Early & Late Inflation Theory

Slides:



Advertisements
Similar presentations
Observational constraints on primordial perturbations Antony Lewis CITA, Toronto
Advertisements

Cosmological Parameters and the WMAP data Antony Lewis CfA, Harvard / CITA, Toronto Standard assumptions – what are the parameters?
Observational constraints and cosmological parameters
Primordial perturbations and precision cosmology from the Cosmic Microwave Background Antony Lewis CITA, University of Toronto
CMB Constraints on Cosmology Antony Lewis Institute of Astronomy, Cambridge
Science with Future CMB Observations Lloyd Knox UC Davis.
Dick Bond Constraining Inflation Trajectories, now & then.
Constraining Inflation Histories with the CMB & Large Scale Structure Dynamical & Resolution Trajectories for Inflation then & now Dick Bond.
Large Primordial Non- Gaussianity from early Universe Kazuya Koyama University of Portsmouth.
Planck 2013 results, implications for cosmology
Parameterizing Dark Energy Z. Huang, R. J. Bond, L. Kofman Canadian Institute of Theoretical Astrophysics.
Phenomenological Classification of Inflationary Potentials Katie Mack (Princeton University) with George Efstathiou (Cambridge University) Efstathiou &
Non-linear matter power spectrum to 1% accuracy between dynamical dark energy models Matt Francis University of Sydney Geraint Lewis (University of Sydney)
COSMOLOGY AS A TOOL FOR PARTICLE PHYSICS Roberto Trotta University of Oxford Astrophysics & Royal Astronomical Society.
Is the Universe homogeneous and isotropic? Marc Kamionkowski (Caltech) Tsvi-fest, 17 December 2009 Statistically.
Component Separation of Polarized Data Application to PLANCK Jonathan Aumont J-F. Macías-Pérez, M. Tristram, D. Santos
Complementary Probes ofDark Energy Complementary Probes of Dark Energy Eric Linder Berkeley Lab.
High Resolution Observations of the CMB with the CBI Interferometer XVIII th IAP Colloquium - July Carlo Contaldi CITA.
Scanning Inflation and Reheating Bottom-up approach to inflation: reconstruction of acceleration trajectories Top-down approach to inflation: seeks to.
NEUTRINO MASS FROM LARGE SCALE STRUCTURE STEEN HANNESTAD CERN, 8 December 2008 e    
The CMB and Neutrinos. We can all measure the CMB T CMB = \ K CMB approx 1% of TV noise! 400 photons/cc at 0.28 eV/cc.
Modern State of Cosmology V.N. Lukash Astro Space Centre of Lebedev Physics Institute Cherenkov Conference-2004.
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/ )
The Cosmic Web & the CMB high resolution frontier Dick Bond Primary CMB anisotropies are strongly damped by photon-baryon shear viscosity at high L > 1000.
Towards inflation and dark energy cosmologies in string generated gravity models Ishwaree Neupane University of Canterbury March 1, th Rencontres.
Cosmology and String Theory F. Quevedo Cambridge CORFU 2005.
US Planck Data Analysis Review 1 Lloyd KnoxUS Planck Data Analysis Review 9–10 May 2006 The Science Potential of Planck Lloyd Knox (UC Davis)
CMB observations and results Dmitry Pogosyan University of Alberta Lake Louise, February, 2003 Lecture 1: What can Cosmic Microwave Background tell us.
1 1 Eric Linder University of California, Berkeley Lawrence Berkeley National Lab Interpreting Dark Energy JDEM constraints.
Making and Probing Inflation Lev Kofman KITPC Beijing November Making Inflation in String Theory How small can be r Gravity Waves from Preheating.
