Licia Verde. Introduction to cosmology. Lecture 4. Inflation

Transcription

1 Licia Verde Introduction to cosmology Lecture 4 Inflation

2 Dividing line

3 We see them like temperature On scales larger than a degree, fluctuations were outside the Hubble horizon at decoupling Potential hill Blueshifted Looks hotter Photons need to climb out of potential wells before they can travel to us (redshift or blueshift) Potential well redshifted Looks colder Given by

4 The horizon expands for a decelerated expansion

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6 There is time between when a perturbation enters the horizon (and starts oscillate) And decoupling, when oscillations freeze. And get imprinted in the CMB. Longer wavelength modes oscillate slower The frequency of the oscillation is equal to the wavenumber times the speed of sound: ω = kc s. The largest scales (sound horizon) can only go through a compression, Smaller scales can go through a compression and a rarefaction Etc Animations courtesy of W. Hu

7 Courtesy of WMAP

8 Power spectrum, again Challenge! rms 1 in 10 5 Even bigger challenge! Expand in spherical harmonics Legendre polynomials Angular power spectrum

9 compression Acoustic peaks (extrema) Rarefaction compression Primordial ripples Fundamental mode

10 compression Potential wells! m geometry baryons (extrema) Rarefaction compression Primordial ripples Fundamental mode

11 Courtesy of WMAP

12 Courtesy of WMAP

13 Today we have an extremely successful cosmological model Think of Friedmann equations, few parameters If we add perturbations:

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17 Impressive agreement: All with a handful of parameters

18 The very latest constraints Forget green for now From Reid et al 09

19 The cosmological model Precision cosmology Basic cosmological parameters known with ~% precision

20 ASIDE (advanced topic!) (by popular request) Neutrinos in cosmology 2 effects: 2 parameters N eff Number of effective neutrino species Neutrinos were behaving like radiation in the very early universe This affects the expansion history and matter radiation equality Mass eignestate They free stream (out of potential wells), damping small-scale perturbations (I.e. cosmological structures)

21 The standard cosmological model 96% of the Universe is missing!!! Major questions : Questions that can be addressed exclusively by looking up at the sky 1)What created the primordial perturbations? 2) What makes the Universe accelerate? These questions may not be unrelated

22 Successes of the Big Bang model GR+cosmological principle Hubble s law CMB Abundance of light elements

23 .. And problems Flatness problem Horizon problem Monopole problem Origin of perturbations

24 The flatness problem Remember Friedmann equations? today For most of the life of the universe: matter+radiation only Matter domination Exercise: Universe was flatter in the past! Radiation dominated Exercise:

25 Very quickly you find that early on 1-Ω <10-60 It is like balancing a pencil on its tip, coming back years later and still fining it balancing on its tip

26 The Horizon problem Different type of Horizons in Cosmology Since light travels at a final speed & Universe is expanding PARTICLE HORIZON: Maximum comoving distance light can have propagated in ti to tf Accounts for all the past expansion history Given the same dt, dp can be very different if a(t) is weird! HUBBLE HORIZON: c/h or c/t0. For normal expansion histories dp ~ c/h For weird ones BEWARE!

27 The Horizon problem The universe is homogeneous and isotropic on large scales 2.726K Consider 2 antipodal points they are separated by 2d H ~30000 Mpc What was the Hubble radius (horizon) back then? Only points at ~0.2 Mpc could have talked

28 Small aside c_s ~c Compare with the size of the CMB spots!

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30 The last scattering surface can be divided in patches of degree size I.e horizons. How could they all be at 2.726K? Imagine students taking an exam, and all returning THE SAME exam down to the commas

31 The monopole problem Phase transitions (water freezing, Magnetization )

32 Defects. Domain walls Cosmic strings monopoles Example from a nematic liquid crystal The most dangerous ones are the monopoles The fact that we are here means that at max there is one monopole in the entire observable universe.

33 And where the heck these perturbations come from?

34 INFLATION to the rescue Started in the 1980 with A. Guth, active research area. Still a paradigm not a proven fact Postulate a period of accelerated expansion at the very beginning! Something like a cosmological constant Different scenarios, particle-physics motivated (?)

35 Why is the Universe so BIG? Inflation to the rescue: an accelerated expansion Inflation begins Inflation ends Example: Even if inflation lasts for NOT BAD!

36 Any weirdness like monopole Would be diluted away!

37 Something like a Λ Inflation solves the Flatness problem For N~100 NOT BAD!

38 Inflation Solves the Flatness Looks curved Problem Looks Flat!!???.. What made the Universe so flat? What made the Universe so big? What made the universe so uniform? What seeded the galaxies?

39 Why is the Universe so uniform? Inflation solves that

40 Inflation solves the Horizon problem In an accelerated expansion the particle horizon and the Hubble horizon can be VERY DIFFERENT Given the same dt, dp can be very different if a(t) is weird!

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43 As an added bonus: Inflation generates Gaussian perturbations: quantum fluctuations stretched to become classical by the expansion. The mechanism is similar to Hawkings radiation. (The event horizon being the complementary concept to the particle horizon ) Turns out that the power spectrum of these perturbations will be a power law: different model of inflation predict slightly different power laws, but all close to scale invariant..

44 Perturbations outside the Horizon? Inflation solves that Fluctuations frozen in

45 CAN THIS BE TESTED? flatness Power law primordial power spectrum Can even hope to distinguish specific models Super horizon fluctuations (polarization) gaussianity Can even hope to distinguish specific models Stochastic background of gravity waves (polarization)

46 Putting it all together Have a cosmological model The parameters are well measured 2 big puzzles: Origin of fluctuations (what made the Universe inflate?) Cosmological constant or dark energy: what is that?