introduction to cosmology today results on dark energy future experiments search for dark energy

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•Introduction to cosmology •Today results on dark energy Search for dark energy

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Page 1: Introduction to cosmology Today results on dark energy Future experiments Search for dark energy

•Introduction to cosmology

•Today results on dark energy

•Future experiments

Search for dark energy

Page 2: Introduction to cosmology Today results on dark energy Future experiments Search for dark energy

Introduction to cosmology(1)

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TT

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rr

221Ω

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.1

curvaturepositiveafork

curvaturenulafork

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Univers is described by general relativity:

Geometry of Universe is fully described by its energy content:

Critical total energy density for which Universe is spatially flat

Matter relative energy density

Radiation relative energy density

Total relative energy density

Cosmological constant or vacuum relative energy density

Page 3: Introduction to cosmology Today results on dark energy Future experiments Search for dark energy

Introduction to cosmology(2)

Each cosmological fluid is characterized by a state equation:

zwwp

zwX

XX .)( 10

)1(334320

101 )1()1()1()1()( wwzwXrmk zezzzHzH

The Hubble parameter (expansion rate) reads simply:

w0=0

w1=0

w0=1/3

w1=0

w0=-1/3

w1=0

w0=?

w1=?

))(( )1

,0

,,,,(

0

log*5.2 wXmkz wF

FHDfm L

With Supernovae the Hubble parameter can be measure through the magnitude

z=redshift

Dark energyw0=-1

w1=0

Page 4: Introduction to cosmology Today results on dark energy Future experiments Search for dark energy

The last SN1a result: Vacuum density energy non zero

Page 5: Introduction to cosmology Today results on dark energy Future experiments Search for dark energy

2002: clusters

2003: WMAP

2003 :SCP+ 11 SNIa HST

1999: SCP/ High z

Today status:The concordance model

Page 6: Introduction to cosmology Today results on dark energy Future experiments Search for dark energy

SNAP

Après l’inflationl’expansion

expa

nsio

n

SNFactory (300 SNe)

CFHTLS (700 SNe)

Mesure de w a 10 % (limitation sol)

SNAP (2000 SNe) mesure w à 0.02 et w1 à 0.1

What can we expect for the future(SNLS/SNAP)

Page 7: Introduction to cosmology Today results on dark energy Future experiments Search for dark energy

data analysis physics

The SN method

Images

Spectra

+ identification.

Ia

magnitude z(redshift)

galaxy

Hubble

SN1a=Are considered as standard candle

Page 8: Introduction to cosmology Today results on dark energy Future experiments Search for dark energy

With which instrument ?

SNAP 2014: USA/French coll.

Page 9: Introduction to cosmology Today results on dark energy Future experiments Search for dark energy
Page 10: Introduction to cosmology Today results on dark energy Future experiments Search for dark energy
Page 11: Introduction to cosmology Today results on dark energy Future experiments Search for dark energy
Page 12: Introduction to cosmology Today results on dark energy Future experiments Search for dark energy
Page 13: Introduction to cosmology Today results on dark energy Future experiments Search for dark energy
Page 14: Introduction to cosmology Today results on dark energy Future experiments Search for dark energy
Page 15: Introduction to cosmology Today results on dark energy Future experiments Search for dark energy

shutter

Focal plane

Spectrograph

electronics

Page 16: Introduction to cosmology Today results on dark energy Future experiments Search for dark energy

Focal plane: Light curvespectrographe

0.61 Gigapixel

•36 CCD’s 10.5 m 3.5 x 3.5k ( 0.34 sq. deg.)

•36 HgCdTe’s 18 m l 2k x 2k ( 0.34 sq. deg.)

Page 17: Introduction to cosmology Today results on dark energy Future experiments Search for dark energy

Sky scanSky scan

Page 18: Introduction to cosmology Today results on dark energy Future experiments Search for dark energy

Spectrograph

Page 19: Introduction to cosmology Today results on dark energy Future experiments Search for dark energy

x

y

Cutting out on the

slices

x

y

Re-arrangement

dispersion

Pixelised image in 3 dimensions

-Whole light conservd-no slit to position - very stable stable-easy to calibrate=> adapted for space

SNAP original spectrograph

Page 20: Introduction to cosmology Today results on dark energy Future experiments Search for dark energy

Expected SNAP results for SN

Page 21: Introduction to cosmology Today results on dark energy Future experiments Search for dark energy

flatStat seule

68 %

Simulation cppm

Comparative results

Page 22: Introduction to cosmology Today results on dark energy Future experiments Search for dark energy

Weak Lensing by Large-Scale Structure

Distortion Matrix:

Direct measure of the distribution of Dark Matter in the universe

jij

iij zgdz

2

)(

Page 23: Introduction to cosmology Today results on dark energy Future experiments Search for dark energy

Weak Lensing + CMB

Expected results for SNAP

Page 24: Introduction to cosmology Today results on dark energy Future experiments Search for dark energy

Contrôle des systématiqueset des dégénérescences

Combiner avec d’autres méthodes•cisaillement gravitationnel (WL)•CMB

In number…

hypothèse

Page 25: Introduction to cosmology Today results on dark energy Future experiments Search for dark energy

Summary

•New questions are now opened:

Can we believe that 70% of Universe energy is unknown ?

What is the nature of dark energy ?

•Ground experiment will probably give a confirmation of the first point

•But only a space telescope will be able to gives answer about the nature of dark energy.

•Otherwise, if CMB/WL/SN do not agree, it will mean that something is wrong in our understanding of cosmology or general relativity….