Inflation and Fundamental Physics

Slides:



Advertisements
Similar presentations
The Nuts and Bolts of Inflation Richard Barrett. Dark Energy SeminarGlasgow 29/11/2003 Inflation What is inflation? What is dark energy? Why was inflation.
Advertisements

The universe today is very nearly flat: It was apparently much flatter in the past: For definiteness, pick g eff =200 and k B T = 3  GeV You should.
Inflation Jo van den Brand, Chris Van Den Broeck, Tjonnie Li Nikhef: April 23, 2010.
Gradient expansion approach to multi-field inflation Dept. of Physics, Waseda University Yuichi Takamizu 29 th JGRG21 Collaborators: S.Mukohyama.
The Cosmological Slingshot Scenario A Stringy Proposal for Early Time Cosmology: Germani, NEG, Kehagias, hep-th/ Germani, NEG, Kehagias, arXiv:
Cosmology and extragalactic astronomy Mat Page Mullard Space Science Lab, UCL 10. Inflation.
Phenomenological Classification of Inflationary Potentials Katie Mack (Princeton University) with George Efstathiou (Cambridge University) Efstathiou &
Cosmological Structure Formation A Short Course
History of the Universe - according to the standard big bang
The Statistically Anisotropic Curvature Perturbation from Vector Fields Mindaugas Karčiauskas Dimopoulos, MK, JHEP 07 (2008) Dimopoulos, MK, Lyth, Rodriguez,
IFIC, 6 February 2007 Julien Lesgourgues (LAPTH, Annecy)
Quintessence – Phenomenology. How can quintessence be distinguished from a cosmological constant ?
New Inflation Amy Bender 05/03/2006. Inflation Basics Perturbations from quantum fluctuations of scalar field Fluctuations are: –Gaussian –Scale Invariant.
InflationInflation Andrei Linde Lecture 1. Plan of the lectures: Inflation: a general outlook Basic inflationary models (new inflation, chaotic inflation,
THE GRACEFUL EXIT FROM INFLATION AND DARK ENERGY By Tomislav Prokopec Publications: Tomas Janssen and T. Prokopec, arXiv: ; Tomas Janssen, Shun-Pei.
Cosmic Inflation Tomislav Prokopec (ITP, UU) Utrecht Summer School, 28 Aug 2009 ˚ 1˚ WMAP 3y 2006.
Yoshiharu Tanaka (YITP) Gradient expansion approach to nonlinear superhorizon perturbations Finnish-Japanese Workshop on Particle Helsinki,
1 Multi-field Open Inflation & Instanton YITP, Kyoto University Kazuyuki Sugimura (Collaborator : D. Yamauchi and M. Sasaki)
Black hole production in preheating Teruaki Suyama (Kyoto University) Takahiro Tanaka (Kyoto University) Bruce Bassett (ICG, University of Portsmouth)
Emergent Universe Scenario
Quantum vacuum in cosmology. What is the vacuum in cosmology ?
THE LARGE SCALE CMB CUT-OFF AND THE TENSOR-TO-SCALAR RATIO Gavin Nicholson Imperial College London with Carlo Contaldi Imperial College London (astro-ph/ )
Quantum cosmology and scale invariance. quantum gravity with scalar field – the role of scale symmetry.
Dilaton quantum gravity and cosmology. Dilaton quantum gravity Functional renormalization flow, with truncation :
1 Circular Polarization of Gravitational Waves in String Cosmology MIAMI, 200 7 Jiro Soda Kyoto University work with Masaki Satoh & Sugumi Kanno.
Probing the Reheating with Astrophysical Observations Jérôme Martin Institut d’Astrophysique de Paris (IAP) 1 [In collaboration with K. Jedamzik & M. Lemoine,
