Structures in the early Universe. Particle Astrophysics chapter 8 Lecture 4
|
|
- Nickolas Haynes
- 5 years ago
- Views:
Transcription
1 Structures in the early Universe Particle Astrophysics chapter 8 Lecture 4
2 overview Part 1: problems in Standard Model of Cosmology: horizon and flatness problems presence of structures Part : Need for an exponential expansion in the early universe Part 3 : Inflation scenarios scalar inflaton field Part 4 : Primordial fluctuations in inflaton field Part 5 : Growth of density fluctuations during radiation and matter dominated eras Part 6 : CMB observations related to primordial fluctuations Structures in early Universe
3 problems in Standard Model of Cosmology related to initial conditions required: horizon problem flatness problem PART 1: PROBLEMS IN STANDARD COSMOLOGICAL MODEL Structures in early Universe 3
4 01-13 Structures in early Universe 4
5 The ΛCDM cosmological model Concordance model of cosmology in agreement with all observations = Standard Model of Big Bang cosmology ingredients: Universe = homogeneous and isotropic on large scales Universe is expanding with time dependent rate Started from hot Big Bang, followed by short inflation period Is essentially flat over large distances Made up of baryons, cold dark matter and a constant dark energy + small amount of photons and neutrinos Is presently accelerating Lecture Expanding Universe 5
6 The ΛCDM cosmological model Concordance model of cosmology in agreement with all observations = Standard Model of Big Bang cosmology Lecture 1 ingredients: Universe = homogeneous and isotropic on large scales Universe is expanding with time dependent rate Started from hot Big Bang, followed by short inflation period Is essentially Q: Which flat mechanism over large caused distances the exponential inflation? Made up of baryons, cold A: scalar dark matter inflaton and field a constant dark energy + small amount of photons and neutrinos Is Exponential presently accelerating inflation takes care of horizon and flatness problems Parts 1,, Expanding Universe 6
7 The ΛCDM cosmological model Concordance model of cosmology in agreement with all observations = Standard Model of Big Bang cosmology Lecture 1 ingredients: Universe = homogeneous and isotropic on large scales Universe is expanding with time dependent rate Started Structures from hot observed Big Bang, in galaxy followed surveys by short and inflation anisotropies period in CMB Is essentially flat over large distances observations: Made up of baryons, Q: What cold dark seeded matter these and structures? a constant dark energy + small amount A: quantum of photons fluctuations and neutrinos primordial universe Is presently accelerating Parts 4, 5, Expanding Universe 7
8 Horizon in static universe Particle horizon = distance over which one can observe a particle by exchange of a light signal v=c Particle and observer are causally connected In flat universe with k=0 : on very large scale light travels nearly in straight line In a static universe of age t photon emitted at time t=0 would travel t < 14 Gyr STATIC DH Would give as horizon distance today the Hubble radius STATIC H Structures in early Universe 8 ct D t0 ct0 4.Gpc
9 Horizon in expanding universe In expanding universe, particle horizon for observer at t 0 t0 Rt0 DH t0 cdt Lecture 1 0 Rt Expanding, flat, radiation dominated universe Rt Rt 0 Expanding, flat, matter dominated universe Rt 0 expanding, flat, with m =0.4, Λ =0.76 t t t t D t ct H 0 0 Rt D t0 3ct0 H D t 3.3ct H 0 0 ~ 14Gpc Structures in early Universe 9
10 Horizon problem At time of radiation-matter decoupling the particle horizon was much smaller than now Causal connection between photons was only possible within this horizon We expect that there was thermal equilibrium only within this horizon Angle subtented today by horizon size at decoupling is about 1 Why is CMB uniform (up to factor 10-5 ) over much larger angles, i.e. over full sky? Answer : short exponential inflation before decoupling Structures in early Universe 10
11 Horizon at time of decoupling Age of universe at matter-radiation decoupling tdec Optical horizon at decoupling This distance measured today angle subtended today in flat matter dominated universe y z dec 1100 D t ct dec H dec H dec dec D t0 ctdec 1 z dec dec dec H D t ct 1 z 0 dec D t 3c t t H 0 0 dec dec Structures in early Universe 11
12 01-13 Structures in early Universe 1
13 Flatness problem 1 universe is flat today, but was much closer to being flat in early universe How come that curvature was so finely tuned to Ω=1 in very early universe? Friedman equation rewritten t 1 R t kc H t R t t n radiation domination matter domination t t 1~ 1~ t t 3 At time of decoupling At GUT time (10-34 s) 1 ~ 10 1 ~ Structures in early Universe 13
