse much faster than energy loss time, so expect SAME shape everywhere. Indeed observed: outer Galaxy can be fitted with same shape as inner Galaxy. Wim de Boer, Karlsruhe DARK2007, Sydney, September 24, 2007 11

Analysis of EGRET Data in 6 sky directions A: inner Galaxy C: outer Galaxy B: outer disc Total

2 for all regions :28/36

Prob.= 0.8 Excess above background > 10σ.

D: low latitude E: intermediate lat.

F: galactic poles A: inner Galaxy (l= ± 30 0 , |b|<5 0 ) B: Galactic plane avoiding A C: Outer Galaxy Wim de Boer, Karlsruhe D: low latitude (10-20 0) E: intermediate lat. (20-60 F: Galactic poles (60-90 DARK2007, Sydney, September 24, 2007 0 ) 0 ) 12

Fits for 180 instead of 6 regions

180 regions: 8 0 in longitude

4 bins in latitude 45 bins

0 0 <|b|<5 0 5 0 <|b|<10 0 10 0 <|b|<20 0 20 0 <|b|<90 0

4x45=180 bins

>1400 data points. Reduced

2 ≈1 with 7% errors BUT NEEDED IN ADDITION to 1/r 2 profile, substructure in the form of 2 doughnut-like rings in the Galactic disc!

Wim de Boer, Karlsruhe ONE RING COINCIDES WITH ORBIT FROM CANIS MAJOR DWARF GALAXY which loses mass along orbit by tidal forces OTHER RING coincides with H 2 ring DARK2007, Sydney, September 24, 2007 13

Dark Matter distribution

Expected Profile Observed Profile

z

xy xz v 2

M/r=cons.

and



(M/r)/r 2



1/r 2 for const.

xz rotation curve Divergent for r=0?

NFW

1/r Isotherm const.

Halo profile Rotation Curve

x y Crane et al. Yanny et al.

disk bulge Inner Ring 1/r 2 profile and rings pendent directions Outer Ring determined from inde Normalize to solar velocity of 220 km/s Wim de Boer, Karlsruhe DARK2007, Sydney, September 24, 2007 14

How does DM substructure form from tidal disruption of dwarf galaxies?

Wim de Boer, Karlsruhe DARK2007, Sydney, September 24, 2007 15

The local group of galaxies

Wim de Boer, Karlsruhe DARK2007, Sydney, September 24, 2007 16

The Milky Way and its 13 satellite galaxies Canis Major Tidal force

ΔF G

1/r 3 Wim de Boer, Karlsruhe DARK2007, Sydney, September 24, 2007 17

Tidal streams of dark matter from CM and Sgt CM Sun Sgt From David Law, Caltech Wim de Boer, Karlsruhe DARK2007, Sydney, September 24, 2007 18

Artistic view of Canis Major Dwarf just below Galactic disc Wim de Boer, Karlsruhe DARK2007, Sydney, September 24, 2007 19

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(10 6 M

from 21 cm line), stars (10 8 M

,visible), dark matter (10 10 M

, EGRET) 20

N-body simulation from Canis-Major dwarf galaxy R=13 kpc,φ=-20 0 ,ε=0.8

prograde Canis Major (b=-15 0 ) retrograde Wim de Boer, Karlsruhe DARK2007, Sydney, September 24, 2007 21

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 2.10

10 M

!

Wim de Boer, Karlsruhe DARK2007, Sydney, September 24, 2007 22

Inner Ring coincides with ring of dust and H 2 gravitational potential well!

-> H 2 Enhancement of inner (outer) ring over 1/r 2 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->H 2 in presence of dust-> grav. potential well at 4-5 kpc.

DARK2007, Sydney, September 24, 2007 23

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. margin from the measured flux of antiprotons. We are able to show that their (=WdB et al) model is excluded by a wide 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 DARK2007, Sydney, September 24, 2007 24

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,

Integral excess of positrons in bulge because positrons are trapped in magnetic mirrors between gas clouds?

Wim de Boer, Karlsruhe DARK2007, Sydney, September 24, 2007 25

The van Allen belts are trapped cosmic rays in magnetic mirrors of earth

Radiation in inner belt: 25 Sv/yr inside space ship Lethal dose for human: 3 Sv/h Satellites switch of electronics, when entering dense radiation areas.

