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Cosmological Inflation: History and Present Status
36

Cosmological Inflation: History and Present Status.

Jan 12, 2016

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Page 1: Cosmological Inflation: History and Present Status.

Cosmological Inflation: History and Present Status

Page 2: Cosmological Inflation: History and Present Status.

Motivated by the book:Breakthrough Beyond the Edge of the World

Valery Rubakov

Alexei Starobinsky

Andrei Linde

Vyacheslav Mukhanov

Vla

dim

ir Lu

kash

Page 3: Cosmological Inflation: History and Present Status.

The first cosmological revolution 1916 - 1929

Rmn – ½ R gmn – 8pL gmn = 16pc-4G Tmn

Page 4: Cosmological Inflation: History and Present Status.

The universe is not just a containment of everything that exists –

This is a physical object!

- Geometry: a closed 3D space + time

- Size: unknown but > 1012 light years

- Dynamics: accelerating expansion

- Density: 10-29 g/сm3

- Equation of state: pressure = 0 (dust)

- Temperature: 2.7о К

- Total energy: 0 (Zero!)

Page 5: Cosmological Inflation: History and Present Status.

Big Bang problems

- Horizon problem (Charles Misner): Universe is the same in the causally unconnected regions

- Flatness problem (W = 1), or r = rc

- Cosmic junk problem: lack of monopoles, cosmic strings etc.

- Entropy problem: ~ 1090 particles within horizon

Page 6: Cosmological Inflation: History and Present Status.

Vladimir Lukash about 1970-ies:

They worked in the frames of “Cosmological postulate”: all problems come from initial conditions that we have to postulate.

Nobody was happy (except theologists) but how to work otherwise?

Observations: r is at most 10% of the critical value (Peebles & Tali).

However it was clear that any value of W degrades very fast to 0 or infinity except W = 1 exactly (Dicke)

The anthropic principle was treated in Zeldovich school as a bad style science

Mid 70-ies: Gunn & Tinsley: the negative deceleration parameter derived from the Hubble diagram (acceleration)

The issue of H: H ~50 km/s/Mpc versus ~75 km/s/Mpc (too young Universe)

Page 7: Cosmological Inflation: History and Present Status.

Reincarnation of the L-term (cosmological term)

Rmn – ½ R gmn – 8pL gmn = 16pc-4G Tmn

( �̇�𝑎 )2- 8/3pL =

G - e 𝑘𝑅𝑜2𝑎 (𝑡 ) 2

Vacuum (p = - e) 𝑎=𝑒𝑡 𝐻

p = w e 𝑎=𝑡2

3 (1+𝑤)

Page 8: Cosmological Inflation: History and Present Status.

The first hint:

Brout, Englert & Gunzig 1961 Creation of Universe ex nihilis with a massive scalar field (a toy model)

The next attempt:

Erast Gliner 1969: non-singular bounce due to “heavy vacuum” with p = -e

Contraction -> expansion through de-Sitter stage

Gliner & Dymnikova 1975: It solves problems of flatness (big Universe) and of a large entropy

Page 9: Cosmological Inflation: History and Present Status.

1980 – The start of the second cosmological revolution

1980 – Starobinsky presents his model and meets criticism for a wrong scenario

1980 Mukhanov & Chibisov claim that de-Sitter stage is necessary to get galaxies from quantum fluctuations 1981 Mukhanov & Chibisov - primordial scalar perturbations and their spectrum

1981 Guth publishes his famous paper

1982 Linde - New inflation (slow roll) + Steinhardt & Albercht (3 month later)

1983 Linde - Chaotic inflation

1986 Linde - Eternal inflation

Page 10: Cosmological Inflation: History and Present Status.

Alexei Starobinsky: modified gravitation

R2 appears as a result of Kazimir effect at a large curvature

Scenario: Universe has started from a pure de-Sitter world which existed indefinite time. Then it dissipated into hot Friedman Universe.

Mukhanov & Others: de-Sitter world is unstable because of quantum fluctuations and incompatible with contraction stage.

Zeldovich: The model can be interpreted as a way of Universe creation from nothing

Vilenkin has formalized this as a tunnel transition.

𝑅→𝑅− 𝑅2

6𝜇

Page 11: Cosmological Inflation: History and Present Status.

Mukhanov & Chibisov: primordial scalar perturbations

Virtual quantum fluctuations produce real perturbations under variable metric

Gravitational waves – Leonid Grischuk

Gravitational waves (tensor perturbations) in Starobinsky model – Starobinsky

Production of scalar perturbations – Lukash (general formalism),

Mukhanov & Chibisov – the concrete result for the concrete model (of Starobinsky) , including the spectrum of perturbations:

First approximation – ns = 1 (flat spectrum) Next approximation – ns = 0.96

Page 12: Cosmological Inflation: History and Present Status.

f

V(f

, T)

Alan Guth:

Scenario of inflation

1. Thermal equilibrium

2. Phase transition

3. Supercooling + Exponential expansion

4. “Boiling” – reheating

Page 13: Cosmological Inflation: History and Present Status.

Answers:

1. The flatness problem is evidently solved with expansion by many orders of magnitude (Wk ~ 10-100, e.g)

2. The horizon problem disappears because all we see inside the horizon was a causally connected piece of a uniform heavy vacuum.

