Das AMS-Experiment - Auf der Suche nach Dunkler Materie im Weltraum. Science on the ISS AMS. Stefan Schael, RWTH Aachen S.C.C. Ting

Das AMS-Experiment Auf der Suche Science nach Dunkler Materie on the ISS im Weltraum AMS January 5, 2007 Stefan Schael, RWTH Aachen S.C.C. Ting ...
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Das AMS-Experiment Auf der Suche Science nach Dunkler Materie on the ISS im Weltraum

AMS

January 5, 2007

Stefan Schael, RWTH Aachen

S.C.C. Ting

D. Clowe et al., astro-ph/0608407

Density fluctuations

The standard cosmological model

CMB + SDSS + 2dFGRS: !b h 2 = 0.0227 ± 0.008

(M. Tegmark, MIT)

!c h 2 = 0.120 ± 0.005 ! " = 0.70 ± 0.03 ! m = 0.30 ± 0.03 H 0 = 69.6 ± 2.4 h = H 0 / 100 km s #1 Mpc #1 (astro-ph-0507503)

The standard cosmological model In this model the Universe is: •

spatially flat, homogeneous and isotropic on large scales



composed of • radiation, ordinary matter (electrons, protons, neutrons and neutrinos)



→4.4%



cold dark matter, which we know nothing about.

→23%



dark energy. which we know less than nothing about.

→73%

Galaxies and large scale structures grew gravitationally from tiny, nearly scale-invariant adiabatic Gaussian fluctuations which we know nothing about.

Dark Matter Searches AMS

e+, p, D, … Charged particles

γ,ν Antares, Km3, … Amanda, Icecube

GLAST CANGAROO, HESS, MAGIC, Veritas, …

Colliders

FNAL, LHC, ILC

Direct detection Ge

WIMP

Dama, CDMS, GENIUS, CRESST, Edelweiss, …

Ge, Si

~20% energy Ionization

Liquid Xe

Heat

Al2O3, LiF ~100% energy

cryogenic detectors

Light

NaI, Xe

~few % energy

CaWo4, BGO

Physics of AMS γ,ν Hubble, Chandra, GLAST, JWST, JDEM Discoveries: (1) Pulsar, (2) Microwave, (3) Binary Pulsars, (4) X Ray sources, solar neutrinos (5) Dark Matter, Dark Energy

…… WHIPPLE, HESS, VERITAS,



The highest energy particles are in Cosmic Rays AMS will perform accurate measurements of energetic cosmic rays (0.1 GeV to 2 TeV)

HiRes

AUGER

SUPER K

Physics of Charged Cosmic Rays

π

µ

e

1 9 4 7 : Disco very o f p io ns C. Po w ell 1 9 1 2 : Disco very o f Co sm ic Rays V. Hess

1 9 3 2 : Disco very o f p o sitro n C. D. And erso n

Discoveries of 1 9 3 6 : Muon ( μ) 1 9 3 8 : 1 0 1 5 eV CR 1 9 4 9 : Kaon ( K) 1 9 4 9 : Lam b d a ( Λ) 1 9 5 2 : Xi ( Ξ) 1 9 5 3 : Sig m a ( Σ) AMS is the first precision magnetic spectrometer in Space



Primary particles by supernovae explosions, …



Secondary particles from nuclear interactions.



Diffusion parameters determined from sec./prim. ratios, e.g. B/C ratio



Halo size determined from radioactive isotopes e.g. 10Be/9Be ratio (τ(10Be)=1.6 106 yr)

Galactic Diffuse γ−rays

Inner Galaxy : Significance ≥ 5 σ

EGRET All-Sky Map ApJ, 613, 962 (2004)

#4/14

SUSY Dark Matter candidate: Neutralino • •

MSSM and R-parity => Stable DM candidate: the LSP Preferred candidate: The Neutralino

! i = N i,1 B! + N i,2 W!3 + N i,3 H! 10 + N i,4 H! 20

Higgs (h, H, A, H±) m1/ 2 = 350 GeV " m ! = 144 GeV

squarks & sleptonen gaugino

MSSM Parameter: m 0 , m1/2 , tan ! , sign( µ ), A0



From astrophysics and cosmology we get: !CDM h 2 = 0.120 ± 0.005

BR(B ! X s" )exp = (3.39

+0.30 ) $10 #4 #0.27

BR(B ! X s" )SM = (3.70 ± 0.30) $10 #4

tan ! = 50, µ > 0, A0 = 0

m1/ 2 = 350 GeV " m ! = 144 GeV

DM Annihilation in Supersymmetry χ

f χ

~

f χ

f

χ

f χ

χ

A

χ

W χ±

f χ

f Z

χ

f ≈37 gammas

Z χ0

W

χ

Z

Dominant χ + χ ⇒ A ⇒ b bbar quark pair

B-Fragmentation known! Hence Spectra of Positrons, Gammas and Antiprotons known!

