portsmouth
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Portsmouth. Cosmo – 02Chicago, September 2002. Models of inflation and primordial perturbations. David Wands Institute of Cosmology and Gravitation University of Portsmouth. V(). . just the kind of peculiar cosmological behaviour we observe today. Cosmological inflation:. - PowerPoint PPT PresentationTRANSCRIPT
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Portsmouth
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Models of inflation and primordial perturbations
David Wands
Institute of Cosmology and GravitationUniversity of Portsmouth
Cosmo – 02 Chicago, September 2002
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• period of accelerated expansion in the very early universe
• requires negative pressure e.g. self-interacting scalar field
• speculative and uncertain physics
Cosmological inflation: Starobinsky (1980)Guth (1981)
V()
•just the kind of peculiar cosmological behaviour we observe today
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• inflation in the very early universe • observed through primordial perturbation spectra
•gravitational waves (we hope)
•matter/radiation perturbations
Models of inflation:
gravitational
instability
new observational data offers precision tests of cosmological parameters and the nature of the
primordial perturbations
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Perturbations in FRW universe:
Characteristic timescales for comoving wavemode k
– oscillation period/wavelength a / k– Hubble damping time-scale H -1
• small-scales k > aH under-damped oscillator
• large-scales k < aH over-damped oscillator
03 2 Hwave equation
H-1 / a
conformal time
comoving wavelength, k-1
radiation or matter eradecelerated expansion
frozen-inoscillates
comoving Hubble length
inflationaccelerated expansion (or contraction)
vacuum
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Vacuum fluctuations
V()
• small-scale/underdamped zero-point fluctuations
• large-scale/overdamped perturbations in growing mode
linear evolution Gaussian random field
ke ik
k 2
2
3
232
2)2(
4
Hk k
aHk
fluctuations of any light fields (m<3H/2) `frozen-in’ on large scales
Hawking ’82, Starobinsky ’82, Guth & Pi ‘82
*** assumes Bunch-Davies vacuum on small scales ***probe of trans-Planckian effects for k/a > MPl Brandenberger & Martin (2000)
effect likely to be small for H << MPl Starobinsky; Niemeyer; Easther et al (2002)
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Inflation -> matter perturbations
HR
for adiabatic perturbations on super-horizon scales0R
during inflation scalar field fluctuation,
scalar curvature on uniform-field hypersurfaces
HR
during matter+radiation era
density perturbation,
scalar curvature on uniform-density
hypersurfaces
time
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high energy / not-so-slow roll1. large field ( MPl )
e.g. chaotic inflation
not-so-high energy / very slow roll2. small field
e.g. new or natural inflation
3. hybrid inflatione.g., susy or sugra models
Single-field models:
slow-roll solution for potential-dominated, over-damped evolution gives useful approximation to growing mode for { , || } << 1
2
22
16 HH
VVM P
2
22
8 Hm
VVM P
Kinney, Melchiorri & Riotto (2001)
0
0
0
see, e.g., Lyth & Riotto
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can be distinguished by observations• slow time-dependence during inflation
-> weak scale-dependence of spectra
• tensor/scalar ratio suppressed at low energies/slow-roll
261 n
162
2
R
T
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• Microwave background +2dF + BBN + Sn1A + HST
Lewis & Bridle (2002)
Observational constraints
08.0scalartensor
spectral index
261 n
Harrison-Zel’dovich
n 1, 0
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• additional fields may play an important role• initial state new inflation• ending inflation hybrid inflation• enhancing inflation assisted inflation
warm inflationbrane-world
inflation
• may yield additional information• non-gaussianity• isocurvature (non-adiabatic) modes
digging deeper:
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Inflation -> primordial perturbations (II)scalar field fluctuations density perturbationstwo fields (,) matter and radiation (m,)curvature of uniform-field slices curvature of uniform-density
slices
HR *
HR
aHkSS
RS
aHkSR
TT
SR
inflation*
*
primordial 01
model-dependent transfer functions
HSS
HSR
,
HS *
nn
nnSm
m
isocurvature
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initial power spectra:
uncorrelated at horizon-crossing
2
*
2*
2* 2
H
2
*
22
*2
* 2
HSR
0**** SR
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primordial power spectra:
correlated! Langlois (1999)2
*
2*
22
2*
22*
2
STTSR
STS
STRR
SSRS
SS
RS
correlation angle measures contribution of non-adiabatic modes to primordial curvature perturbation
22/122/12 1cos
RS
RS
T
T
SR
RS
can reconstruct curvature perturbation at horizon-crossing
222* sin RR
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consistency conditions:
single-field inflation: Liddle and Lyth (1992) Tn
R
T
R
TRR 8
2*
2*
2
22
*2
gravitational waves:
2
1632
2
2*
22
*2
T
Pl
n
RMHTT
two-field inflation: Wands, Bartolo, Matarrese & Riotto (2002) 22
2*
2*
2
2
sin8sin TnR
T
R
T
multi-field inflation: Sasaki & Stewart (1996)
TnR
TRR 8
2
22
*2
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microwave background predictions
adiabatic isocurvature correlation
Cl = A2 + B2 + 2 A B cos
Bucher, Moodley & Turok ’00 nS = 1 Trotta, Riazuelo & Durrer ’01Amendola, Gordon, Wands & Sasaki ’01
best-fit to Boomerang, Maxima & DASI
B/A = 0.3, cos = +1, nS = 0.8b = 0.02, cdm = 0.1, = 0.7
}
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curvaton scenario:
large-scale density perturbation generated entirely by non-adiabatic modes after inflation
assume negligible curvature perturbation during inflation 02
* R
Lyth & Wands, Moroi & Takahashi, Enqvist & Sloth (2002)
22,
2*
22 )/( decayRS STR
late-decay, hence energy density non-negligible at decaydecayRST ,
light during inflation, hence acquires isocurvature spectrum
2*S
•negligible gravitational waves
•100%correlated residual isocurvature modes
•detectable non-Gaussianity if ,decay<<1
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primordial non-gaussianitysimple definition in terms of conformal Newtonian potential =3R/5
where fNL = 0 for linear evolution 22
GaussGaussNLGauss f Komatsu & Spergel (2001)also Wang & Kamiokowski (2000)
significant constraints on fNL from all-sky microwave background surveys• COBE fNL < 2000
• MAP fNL < 20
• Planck fNL < 5theoretical predictions
• non-linear inflaton dynamics constrained fNL < 1 Gangui et al ‘94• dominant effect from second-order metric perturbations? Acquaviva et al (2002) • but non-linear isocurvature modes could allow fNL >> 1 Bartolo et al (2002)• e.g., curvaton fNL 1 / ,decay Lyth, Ungarelli & Wands (2002)
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Conclusions:1. Observations of tilt of density
perturbations (n1) and gravitational waves (>0) can distinguish between slow-roll models
2. Isocurvature perturbations and/or non-Gaussianity may provide valuable info
3. Non-adiabatic perturbations (off-trajectory) in multi-field models are an additional source of curvature perturbations on large scales
4. Consistency relations remain an important test in multi-field models - can falsify slow-roll inflation