Wim de Boer, Karlsruhe DARK2007, Sydney, September 24, 2007 26

Escape time of cosmic rays and grammage (distance x density) B/C determines grammage 10 Be/ 9 Be determines escape time B/C=secondary/prim.determines grammage (smaller than disc!) In GALPROP: by large halo In CHANDRAN: by reflecting molecular clouds Wim de Boer, Karlsruhe 10 Be (t 1/2 = 1.51 Myr) In GALPROP: In CHANDRAN: DARK2007, Sydney, September 24, 2007 is cosmic clock: lifetime of cosmics 10 by large halo 7 yrs. by long trapping . 27

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 10 Be/ 9 Be Wim de Boer, Karlsruhe DARK2007, Sydney, September 24, 2007 28

Comparing radioactive isotopes with positron distribution (Knödlseder et al.) 1809 keV ( 26 Al) 511 keV Problem: expect most low energy positrons to originate from radioactive nuclei with β+ decay.

But these are distributed in bulge AND disk.

Positrons mostly in bulge. Why???

Unknown positron source only in bulge?? Light DM?

Or simply: relativistic positrons escape in disk and annihilate in bulge?

Wim de Boer, Karlsruhe DARK2007, Sydney, September 24, 2007 29

astro-ph/0509298 NO annihilation in molecular clouds (MC), although 75% of mass in MC. Why?

Either volume of MC too small OR MC are magnetic mirrors as postulated by Chandran!

Wim de Boer, Karlsruhe DARK2007, Sydney, September 24, 2007 30

What about Supersymmetry?

Assume mSUGRA

5 parameters: m 0 , m 1/2 , tanb, A, sign μ Wim de Boer, Karlsruhe DARK2007, Sydney, September 24, 2007 31

EGRET excess interpreted as DM consistent with WMAP, Supergravity and electroweak constraints

Stau coannihilation

Stau LSP Too large boostfactor for EGRET data Charginos, neutralinos and gluinos light h<114 Wim de Boer, Karlsruhe Bulk

WMAP EGRET

LSP largely Bino

DM may be supersymmetric partner of CMB DARK2007, Sydney, September 24, 2007 32

Gauge unification perfect with SUSY spectrum from EGRET SM SUSY NO FREE parameter With SUSY spectrum from EGRET + WMAP data and start values of couplings from final LEP data perfect gauge coupling unification!

Also b->s

and g-2 in agreement with SUSY spectrum from EGRET Wim de Boer, Karlsruhe DARK2007, Sydney, September 24, 2007 33

Indirect DM detection from solar neutrinos

SUN 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).

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 DARK2007, Sydney, September 24, 2007 34

Direct Detection of WIMPs WIMPs elastically scatter off nuclei => nuclear recoils Measure recoil energy spectrum in target

0 H,Z

0 If SUSY particle spectrum known, elastic scattering X-section can be calculated Wim de Boer, Karlsruhe DARK2007, Sydney, September 24, 2007 EGRET?

35

Galaxy formation starting from quantum fluctuations

Clustering enhances flux from DMA by factor 20-200 (Dokuchaev et al.) Wim de Boer, Karlsruhe 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 DARK2007, Sydney, September 24, 2007 37

8 physics questions answered SIMULTANEOUSLY if WIMP = thermal relic

Astrophysicists:

Galactic Gamma Rays?

Astronomers:

at R 0 ≈ 11 kpc?

Cosmologists:Particle physicists:

A: DM annihilation Why a change of slope in the galactic rotation curve A: DM substructure Why ring of stars at 13 kpc?

Why ring of molecular hydrogen at 4 kpc? Why S-shape in gas flaring? How is DM annihilating?

How is Cold Dark Matter distributed?

A: into quark pairs A: standard profile + substructure Is DM annihilating as expected in Supersymmetry?

A: Cross sections perfectly consistent with mSUGRA for light gauginos, heavy squarks/sleptons Wim de Boer, Karlsruhe DARK2007, Sydney, September 24, 2007 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 π 0 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 DARK2007, Sydney, September 24, 2007 39