A nonequilibrium renormalization group approach to turbulent reheating A case study in nonlinear nonequilibrium quantum field theory J. Zanella, EC Part.
Yugo Abe (Shinshu University) July 10, 2015 In collaboration with T. Inami (NTU), Y. Kawamura (Shinshu U), Y. Koyama (NCTS) YA, T. Inami,
Dilaton quantum gravity and cosmology. Dilaton quantum gravity Functional renormalization flow, with truncation :
Non-Gaussianity, spectral index and tensor modes in mixed inflaton and curvaton models Teruaki Suyama (Institute for Cosmic Ray Research) In collaboration.
Fibre Inflation High-Fibre models from regular potentials String Pheno Workshop: CERN 2008 C.P. Burgess with M. Cicoli and F.Quevedo.
Big bang or freeze ?. conclusions Big bang singularity is artefact Big bang singularity is artefact of inappropriate choice of field variables – of inappropriate.
PHY th century cosmology 1920s – 1990s (from Friedmann to Freedman)  theoretical technology available, but no data  20 th century: birth of observational.
General Relativity Physics Honours 2008 A/Prof. Geraint F. Lewis Rm 560, A29 Lecture Notes 10.
Big bang or freeze ?. conclusions Big bang singularity is artefact Big bang singularity is artefact of inappropriate choice of field variables – of inappropriate.
Inflationary Theory of Primordial Cosmological Perturbation Project for General Relativity (Instructor: Prof.Whiting) Sohyun Park.
Can observations look back to the beginning of inflation ?
Dark Energy in the Early Universe Joel Weller arXiv:gr-qc/
Quantum Noises and the Large Scale Structure Wo-Lung Lee Physics Department, National Taiwan Normal University Physics Department, National Taiwan Normal.
IRGAC Cosmological perturbations in stochastic gravity Yuko Urakawa with Kei-ichi Maeda.
ETSU Astrophysics 3415: “The Concordance Model in Cosmology: Should We Believe It?…” Martin Hendry Nov 2005 AIM:To review the current status of cosmological.
Theory and observations
Collapse of Small Scales Density Perturbations
Quintessential Inflation
Formation of universe, blackhole and 1st order phase transition
The Origin and the Fate of the Universe
Recent status of dark energy and beyond
Monday, November 12, 2007 Vilenkin Chs: 1-3.
US Treasury & Its Borrowing
Inflation with a Gauss-Bonnet coupling
AOE/ESM 4084 Engineering Design Optimization
Technology Update Kris Young Director of Technology
String/Brane Cosmology
Quantum Spacetime and Cosmic Inflation
Summer Success Academy Program Analysis Spring 2016
Adaptive Perturbation Theory: QM and Field Theory
Shintaro Nakamura (Tokyo University of Science)
Final Budget Amendment and Proposed Budget
Can trans-Planckian Physics be seen in the CMB? C.P. Burgess
General, single field Inflation
Big bang or freeze ?.
2015/16 Evaluation Summary October 4, 2016 Jordan Harris
2016 State Assessment Results
Business Services Update Board of Education Workshop December 1, 2015
TROY SCHOOL DISTRICT ENROLLMENT PROJECTIONS February 7, 2017
2015/16 Evaluation Summary October 18, 2016 Jordan Harris
Final Budget Amendment and Proposed Budget
Business Services Update Board of Education Workshop March 7, 2017
Binhai Zhu Computer Science Department, Montana State University
Binhai Zhu Computer Science Department, Montana State University
Presentation transcript:

Inflation and Fundamental Physics What do cosmological measurements say about the very early universe? C.P. Burgess Frequently, presenters must deliver material of a technical nature to an audience unfamiliar with the topic or vocabulary. The material may be complex or heavy with detail. To present technical material effectively, use the following guidelines from Dale Carnegie Training®.   Consider the amount of time available and prepare to organize your material. Narrow your topic. Divide your presentation into clear segments. Follow a logical progression. Maintain your focus throughout. Close the presentation with a summary, repetition of the key steps, or a logical conclusion. Keep your audience in mind at all times. For example, be sure data is clear and information is relevant. Keep the level of detail and vocabulary appropriate for the audience. Use visuals to support key points or steps. Keep alert to the needs of your listeners, and you will have a more receptive audience. with M. Cicoli, M.Gomez-Reino,G.Tasinato, F.Quevedo and I.Zavala

Outline Inflation String inflation Why is it so widely believed to have happened? What can we expect to learn? String inflation Why build models only a mother could love? UniverseNet Inflation

Outline Inflation String inflation Why is it so widely believed to have happened? What can we expect to learn? String inflation Why build models only a mother could love? UniverseNet Inflation

Inflation Who says it took place? What might one hope to learn if so? Start with the picture of how scales evolve during and after inflation; Describe the inflaton-metric system in its original and Mukhanov form; Describe the squeezing of the Mukhanov vacuum into the Bunch-Davies vacuum UniverseNet Inflation

Inflation Who says it took place? What might one hope to learn if so? WMAP Concordance cosmology provides a great description of the wealth of cosmological data. Who says it took place? What might one hope to learn if so? Start with the picture of how scales evolve during and after inflation; Describe the inflaton-metric system in its original and Mukhanov form; Describe the squeezing of the Mukhanov vacuum into the Bunch-Davies vacuum UniverseNet Inflation

Inflation Who says it took place? What might one hope to learn if so? NCSA simulation Evidence supports the picture that structure forms from the collapse of an initially uniform distribution. Who says it took place? What might one hope to learn if so? Start with the picture of how scales evolve during and after inflation; Describe the inflaton-metric system in its original and Mukhanov form; Describe the squeezing of the Mukhanov vacuum into the Bunch-Davies vacuum UniverseNet Inflation

Inflation Who says it took place? What might one hope to learn if so? Concordance model works well, if the universe starts off in just the right way: Initially very flat: Initially very homogeneous: surprise given speed of expansion seem to be no primordial defects Who says it took place? What might one hope to learn if so? Start with the picture of how scales evolve during and after inflation; Describe the inflaton-metric system in its original and Mukhanov form; Describe the squeezing of the Mukhanov vacuum into the Bunch-Davies vacuum UniverseNet Inflation

Inflation Who says it took place? What might one hope to learn if so? Concordance model works well, if the universe starts off in just the right way: Initially very flat: Initially very homogeneous: surprise given speed of expansion seem to be no primordial defects Who says it took place? What might one hope to learn if so? Radiation domination: Matter domination: Start with the picture of how scales evolve during and after inflation; Describe the inflaton-metric system in its original and Mukhanov form; Describe the squeezing of the Mukhanov vacuum into the Bunch-Davies vacuum UniverseNet Inflation

Inflation Who says it took place? What might one hope to learn if so? Concordance model works well, if the universe starts off in just the right way: Initially very flat: Initially very homogeneous: surprise given speed of expansion seem to be no primordial defects Who says it took place? What might one hope to learn if so? Start with the picture of how scales evolve during and after inflation; Describe the inflaton-metric system in its original and Mukhanov form; Describe the squeezing of the Mukhanov vacuum into the Bunch-Davies vacuum UniverseNet Inflation

Inflation Who says it took place? What might one hope to learn if so? Concordance model works well, if the universe starts off in just the right way: Initially very flat: Initially very homogeneous: surprise given speed of expansion seem to be no primordial defects Who says it took place? What might one hope to learn if so? Initially very homogeneous Start with the picture of how scales evolve during and after inflation; Describe the inflaton-metric system in its original and Mukhanov form; Describe the squeezing of the Mukhanov vacuum into the Bunch-Davies vacuum UniverseNet Inflation

Inflation Who says it took place? What might one hope to learn if so? Concordance model works well, if the universe starts off in just the right way: Initially very flat: Initially very homogeneous: surprise given speed of expansion seem to be no primordial defects Who says it took place? What might one hope to learn if so? Initially very homogeneous Start with the picture of how scales evolve during and after inflation; Describe the inflaton-metric system in its original and Mukhanov form; Describe the squeezing of the Mukhanov vacuum into the Bunch-Davies vacuum UniverseNet Inflation

Inflation Who says it took place? What might one hope to learn if so? Concordance model works well, if the universe starts off in just the right way: Initially very flat: Initially very homogeneous: surprise given speed of expansion seem to be no primordial defects Who says it took place? What might one hope to learn if so? fluctuations freeze once larger than H-1, so the problem is while so the product aH decreases with t Start with the picture of how scales evolve during and after inflation; Describe the inflaton-metric system in its original and Mukhanov form; Describe the squeezing of the Mukhanov vacuum into the Bunch-Davies vacuum UniverseNet Inflation