3. All exotic “defects” were swept away during inflation out of the horizon

4. A huge entropy results from the decay of self-reproducing scalar field

Page 14: Cosmological Inflation: History and Present Status.
Page 15: Cosmological Inflation: History and Present Status.

New inflation

f+ 3 H f + V’( )f = 0.. .

Linde 1982

Albrecht & Steinhardt3 months later

Page 16: Cosmological Inflation: History and Present Status.
Page 17: Cosmological Inflation: History and Present Status.

Chaotic inflation Linde 1983

f > Mpl

f(x) – homogeneous at ~ 10 Rhor

Page 18: Cosmological Inflation: History and Present Status.

Starobinsky model in terms of a scalar field

V(f) ~ log2 (f)

Page 19: Cosmological Inflation: History and Present Status.

Ethernal inflation Linde 1986

Planck limit

Page 20: Cosmological Inflation: History and Present Status.

Andrei Linde

Page 21: Cosmological Inflation: History and Present Status.
Page 22: Cosmological Inflation: History and Present Status.

Predictions (According to Slava Mukhanov)

1. Flatness W=1

2. Spectral slope of primordial perturbations ns ~ 0.96 – 0.97

3. Gaussianity

4. Adiabaticity

5. Gravitational waves

Page 23: Cosmological Inflation: History and Present Status.

WMAP 2001 – 2010

Band 0.32 – 1.3 см

Thermal equilibrium in the shadow ~40К

Mirror 1.4 Х 1.6 м

The data were opened in 2002

«Планк» 2009 – 2013

Band 0.035 – 1см

Liquid helium

Mirror 1.5 Х 1.9 м

Data opening: 2013?

Page 24: Cosmological Inflation: History and Present Status.

What one can see on this picture?Cold spot, “fingers”, concentric rings. Also “SH”,

Zuntz, Zibin, Zunkel & Zwart, 01/04/2014

Page 25: Cosmological Inflation: History and Present Status.

What we have to search in this map?

A.D. Sakharov 1963.

Primordial perturbations produce acoustic waves

with common phase. (Standing waves)

Waves coming to recombination with the phase

p, 2p, 3 p have maximal amplitudes

- With the phase p/2, 3p/2, 5p/2 – minimal amplitudes

Sakharov assumed a wrong model (cold universe) where peaks were of a very short scale

Reconsidered for correct model

Sunyaev & Zeldovich + Peebles & Yu

Sakharov oscillations are observable!

Page 26: Cosmological Inflation: History and Present Status.

Silk effect

Page 27: Cosmological Inflation: History and Present Status.

Fit of the multipole spectrum

Free parameters:1. The amplitude of primordial perturbations (normalization)

2. The spectral slope (with a deviation from a flat)

3. The share of the baryonic matter (affects the height of the first peak)

4. The share of the dark matter (affects the ratio between peaks)

5. The curvature parameter W (defines the angular scale of the whole picture)

6. Free electron optical depth (reionization z) affects the curve at low L

-----------------------

Page 28: Cosmological Inflation: History and Present Status.

Curvature

Wk = 0.001+-0.006

Dark matter

Wc = 0.259+-0.005

Baryonic matter

Wb = 0.048+-0.001

Page 29: Cosmological Inflation: History and Present Status.

1. W = 1 (Flat Universe) ++!! Planck + other data: W = 0.001 +/- 0.007

2.. Ns = 0.96 – 0.97 ++! ns = 0.96 +/- 0.07

3. Adiabaticity Confirmed (position of acoustic peaks)

4. Gaussianity Confirmed at the level ruling out complicated models

Linde: there was a rumor that WMAP has observed a non-gaussianity. Some people were excited. The rumor had no ground.

5. Gravitational waves Not confirmed yet

Predictions / Measurements

Page 30: Cosmological Inflation: History and Present Status.

Starobinsky model

BICEP2

Page 31: Cosmological Inflation: History and Present Status.

It was too early to drink champagne!

BICEP 2

South pole

Page 32: Cosmological Inflation: History and Present Status.

B-mode at the level r = 0.2

The result is in contradiction with Planck data (too large)

Поляризованная пыль?

Page 33: Cosmological Inflation: History and Present Status.
Page 34: Cosmological Inflation: History and Present Status.

Alternatives

Steinhardt & Turok Ekpyrotic model Bounce due to brane collision

p > + !eStrong criticism by Andrei Linde and others(pyrotechnical model)

Rubakov A primordial vacuum with conform invariance No massive particles, no gravity, no scale (… and the Sent Spirit flied over the water)

A spontaneous breaking

Hot Fridman Universe

Page 35: Cosmological Inflation: History and Present Status.

Linde, Mukhanov, Stasrobinsky:

Inflation theory is simple (in ideology), solves all problems and has predicted future observations.

Alternatives are more complicated, require additional entities and give no clear predictions

Rubakov:

Until primordial gravitational waves are detected alternative models have a right for existence (and it is worth to wait with Nobel prize)

However, one part of the theory has no alternatives: the quantum production of primordial perturbations by Mukhanov $ Chibisov

Page 36: Cosmological Inflation: History and Present Status.

My impressions:

- Inflation theory far exceeds alternatives in ideological simplicity and predictive power. Also the most economical in the sense of extra entities.

- Among the inflation models the best is that of Alexei Starobinsky with the same reason.

- William Occam probably would agree with me.