WMAP CMB power spectrumsuto/myresearch/bao_kekph07.pdf · Should still apply now ... Why important...
Transcript of WMAP CMB power spectrumsuto/myresearch/bao_kekph07.pdf · Should still apply now ... Why important...
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Exploring dark energy in the universe through
baryon acoustic oscillation
KEK Annual Theory Meeting on Particle Physics Phenomenology (KEKPH07): March 3, 2007
KEK Annual Theory Meeting on Particle Physics Phenomenology (KEKPH07): March 3, 2007
Yasushi Suto Department of Physics, University of Tokyo
SDSS galaxy correlation
WMAPCMB power spectrum
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Without dark nights, one could have never imagined …
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what really dominates our world
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a planet with six Suns
no “night” except the total eclipse due to another planet every 2050 yearsPeople realized the true world for the first time through the darkness full of “stars”
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Darkness is the key to understanding our world betterBeyond the edge of our current horizon (= “darkness”, “dark night”)philosophy, astronomy, and therefore physics started from thinking in the darkShould still apply now
Another element: dark matter, dark energyAnother Earth: extrasolar planetAnother world: MultiverseAnother life: extra-terrestrial intelligence
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Dark energy in the universe
cosmic acceleration
Size
of t
he
univ
erse
time
Universal repulsion?Cosmological constant?Dark energy?Modified gravity?
13.7 Gyr
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1916: general relativity1917: Einstein’s static universeAfter 1980’s: vacuum energy density
Natural value: the Planck units
Observed value:
From cosmological constant to dark energy
μνμνμνμν π TGggRR 821
=Λ+−
⎟⎟⎠
⎞⎜⎜⎝
⎛ Λ−=− μνμνμνμν π
π gG
TGgRR8
821
Cosmological constant(geometrical quantity)
Dark energy(matter field)
12120
3935
103
g/cm102.5 ≈Λ
≡Ω⇔×≈=Λ Λ HGch
7.0≈ΩΛThe worst discrepancy in the history of physics !
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Dark energy and the equation of state of the universe
Parameterized equation of state(pressure) = w x (density)
w=0: dark matter,w=1/3: radiationw=-1: cosmological constant
Poisson eq. in GR : Δφ=4πG(ρ+3p)=4πGρ(1+3w)
w<-1/3 ⇒ repulsion forceNegative pressure: dark energyMore generally w may be time-dependent
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Why important ?New physics
major but unknown component of the universe ?Breakdown of general relativity at cosmological scales?
Astronomy is the key
1
10
100
1000
10000
1993
1994
1995
1996
1997
1998
1999
2000
2001
2002
2003
2004
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2006
Papers posted on astro-ph
Dark energy related papers
Total number
Steven Weinberg“Right now, not only for cosmology but for elementary particle theory this is the bone in the throat”Edward Witten“Would be number one on my list of things to figure out”Frank Wilczek“Maybe the most fundamentally ysteriousthing in basic science”
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cosmic accelerationgeometry of the universeevolution of structureProbes
Supernova Hubble diagramCosmic Microwave BackgroundGravitational lensingBaryon Acoustic Oscillation
Signatures of dark energy
t
R
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Standard candle: Type Ia Supernova
××
SN Iaabsolute luminosity: L
SN2001cw(z=0.93)
observed flux: F
Distance: D
FLDπ4
=
dark energy parameter can be read off from the comparison between the model and the observation
observational estimate
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Accelerating universe from SN Ia data
Rel
ativ
e ob
serv
atio
nal
flu
x of
SN
e
Dimmer (more distant)
Brighter (closer)
timepresent past
acceleration
deceleration
normalized by empty universe prediction
××
SN Legacy Survey (Astier et al. 2006)
SN Ia
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Standard ruler: baryon-photon acoustic oscillation length
Sound horizon length at recombination(=cs×0.37Myr)
rs=147 (Ωm h2 / 0.13)-0.25 (Ωb h2 / 0.024)-0.08 MpcEstimate the distance to the CMB last-scattering surface using the above as a standard ruler
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Acoustic oscillation illustrated (1)
in the early universe, the major components of the universe, i.e., dark matter, baryons, photons, neutrinos,behave as a strongly-coupled single fluid
http://cmb.as.arizona.edu/~eisenste/acousticpeak/acoustic_physics.html
Mass excess profile around a perturbation
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Acoustic oscillation illustrated (2)
neutrinos decouple earlier and start free-streaming
dark matter stays around the center due to its self-gravity
baryons and photons behave as a single fluid. The central concentration induces pressure and generates an outward acoustic spherical wave
http://cmb.as.arizona.edu/~eisenste/acousticpeak/acoustic_physics.html
Mass excess profile around a perturbation
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Acoustic oscillation illustrated (3)
http://cmb.as.arizona.edu/~eisenste/acousticpeak/acoustic_physics.html
