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The matter particles
The ‘Standard Model’
The fundamental interactions
Gravitation electromagnetism weak nuclear force strong nuclear force
= Cosmic DNA
Some particles have mass, some do not
+1 0 -1
W + Z 0 W -
Mass 80.419 91.188 80.419
0photon
Mass 0
Where do the masses come from?
Newton:Weight proportional to Mass
Einstein:Energy related to Mass
Neither explained origin of Mass
Are masses due to Higgs boson? (yet another particle)
Noise Sources in LIGOGround motion couplesinto motion of mirrors
Counting statistics ofphotons at photodiode
Thermal excitations ofmirror suspensions
10-24
10-23
10-22
10-21
10-20
10-19
10-18
1 10 100 1000 104
h (
Hz-1
/2)
Virgo
LIGO
Resonantantennas
Hz
GEO
Core Collapse@ 10 Mpc
BH-BH MergerOscillations@ 100 Mpc
Pulsars hmax – 1 yr integration
BH-BH Inspiral,z = 0.4
BH-BH Inspiral, 100 Mpc
QNM from BH Collisions, 1000 - 100 Msun, z=1
NS, =10-6 , 10 kpc
QNM from BH Collisions, 100 - 10 Msun, 150 Mpc
NS-NS Inspiral, 300 Mpc
NS-NS MergerOscillations@ 100 Mpc
Credit: P.Rapagnani
Design sensitivity
Measured sensitivity
C7 NS/NS maximum distance ~ 1.5 Mpc
(7 W)(7 W)(7 W)(7 W)(0.7 W)(0.7 W)(0.7 W)
Design NS/NS maximum distance ~ 30 Mpc
WMAP satellite
At t = 400 000 yrs, the Universe becomes transparent: photons no longer interact with
matterBIG BANG
Cosmological background T = 3 K = - 270 °C
Looking back to the primordial Universe
When do graviton decouple?
Interaction rate ~ GN2 T5 ~ ----T5
MPl4
Expansion rate H ~ ----
---- ~ ----
T2
T3
MPl
MPl3
H
Gravitons decouple at the Planck era : fossile radiation
(radiation dominated era)
Update Scores LCDM TeVeS-
MOND• Solar System ? ?
• Tides/vertical force
• Rot. curves HSB/LSB
• Lensing by Ellip/Clusters
• Hubble Expansion/CMB ????
Stay Tuned!
OG 2.7: New ExperimentsCherenkov TelescopesCherenkov Telescopes
4. HESS-II [Vincent]
• New 28m telescope.• 2048 pixel camera.• Lower energy 40-50
GeV.
5. MAGIC-II [Teshima]
• New 17m telescope.• Possible high-QE
camera.• 2007 schedule.
MAGIC-IMAGIC-I MAGIC-IIMAGIC-II
85m
Future ConceptsLarge Cherenkov Tel. Arrays
HE-ASTRO: 217 Telescopes (ø10m), 80m separation.1.1 km2 collection area & 15o FOV !
Fie
ld o
f vi
ew [
π s
r] Field
of view
[deg
]
Collecting Area [km2]
Also, detailed work in Europe and Japan. Cherenkov Telescope Array (CTA)concept well underway.
How to go deeper
• A future mission should:– Achieve BLIP– Observe longer (~2)
• ~2 for satellites• John will discuss ground-
based
– Use many more pixels
• To go much deeper, we must use arrays.
The South Pole
NSF NSFNSF
NSF
Natural WIMP candidate:SUSY LSP neutralino
Stable if SUSY exists and R-parity is conserved
• Direct detection:– WIMP scattering off nuclei
˜ χ 10 =N11
˜ B +N12˜ W 3 +N13
˜ H 10 +N14
˜ H 20
Zg = N11
2+ N12
2gaugino fraction:
PMTsPMTs
PEEK SupportsPEEK Supports
CathodeCathode
GridsGrids
Waveshifter/ReflectorWaveshifter/Reflector
Moore’s sensitivity law ?
• Rapid evolution of sensitivity of discriminating experiments(CDMS, EDELWEISS, CRESST, WARP, XENON…)
• But goals are still ≈3 orders of magnitude beyond present best performances
(After Gaitskell)
Full Macho Halo:
LMC
0.45 10-6
SMC
0.65 10-6
Self lensing:
LMC-LMC
0.005 - 0.05 10-6
SMC-SMC
0.04 10-6
Lensing LMC-Galactic stars:
LMC-gal
0.01 10-6
Lensing Galactic-Galactic stars:
gal-gal
2.0 10-6
Events rate comparison :
(MACHO 0.12 10-6)
_3% at 10-2 M
Final EROS combined limit (1990-2003)
_7% at 0.4 M
_10% at 1 M
LMC data set / No event
LMC + SMC data set with 1 SMC halo candidate
Domain excluded from all EROS data
ZOOMZOOM