Inflation Who says it took place? What might one hope to learn if so? Concordance model works well, if the universe starts off in just the right way: Initially very flat: Initially very homogeneous: surprise given speed of expansion seem to be no primordial defects Who says it took place? What might one hope to learn if so? fluctuations freeze once larger than H-1, so the problem is while so the product aH decreases with t Start with the picture of how scales evolve during and after inflation; Describe the inflaton-metric system in its original and Mukhanov form; Describe the squeezing of the Mukhanov vacuum into the Bunch-Davies vacuum UniverseNet Inflation

Inflation Who says it took place? What might one hope to learn if so? Concordance model works well, if the universe starts off in just the right way: Initially very flat: Initially very homogeneous: surprise given speed of expansion seem to be no primordial defects Who says it took place? What might one hope to learn if so? Possible solution: extrapolation into the past is wrong Start with the picture of how scales evolve during and after inflation; Describe the inflaton-metric system in its original and Mukhanov form; Describe the squeezing of the Mukhanov vacuum into the Bunch-Davies vacuum eg: if the universe bounced UniverseNet Inflation

Inflation Who says it took place? What might one hope to learn if so? Concordance model works well, if the universe starts off in just the right way: Initially very flat: Initially very homogeneous: surprise given speed of expansion seem to be no primordial defects Who says it took place? What might one hope to learn if so? Possible solution: extrapolation into the past is wrong Start with the picture of how scales evolve during and after inflation; Describe the inflaton-metric system in its original and Mukhanov form; Describe the squeezing of the Mukhanov vacuum into the Bunch-Davies vacuum but: how do you get a bounce? UniverseNet Inflation

Inflation Who says it took place? What might one hope to learn if so? Concordance model works well, if the universe starts off in just the right way: Initially very flat: Initially very homogeneous: surprise given speed of expansion seem to be no primordial defects Who says it took place? What might one hope to learn if so? Possible solution: extrapolation into the past is wrong Start with the picture of how scales evolve during and after inflation; Describe the inflaton-metric system in its original and Mukhanov form; Describe the squeezing of the Mukhanov vacuum into the Bunch-Davies vacuum or: if the expansion accelerated UniverseNet Inflation

Inflation Who says it took place? What might one hope to learn if so? Concordance model works well, if the universe starts off in just the right way: Initially very flat: Initially very homogeneous: surprise given speed of expansion seem to be no primordial defects Who says it took place? What might one hope to learn if so? Possible solution: extrapolation into the past is wrong Start with the picture of how scales evolve during and after inflation; Describe the inflaton-metric system in its original and Mukhanov form; Describe the squeezing of the Mukhanov vacuum into the Bunch-Davies vacuum require aH to grow by ~ e60 UniverseNet Inflation

Inflation Who says it took place? What might one hope to learn if so? Concordance model works well, if the universe starts off in just the right way: Initially very flat: Initially very homogeneous: surprise given speed of expansion seem to be no primordial defects Who says it took place? What might one hope to learn if so? Possible solution: extrapolation into the past is wrong Start with the picture of how scales evolve during and after inflation; Describe the inflaton-metric system in its original and Mukhanov form; Describe the squeezing of the Mukhanov vacuum into the Bunch-Davies vacuum but: why should it start? Or end? UniverseNet Inflation

Inflation Who says it took place? What might one hope to learn if so? courtesy A. Linde Concordance model works well, if the universe starts off in just the right way: Initially very flat: Initially very homogeneous: surprise given speed of expansion seem to be no primordial defects Who says it took place? What might one hope to learn if so? Possible solution: extrapolation into the past is wrong Start with the picture of how scales evolve during and after inflation; Describe the inflaton-metric system in its original and Mukhanov form; Describe the squeezing of the Mukhanov vacuum into the Bunch-Davies vacuum and must it end everywhere? UniverseNet Inflation

Inflation Who says it took place? What might one hope to learn if so? A. Guth Archetype: if p = - r then Friedmann eq implies much like dark energy (but with a larger H) Who says it took place? What might one hope to learn if so? Start with the picture of how scales evolve during and after inflation; Describe the inflaton-metric system in its original and Mukhanov form; Describe the squeezing of the Mukhanov vacuum into the Bunch-Davies vacuum UniverseNet Inflation