Clustering in the Sloan Digital Sky Survey Bob Nichol (ICG, Portsmouth) Many SDSS Colleagues.
Surveying Inflation and Reheating Cosmological Landscape: Strings, Gravity and Inflation Seoul, September 2005 “K. listened intently. So the Castle had.
Probing inflation with CMB anisotropies Zong-Kuan Guo (ITP, CAS) ICFPC 2012 (Weihai) August 12, 2012.
MATTEO VIEL THE LYMAN-  FOREST AS A COSMOLOGICAL PROBE Contents and structures of the Universe – La Thuile (ITALY), 19 March 2006.
CMB as a dark energy probe Carlo Baccigalupi. Outline  Fighting against a cosmological constant  Parametrizing cosmic acceleration  The CMB role in.
Observational constraints and cosmological parameters Antony Lewis Institute of Astronomy, Cambridge
Dick Bond Inflation Then  k  =(1+q)(a) ~r/16 0<   = multi-parameter expansion in ( ln Ha ~ lnk) ~ 10 good e-folds in a (k~10 -4 Mpc -1 to ~ 1 Mpc.
BBN: Constraints from CMB experiments Joanna Dunkley University of Oxford IAUS Geneva, Nov
The Planck Satellite Hannu Kurki-Suonio University of Helsinki Finnish-Japanese Workshop on Particle Cosmology, Helsinki
Testing the slow roll inflation paradigm with the Big Bang Observer
Adventures in Parameter Estimation Jason Dick University of California, Davis.
Inflation and Branes Bottom-up approach to inflation: reconstruction of acceleration trajectories Top-down approach to inflation: seeks to embed it in.
Observational constraints on inflationary models Zong-Kuan Guo (ITP, CAS) CosPA2011 (Peking Uni) October 31, 2011.
Dynamical & Resolution Trajectories for Inflation then & now Dick Bond Inflation Now 1+w(a)=  f(a/a  eq ) to 3 (1+q)/2 ~ 1 good e-fold. Only ~2 parameters.
Unesco July 2005Francis Bernardeau SPhT Saclay1 Models of inflation with primordial non-Gaussianities Francis Bernardeau SPhT Saclay Collaboration with.
1 1 Dark Energy with SNAP and other Next Generation Probes Eric Linder Berkeley Lab.
Trajectories Bond, Contaldi, Frolov, Kofman, Souradeep, Vaudrevange 05.
CMB, lensing, and non-Gaussianities
Constraining Inflation Trajectories with the CMB & Large Scale Structure Dick Bond Dynamical & Resolution Trajectories/Histories, for Inflation then &
2-year Total Intensity Observations year Polarization Observations Cosmic Background Imager Tony Readhead Zeldovich celebration.
Dynamical Trajectories for Inflation now & then Dick Bond Inflation Now 1+ w (a)=  s f(a/a  eq ; a s /a  eq ) goes to  a  x3/2 = 3 (1+q)/2 ~1 good.
CMB physics Zong-Kuan Guo 《现代宇宙学》
Bond, Boyle, Kofman, Prokushkin, Vaudrevange
Testing Primordial non-Gaussianities in CMB Anisotropies
Cosmological Sources of Stochastic Gravitational-Wave Background
Supporting Observations TPX – dust Polarized Sources
Kähler Moduli Inflation
Inflation Then k=(1+q)(a) ~r/16 0<
The Cosmic Microwave Background and the WMAP satellite results
Inflation with a Gauss-Bonnet coupling
WMAP 3-year constraints on the inflationary expansion
宇宙微波背景辐射与早期宇宙物理 郭宗宽(中科院理论物理研究所) 南开大学物理学院 2012年3月16日.
Features in the primordial power spectrum:
Precision cosmology, status and perspectives
Inflation and the cosmological density perturbation
General, single field Inflation
暴涨模型及观测检验 郭宗宽 中科院理论物理所 中国科技大学交叉学科理论研究中心 2011年6月30日.
Measurements of Cosmological Parameters
“B-mode from space” workshop,
6-band Survey: ugrizy 320–1050 nm
Presentation transcript:

Early & Late Inflation Theory cf. CMB+LSS @ CITA Concordance (pre-WMAP2++) & discordant notes. The “basic parameters”: LCDM with power law index and no/little GW is concordant. Some discord .. always. Extension to larger parameter lists. Are current discordant notes statistically significant, systematics, astrophysics, fundamental physics? Add parameters: theory priors – cost function, baroqueness, taste? r_ts (<.72/<.36??), k_BSI, dn_s/dlnk, size_U/chi_U, subdominant (isoc/adiab), z_reh (+VMOs?) {e.g. Vaudrevange, Lewis, McDonald @ CITA/PI focus gp; soon Nolta WMAP2} Resolving (or celebrating) discord with planned experiments. break degeneracies of cosmic parameters planned CMB+ext, with ext= z-surveys, cl-gp surveys (Sunyaev-Zeldovich/Opt/X/weaklens), weak lensing LSS surveys, SN CMB High-L frontier TT: near term, cbipol, boom2Kpol, acbar forecasts. Long term Apex, ACT, SPT, Quiet forecasts. CMB Polarization EE/BB, High & Low-L: CBI, BOOM2K , DASI, CAPMap, WMAP2, BICEP, QUaD, Polarbear, QUIET, AMiBA, Planck, … CMBpol

Anomalies: Systematics, Statistics, AstroPhysics or Fundamental Physics? “anomalies” @ low L 2,3; ~20-30; check@200, > 600? ET checkmarks 2, 22, 222, 2222 Issues: L=2,3 how low is the probability? Glitches? non-WMAP data e.g. Acbar/CBI calibration CBI anomalous power @ L > 2000, Sunyaev Zeldovich effect in the cosmic web is plausible if s8 if ~ 0.9 (nonlinear gasdynamics) Statistical isotropy broken on large scales?

uniform-acceleration Jan04 CMB data cf. good-fit LCDM uniform-acceleration model

String Theory Landscape @ Stanford Perhaps 10 different vacua 100

single field inflation vs. WMAP1+ext+ext WMAP1 Peiris et al. 2003 Each point is a “viable slow-roll” model, able to sustain inflation for sufficient e-foldings to solve the horizon problem and make the Universe (nearly) flat BUT highly restricted. Monte Carlo simulations using “flow-equations” (Kinney 2002). slow-roll priors are artificial, highly restrictive & misleading about allowed inflationary phase space. Equivalent to a power series expansion of order 5, 6, 8 of histories. CITA approach: efficiently sampled inflation acceleration histories (trajectories). Physics priors: NONE - all are allowed (constrain by taste, e.g. allowed bumpiness). Only data can decide, includes very weak “priors” like “anthropic data” as well as high precision CMB+LSS. Monte Carlo simulation of acceleration histories Don’t interpret points statistically! Each point has equal weight Not every point coincides with a physically realistic model Monte Carlo realizations of inflationary flow equations

Potential of the Hybrid D3/D7 Inflation Model String Theory Landscape & Inflation++ Phenomenology for CMB+LSS running index as simplest breaking (back to early 80s), radically broken scale invariance, 2+-field inflation, isocurvatures, Cosmic strings/defects, compactification & topology, & other baroque add-ons. subdominant String/Mtheory-motivated, extra dimensions, brane-ology, reflowering of inflaton/isocon models (includes curvaton), modified kinetic energies, k-essence, Dirac-Born-Infeld [sqrt(1-momentum**2), “DBI in the Sky” Silverstein etal 2004], etc. KKLT, KKLMMT any acceleration trajectory will do?? q (ln Ha) H(phi,…) V(phi,…) Measure?? anti-baroque prior 14 std inflation parameters + many many more e.g. “blind” search for patterns in the primordial power spectrum Potential of the Hybrid D3/D7 Inflation Model

Running of the Spectral Index : Parameter Fits [Tegmark et al. astro-ph/0310723] [Spergel et al. ApJS, 148, 175] [Bond, Contaldi & Pogosyan astro-ph/0310735] [CBI VII, Readhead et al. astro-ph/0402359] CMB + weak lens s8 CMB data only [dns/dlnk] <0 in Jan03, Mar03 & Mar04

PLANCK vs. WMAP4yr + Ground based telescopes (circa ~ 2008) WMAP 4yr + Ground-based telescopes pre-Planck ACT/SPT-like (bolometers) ; QUIET (HEMT arrays). Coverage assumed; ~few % of the sky (1000 sq deg); polarization included PLANCK (2007+)

END

Systematic error budget? .. McDonald etal, Haehnelt etal No running: dn/dlnk~0 Damped Lyman alpha system effect at small scales + increased WMAP errors at large scales of Slosar & Seljak 04 Systematic error budget? .. McDonald etal, Haehnelt etal

B+Contaldi+Kofman+Souradeep+Vaudrevange+ acceleration trajectories, “featured” potentials, expansions about uniform q(T) (aka slow-roll-ology in the Hamilton-Jacobi/stochastic inflation formulation – works OK), … & the nonlocal WKB++ approximation (Habib etal 02,04) B+Contaldi+Kofman+Souradeep+Vaudrevange+