Galaxy = Super B-Fabrik with rate 1040 x B-Factory

AMS-01: STS-91 1998 Flight Results



Energy Range: 100 MeV/n102 1-300 GeV acceptance: 0.5m2sr Choosen configuration for 60 cm height: 20 Layers each existing of: • 22 mm fibre fleece • Ø 6 mm straw tubes filled with Xe/CO2 80%/20% 12 layers in the bending plane 2 x 4 layers in the non-bending plane

Straw Module

Straw tube proportional counter modules: •Straw tubes: 72 µm multilayer aluminium kapton foil, Ø 6 mm , 0.8 ÷ 2.0 m length • Wire: tungsten anode wire, 30 µm Ø, tension ≈ 100 g • Gas mixture: Xe / CO2 (80% / 20%) • Operating HV ~ 1380 V → Gasgain of ~ 3000 • 1 Module → 16 Straws, 100 µm mechanical accuracy • 328 Modules → 5248 Straws

TRD Test Beam Results I • • •

20 layer TRD detector in the test beam at CERN in 2000 we have recorded 3 million events providing signals for protons, electrons, muons and pions at energies from 5-250 GeV Muon events have been used for an intercalibration of the individual straws to a relative accuracy of 2%.

ep+

single layer !

TRD Testbeam Results

TRD single Straw Test to select 5248 good straws

TRD Flight Hardware

AMS-02 Transition Radiation Detector

Performance of the AMS-02 Transition Radiation Detector. Published in Nucl.Instrum.Meth.A558:526-535,2006.

Anti-Protons

Test b eam 1 5 8 GeV/n

M. Battaglia et al., hep-ex/0106207

Post-LEP CMSSM Benchmarks for Supersymmetry M. Battaglia et al., hep-ph/0112013 F

E

M

M

K

H L

J

I B

D

G

A

C

Blue region allowed WMAP, etc. At benchmarks “K” & “M” Supersymmetric particles are not visible at the LHC, but are accessible to AMS.

Benchmark “M” (not accessible to LHC) AMS spectra with Mχ = 840 GeV

K

Zusammenfassung •

Wir haben indirekte Evidenz für die Existenz von Dunkler Materie auf ganz verschiedenen Längenskalen:

!CDM h 2 = 0.120 ± 0.005 !b h 2 = 0.0227 ± 0.0008 •

Wir beobachten Anomalien in den Spektren der kosmischen Höhenstrahlung, die wir mit der Annihilation von Dunkler Materie erklären könnten.



Innerhalb der nächsten 5 Jahre erwarten wir Antworten von: –

Beschleuniger Experimenten: Tevatron (2008)



Experimenten zur direkten Suche: CMDS, Edelweis, CRESST, XENON, ...



Experimenten zur indirekten Suche: • Im Weltraum: PAMELA, GLAST, AMS-02 • Neutrino-Exp.: IceCube, ANTARES • Cherenkov-Teleskope: HESS, MAGIC

J.J Beatty et al., PRL 93 (2004) 241102 PAMELA error > 30%

10 events PAMELA projection A SUSY Model (LSP of 91 GeV) (Projection)

y06K304b

#6/14

Modes of Neutralino Annihilations : tanβ=10 χ1

f

t

χ1

∼ f χ1

χ1

Z0 f

χ1

t

W+ (Z0)

∼ τ

χ1 ∼ τ

χ± (χn0) τ

χ1 W- (Z0)

γ

#7/14

Modes of Neutralino Annihilations : tanβ=53 χ1

b

A0 χ1

b 2

m f ( N1 N 3( 4) ' m * $ ) % " tan ! mW & mA #

#8/14

χ2 : e+/(e++e-) Only tanβ=10

tanβ=30

tanβ=40

χ2 : γ−rays Only n.d.f = 12

tanβ=50

tanβ=52