Inflation Who says it took place? What might one hope to learn if so? A. Guth; A. Linde; A. Albrecht & P. Steinhardt How to achieve p = - r ? For a single homogeneous scalar field so homogeneous slow roll can make things work Who says it took place? What might one hope to learn if so? Start with the picture of how scales evolve during and after inflation; Describe the inflaton-metric system in its original and Mukhanov form; Describe the squeezing of the Mukhanov vacuum into the Bunch-Davies vacuum UniverseNet Inflation

Inflation Who says it took place? What might one hope to learn if so? Lyth So Hubble scale is approximately constant provided are small Who says it took place? What might one hope to learn if so? Start with the picture of how scales evolve during and after inflation; Describe the inflaton-metric system in its original and Mukhanov form; Describe the squeezing of the Mukhanov vacuum into the Bunch-Davies vacuum UniverseNet Inflation

Inflation Who says it took place? What might one hope to learn if so? For example V = (1/2) m2 f2 (large-field model) then positive and ~ e are small for large f. (Must then have m not too large.) Also, inflation ends as f is driven to smaller values. Who says it took place? What might one hope to learn if so? Start with the picture of how scales evolve during and after inflation; Describe the inflaton-metric system in its original and Mukhanov form; Describe the squeezing of the Mukhanov vacuum into the Bunch-Davies vacuum UniverseNet Inflation

Inflation Who says it took place? What might one hope to learn if so? Large-field variation V = V0 – A exp (-l f) then negative and >> e are small for large f (and V is bounded in this region) Who says it took place? What might one hope to learn if so? Start with the picture of how scales evolve during and after inflation; Describe the inflaton-metric system in its original and Mukhanov form; Describe the squeezing of the Mukhanov vacuum into the Bunch-Davies vacuum UniverseNet Inflation

Inflation Who says it took place? What might one hope to learn if so? For example V = V0 - (1/2) m2 f2 then negative, bigger than e are small for small f and m . Who says it took place? What might one hope to learn if so? Start with the picture of how scales evolve during and after inflation; Describe the inflaton-metric system in its original and Mukhanov form; Describe the squeezing of the Mukhanov vacuum into the Bunch-Davies vacuum UniverseNet Inflation

Inflation Who says it took place? What might one hope to learn if so? Start with the picture of how scales evolve during and after inflation; Describe the inflaton-metric system in its original and Mukhanov form; Describe the squeezing of the Mukhanov vacuum into the Bunch-Davies vacuum UniverseNet Inflation

Inflation Who says it took place? What might one hope to learn if so? Mukhanov; Hawking; Linde; Guth & Pi; Steinhardt; … Bonus: besides providing a framework within which primordial seeds of CMB fluctuations can be explained, inflation also provides a mechanism: primordial quantum fluctuations. Who says it took place? What might one hope to learn if so? Start with the picture of how scales evolve during and after inflation; Describe the inflaton-metric system in its original and Mukhanov form; Describe the squeezing of the Mukhanov vacuum into the Bunch-Davies vacuum UniverseNet Inflation

Inflation Who says it took place? What might one hope to learn if so? CMB and large-scale structure sample density correlations Who says it took place? What might one hope to learn if so? Start with the picture of how scales evolve during and after inflation; Describe the inflaton-metric system in its original and Mukhanov form; Describe the squeezing of the Mukhanov vacuum into the Bunch-Davies vacuum UniverseNet Inflation

Inflation Who says it took place? What might one hope to learn if so? Separating primordial from late-time fluctuations primordial part transfer function Who says it took place? What might one hope to learn if so? Start with the picture of how scales evolve during and after inflation; Describe the inflaton-metric system in its original and Mukhanov form; Describe the squeezing of the Mukhanov vacuum into the Bunch-Davies vacuum UniverseNet Inflation

Inflation Who says it took place? What might one hope to learn if so? Separating primordial from late-time fluctuations Who says it took place? What might one hope to learn if so? Start with the picture of how scales evolve during and after inflation; Describe the inflaton-metric system in its original and Mukhanov form; Describe the squeezing of the Mukhanov vacuum into the Bunch-Davies vacuum Structure growth requires k/a > H and the universe is matter dominated. k-4 suppression because modes with k/a = H during rad. dom. must await mat. dom. UniverseNet Inflation

