Making and Probing Inflation Lev Kofman KITPC Beijing November 6 2007 Making Inflation in String Theory How small can be r Gravity Waves from Preheating.

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Presentation transcript:

Making and Probing Inflation Lev Kofman KITPC Beijing November Making Inflation in String Theory How small can be r Gravity Waves from Preheating

Concise History of the Early Universe

Early Universe Inflation Scale factor time Realization of Inflation

Inflation in the context of ever changing fundamental theory inflationOld Inflation New Inflation Chaotic inflation Double Inflation Extended inflation DBI inflation Super-natural Inflation Hybrid inflation SUGRA inflation SUSY F-term inflation SUSY D-term inflation SUSY P-term inflation Brane inflation K-flation Roulette Warped Brane inflation inflation Power-law inflation Tachyon inflation Racetrack inflation Assisted inflation

Family phase portrait of inflation

string theorist CY AdS 3+1 FRW Inflation in String Theory: Cosmology with Compactification

string theorist CY AdS 3+1 FRW Inflation in String Theory: Cosmology with Compactification 3+1 FRW CY cosmologist

Modular Inflation. Modular Inflation. They use Kahler moduli/axion like the fields that are a present in the KKLT stabilization. Brane inflation. Brane inflation. The inflaton field corresponds to the distance between branes in Calabi-Yau space. Historically, this was the first class of string inflation models. Modular Inflation. Modular Inflation. They use Kahler moduli/axion like the fields that are a present in the KKLT stabilization. Brane inflation. Brane inflation. The inflaton field corresponds to the distance between branes in Calabi-Yau space. Historically, this was the first class of string inflation models. String Theory inflation models

Inflation with branes in String Theory 4-dim picture Prototype of hybrid inflation

Inflation with branes in String Theory 4-dim picture Prototype of hybrid inflation throat warped geometry Mobile brane KKLMMT

m  2 = 2H Conformal coupling problem Due to conformal coupling effective inflaton mass Expected to prevent inflation

m  2 = 2H Conformal coupling problem Due to conformal coupling effective inflaton mass Expected to prevent inflation Rapid-roll Inflation with conformal coupling

Scalar field non-minimally coupling with gravity

Rapid-roll inflation with conformal field De Sitter solution

Efoldings warping

Efoldings and mass hierarchy Energy scale

Efoldings and mass hierarchy solution

Kahler moduli Inflation (Conlon&Quevedo hep-th/050912) Roulette Inflation-Kahler moduli/axion (Bond, LK, Prokushkin&Vandrevange hep-th/ )

String theory landscape of the Kahler moduli/axion Inflation

Ensemble of Inflationary trajectories

Lessons: Multiple fields Inflation Ensemble of acceleration histories (trajectories) for the same underlying theory Prior probabilities of trajectories P(H(t)) Small amplitude of gravity waves r from inflation

Generation of gravitational waves from inflation

time Hubble radius end of inflation recombination

inflation Hot FRW Initial conditions from Inflation

Baumann&Mcallister hep-th/ Lyth hep-ph/ Efstathiou &Mack astro-ph/

.Spider Balloon Planck Satellite CMBPol 2017 Measurement of GW from CMB anisotropy polarization < 0.34 Current limit Ultimate limit

superheavy gravitino A discovery or non-discovery of tensor modes would be a crucial test for string theory and particle phenomenology unobservable for inflationary perturbations KKLT Kallosh, Linde hepth/ Amplitude of GW and gravitino mass

Particlegenesis time Inflation no entropy no temperature BANG

Occupation number Classical Quantum Resonant Preheating in Chaotic Inflation

preheating exp excitation Kolmogorov turbulence of bosons thermalization Non-linear “bubbly” stage

Classical Quantum Decay of inflaton and preheating after inflation movie Felder, LK hep-ph/

Classical Quantum Decay of inflaton and preheating after inflation movie

Classical Quantum Decay of inflaton and preheating after inflation

Evolutionof energy density Evolution of gravitational potential l A. Frolov 07

Tachyonic Preheating in Hybrid Inflation l movie

Tachyonic Preheating

Generation of gravitational waves from random media

time Hubble radius end of inflation recombination

Stochastic background of gravitational waves emitted from preheating after inflation

Emission of stochastic GW by random media

Emission of stochastic GW by random scalar fields First order phase transitions Second order phase transitions Topological defects formation Thermal bath of scalars Tachyonic preheating Resonant preheating

No GW emission

GW generated for non-trivial dispersion relation

Random gaussian fields

Emission of GW from preheating

Numerical calculations of GW emission from Preheating

Analytic check

estimation Shortcut to the answer Felder, LK hep-ph/

topological effects after hybrid inflation (unstable) formation of defects results in GW emission

Application to particular hybrid model

GW from high energy inflation are targeted by CMB B-mode polarization experiments The story of stochastic gravitational waves is CMB anisotropies of 21 century GW from low-energy inflation are targeted by GW astronomy