After recombination (z=1000, t=0.37Myr) , baryons and photons decouple. photons start free-streaming while baryons keep the acoustic features
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Acoustic oscillation illustrated (4)
http://cmb.as.arizona.edu/~eisenste/acousticpeak/acoustic_physics.html
after decoupled from photons, baryons fall into the gravitational potential due to dark matter
dark matter acquires the baryon acoustic feature via their gravitational evolution
Final mass (baryons + dark matter) density profile
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Evolution of density profile around a peak
http://cmb.as.arizona.edu/~eisenste/acousticpeak/acoustic_physics.html
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CMB acoustic oscillation
NASA/WMAP Science Team
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BAO as a standard ruler
Distant measurement at different epochsPromising methodology to observationally constrain dark energy
Picture credit: Bob Nichol
Mpc)/024.0()/13.0(147 08.0225.02 hhr bms ΩΩ=
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Acoustic scales and geometry of the universe
NASA/WMAP Science Team
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Power spectrum of mass density fluctuations with baryon acoustic
oscillation effect
(A.Taruya, T. Nishimichi)
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Acoustic oscillations detected
SDSS galaxy correlation function
Eisenstein et al. (2005)
CMB photonsWMAP 3yr(Spergel et al. 2007)
z=1000
z=0.4
Mpc)/024.0()/13.0(147 08.0225.02 hhr bms ΩΩ=
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Percival et al. (2007)
WMAP3
SDSS galaxies
Ωm=0.24 best-fit
WMAP modelCMB acoustic peaks
Baryon acoustic oscillation
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Combined constraints from SN and BAO
w=-1.023±0.090(systematic)±0.054(statistical)
SN Legacy Survey(Astier et al. 2006)
SDSS galaxy BAO (Eisenstein et al. 2005)
Matter density parameter
Matter density parameterDar
k en
ergy
den
sity
par
amet
er
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future dark energy survey projectsDES: Dark Energy Survey (Fermi Lab+, 2011-?)
Imaging galaxy survey5000 deg2@Chile 4m telescope
HSC: Hyper Suprime-Cam (Subaru+Princeton, 2011-)Imaging galaxy survey 1.5deg FOV2000 deg2@Subaru 8m telescope
LSST: Large Synoptic Survey Telescope (SLAC+, 2014-?)Imaging galaxy survey20000 deg2@Chile 8.4m dedicated telescope
WFMOS: Wide Field Multi-Objects Spectrograph (Subaru+Gemini+???, 2015-???)
Spectroscopic galaxy survey 1.5deg FOV4000 fibers, 20000 galaxy redshifts a night
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Hyper Suprime-Cam projectMinistry of Education, Special Priority Area Grant-in-Aid: 2006-2011“Study of Dark Energy from Wide-Field Deep Survey of the Universe”Constraining dark energy via gravitational lensing survey
PI: Hiroshi Karoji (NAOJ)CCD: Satoshi Miyazaki (NAOJ)DAQ: Hiroaki Aihara (U.Tokyo)Theory groups at NAOJ, Univ. of Tokyo, Nagoya Univ. Tohoku Univ.
Princeton Univ. will join officially
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WFMOS proposal: Subaru+Geminispectroscopic survey
Observational constraints on dark energyAccurate measurement of the baryon acoustic scales in galaxy distribution4000 multi-fiber spectrograph on 1.5deg FOV cameta at Subaru prime focus
0.5<z<1.3: emission line galaxies2×106 gals/2000 deg2 ⇒ 1400 pointings(900hours)
2.3<z<3.3: Lyman-break galaxies6×105 gals/300 deg2 ⇒ 200 pointings(800hours)
Determine H(z) and D(z) within 1% precisionDetermine w within 3% precision and dw/dzwithin 25% precision
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modified gravity vs. cosmological constant: from SDSS to WFMOS
Yamamoto, Bassett, Nichol, Suto & YahataPRD 74(2006)063525, astro-ph/0605278
modified Friedmann equation (spatially flat)
n=2: DGP model, n=∞ : cosmological constant
rc: key parameter ~1/H0
r<rc: 4D space-time, r>rc: 5D space-timeif spatially flat
ρπ3
8/22
/22 G
rHH nc
n
=− −
mn
crH Ω−=− 1)( 2/20
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Predicted shifts of BAO peaks
Yamamoto et al. (2006)purely linear theory, observation in ΛCDM assumed
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Current constraints from the SDSS LRG sample
Yamamoto et al. (2006)
fit to linear theory for k<0.2hMpc-1
observation in ΛCDM assumed
data from Hütsi (astro-ph/0409278)
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Expected constraints from future WFMOS z=1 sample
Yamamoto et al. (2006)
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Univ. of TokyoRes. Center for
the Early Universecoordinator
Yasushi Suto
Princeton U.Dept. of
Astrophys. Sci.coordinator
Edwin Turner
CaltechDept. of Astron.
coordinatorRichard Ellis
Edingburgh U.Royal Obs.coordinator
John Peacock
CMBGravitational lensBaryon oscillation
SupernovaWeak lens mapping
Theoretical modelBaryon oscillationWeak lens mapping
NAOJTohoku Univ.
Hiroshima Univ.
Kyoto Univ.
Nagoya Univ.
International Research Network for Dark Energy(JSPS, core-to-core program 2007-2008)
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We now realize an amazing fact that our world beyond this blue sky is dominated by dark energy
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Let us thank our Earthfor wonderful dark nights