Inflation Who says it took place? What might one hope to learn if so? Evidence is that primordial fluctuations are simple with index and As chosen to ensure Who says it took place? What might one hope to learn if so? Start with the picture of how scales evolve during and after inflation; Describe the inflaton-metric system in its original and Mukhanov form; Describe the squeezing of the Mukhanov vacuum into the Bunch-Davies vacuum UniverseNet Inflation

Inflation Who says it took place? What might one hope to learn if so? ns = 1 is special (Harrison-Zeldovich) d T/T tracks Newtonian potential so with then is scale invariant if ns = 1. Who says it took place? What might one hope to learn if so? Start with the picture of how scales evolve during and after inflation; Describe the inflaton-metric system in its original and Mukhanov form; Describe the squeezing of the Mukhanov vacuum into the Bunch-Davies vacuum UniverseNet Inflation

Inflation Who says it took place? What might one hope to learn if so? Mukhanov; Hawking; Linde; Guth & Pi; Steinhardt; … What is predicted by single-field models? Must propagate initial d f at horizon exit to determine d F at late times, but why should d f be nonzero? Although classical fluctuations are damped during inflation, they are replenished by quantum fluctuations so d f ~ H/2p Who says it took place? What might one hope to learn if so? Start with the picture of how scales evolve during and after inflation; Describe the inflaton-metric system in its original and Mukhanov form; Describe the squeezing of the Mukhanov vacuum into the Bunch-Davies vacuum UniverseNet Inflation

Inflation Who says it took place? What might one hope to learn if so? Can compute linear fluctuations in inflaton and metric and evolve forward using quantum fluctuations as the initial condition at horizon exit. Who says it took place? What might one hope to learn if so? Start with the picture of how scales evolve during and after inflation; Describe the inflaton-metric system in its original and Mukhanov form; Describe the squeezing of the Mukhanov vacuum into the Bunch-Davies vacuum Tensor modes evolve independently. Scalar mixes with Newtonian potential by an amount controlled by df/dt UniverseNet Inflation

Inflation Who says it took place? What might one hope to learn if so? Mukhanov For single field there is a simple integral for modes with k/a < H Who says it took place? What might one hope to learn if so? Start with the picture of how scales evolve during and after inflation; Describe the inflaton-metric system in its original and Mukhanov form; Describe the squeezing of the Mukhanov vacuum into the Bunch-Davies vacuum Primordial fluctuations can be robustly evolved when outside the Hubble scale UniverseNet Inflation

Inflation Who says it took place? What might one hope to learn if so? For two regions with F approximately constant Who says it took place? What might one hope to learn if so? Start with the picture of how scales evolve during and after inflation; Describe the inflaton-metric system in its original and Mukhanov form; Describe the squeezing of the Mukhanov vacuum into the Bunch-Davies vacuum Ff varies inversely with e if initial region is inflating. UniverseNet Inflation

Inflation Who says it took place? What might one hope to learn if so? In this way one finds standard single-field formulae Scalar perturbations Tensor perturbations Who says it took place? What might one hope to learn if so? Start with the picture of how scales evolve during and after inflation; Describe the inflaton-metric system in its original and Mukhanov form; Describe the squeezing of the Mukhanov vacuum into the Bunch-Davies vacuum In principle 3 parameters (H, e, h) give 4 observables. UniverseNet Inflation

Inflation Who says it took place? What might one hope to learn if so? In this way one finds standard single-field formulae Scalar perturbations Tensor perturbations Who says it took place? What might one hope to learn if so? Start with the picture of how scales evolve during and after inflation; Describe the inflaton-metric system in its original and Mukhanov form; Describe the squeezing of the Mukhanov vacuum into the Bunch-Davies vacuum Conventional to define r = QT/QF (= 16 e = -8 nT.) UniverseNet Inflation

Inflation Who says it took place? What might one hope to learn if so? In this way one finds standard single-field formulae Scalar perturbations Tensor perturbations Who says it took place? What might one hope to learn if so? Start with the picture of how scales evolve during and after inflation; Describe the inflaton-metric system in its original and Mukhanov form; Describe the squeezing of the Mukhanov vacuum into the Bunch-Davies vacuum Conventional to define r = QT/QF (= 16 e = -8 nT.) UniverseNet Inflation

Inflation Who says it took place? What might one hope to learn if so? In particular, d T/ T ~ 10-5 implies Start with the picture of how scales evolve during and after inflation; Describe the inflaton-metric system in its original and Mukhanov form; Describe the squeezing of the Mukhanov vacuum into the Bunch-Davies vacuum So if e and h are similar in size then V should be very large relative to other particle physics scales. (Measurement of tensor modes would remove the assumption that e and h are similar Also, large-field models tend to give larger tensor modes UniverseNet Inflation

Inflation Who says it took place? What might one hope to learn if so? The good news: Predictive* and good agreement with observations: Close to HZ spectrum (precisely constant H gives scale invariant result) Gaussian fluctuations (ie <f f f f> not independent of <f f>) because slow roll implies weak inflaton self-couplings Evolution to present relatively model-independent Who says it took place? What might one hope to learn if so? Start with the picture of how scales evolve during and after inflation; Describe the inflaton-metric system in its original and Mukhanov form; Describe the squeezing of the Mukhanov vacuum into the Bunch-Davies vacuum and possibly more if tensor fluctuations are obseved UniverseNet Inflation

Inflation Who says it took place? What might one hope to learn if so? *Less predictive with more complicated models eg: Additional scalar fields: Should there be other light fields besides the inflaton during inflation then there are more than 3 parameters and predictions can change. In particular, z is no longer conserved, so can obtain more complicated post-inflationary evolution. (Can also remain simple, such as if in thermal equilibrium.) Interactions can be stronger, so can obtain observable non-gaussianity. Who says it took place? What might one hope to learn if so? Start with the picture of how scales evolve during and after inflation; Describe the inflaton-metric system in its original and Mukhanov form; Describe the squeezing of the Mukhanov vacuum into the Bunch-Davies vacuum UniverseNet Inflation

Inflation Who says it took place? What might one hope to learn if so? Linde *Less predictive with more complicated models eg: Additional scalar fields: Should there be other light fields besides the inflaton during inflation then more than 3 parameters and predictions can change. In particular, interactions can be stronger and z is no longer conserved, so can obtain observable non-gaussianity. Who says it took place? What might one hope to learn if so? For example: hybrid inflation Start with the picture of how scales evolve during and after inflation; Describe the inflaton-metric system in its original and Mukhanov form; Describe the squeezing of the Mukhanov vacuum into the Bunch-Davies vacuum UniverseNet Inflation

Inflation Who says it took place? What might one hope to learn if so? The bad news: Homogeneous slow roll is usually not generic, and can be sensitive to initial conditions; Very flat potentials have naturalness problems, and inflationary potentials are so flat they are sensitive to ‘planck slop’ (Mp suppressed interactions); Reheating not understood Predictions possible at all? (transplackia, multiverse) Who says it took place? What might one hope to learn if so? Start with the picture of how scales evolve during and after inflation; Describe the inflaton-metric system in its original and Mukhanov form; Describe the squeezing of the Mukhanov vacuum into the Bunch-Davies vacuum UniverseNet Inflation

Inflation Who says it took place? What might one hope to learn if so? Much of the bad news depends on the details of physics at the large energies relevant to the inflationary epoch: Who says it took place? What might one hope to learn if so? Start with the picture of how scales evolve during and after inflation; Describe the inflaton-metric system in its original and Mukhanov form; Describe the squeezing of the Mukhanov vacuum into the Bunch-Davies vacuum If the inflationary scale is so close to the gravity scale, won’t all of the new degrees of freedom at this scale completely change the picture? UniverseNet Inflation

Inflation Who says it took place? What might one hope to learn if so? The bottom line (part I): The great success of standard cosmology relies on relatively special initial conditions Very simple single-field inflationary models provide a simple description of these initial conditions Cosmological measurements provide limited information about very high energy physics Successful cosmologies rely on features that are unusual for physical theories (flat scalar potentials): what does this tell us? Who says it took place? What might one hope to learn if so? Start with the picture of how scales evolve during and after inflation; Describe the inflaton-metric system in its original and Mukhanov form; Describe the squeezing of the Mukhanov vacuum into the Bunch-Davies vacuum UniverseNet Inflation

fin UniverseNet Inflation