14 01-13 Structures in early Universe 14
15 Flatness problem How could Ω have been so closely tuned to 1 in early universe? Standard Cosmology Model does not contain a mechanisme to explain the extreme flatness The solution is INFLATION Big Bang Planck scale? GUT scale today t s t s Structures in early Universe 15
16 Horizon problem Flatness problem Non-homogenous universe The solution is INFLATION Structures in early Universe 16
17 The need for an exponential expansion in the very early universe PART EXPONENTIAL EXPANSION Structures in early Universe 17
18 Steady state expansion Radiation dominated Described by SM of cosmology Exponential expansion inflation phase Rubakov Structures in early Universe 18
19 Constant energy density & exponential expansion Assume that at Planck scale the energy density is given by a cosmological constant 8 G A constant energy density causes an exponential expansion For instance between t 1 and t in flat universe tot H R 8 R G 3 3 R =e H t -t R Structures in early Universe 19
20 When does inflation happen? Inflation period Structures in early Universe 0
21 When does inflation happen? Grand Unification at GUT energy scale GUT time couplings of Electromagnetic Weak Strong interactions are the same At end of GUT era : spontaneous symmetry breaking into electroweak and strong interactions Next, reheating and production of particles and radiation Start of Big Bang expansion with radiation domination kt GUT t GUT 16 ~10 GeV 34 ~ 10 sec Structures in early Universe 1
22 How much inflation is needed? 1 Calculate backwards size of universe at GUT scale after GUT time universe is dominated by radiation If today R t t 1 R t R t GUT t t GUT R t0 ~ D static H t0 ct0 c 4 10 s ~ 4 10 m 1 Then we expect R t GUT ~ R t On the other hand horizon distance at GUT time was D ~ ~ 10 H s 4 10 s tgut ctgut m EXPECTED R t ~1m Structures in early Universe GUT
23 01-13 Structures in early Universe 3
24 How much inflation is needed? It is postulated that before inflation the universe radius was smaller than the horizon distance at GUT time Size of universe before inflation R1 10 Inflation needs to increase size of universe by factor 6 m R GUT 1m R start inflation 10 m e H t t1 60 R R 1 e H t -t 1 At least 60 e-folds are needed Structures in early Universe 4
25 horizon problem is solved Whole space was in causal contact and thermal equilibrium before inflation Some points got disconnected during exponential expansion entered into our horizon again at later stages horizon problem solved Structures in early Universe 5
26 Scientific American Feb Structures in early Universe 6
27 Flatness problem is solved If curvature term at start of inflation is roughly 1 Then at the end of inflation the curvature R t is even closer to 1 kc H R t kc 1 H R t kc H t 1 1 O 1 R =e 10 1 R at t 10 1 s 1 H t1 -t Structures in early Universe 7
28 Conclusion so far Constant energy density yields exponential expansion This solves horizon and flatness problems What causes the exponential inflation? Structures in early Universe 8
29 Scalar inflaton field PART 3 INFLATION SCENARIOS Structures in early Universe 9
30 Introduce a scalar inflaton field Physical mechanism underlying inflation is unknown Postulate by Guth (1981): inflation is caused by an unstable scalar field present in the very early universe dominates during GUT era (kt GeV) spatially homogeneous depends only on time : (t) inflaton field describes a scalar particle with mass m Dynamics is analogue to ball rolling from hill Scalar has kinetic and potential energy Structures in early Universe 30
31 V(Φ) Chaotic inflation scenario (Linde, 198) Inflation starts at different field values in different locations Inflaton field is displaced from true minimum by some arbitrary mechanism, probably quantum fluctuations Total energy density associated with scalar field 1 c V During inflation the potential V( ) is only slowly varying with slow roll approximation Kinetic energy can be neglected Lineweaver inflation Φ reheating Structures in early Universe 31
32 Slow roll leads to exponential expansion Total energy in universe = potential energy of field c V c ~ V ~ cst Friedman equation for flat universe becomes H H R R 8 c 3 M PL 8 G 3 V H ~ cst Exponential expansion Structures in early Universe 3
33 Reheating at the end of inflation Lagrangian energy of inflaton field 3 L T V R V Mechanics (Euler-Lagrange) : equation of motion of inflaton field dv 3H t 0 d Frictional force due to expansion = oscillator/pendulum motion with damping field oscilllates around minimum stops oscillating = reheating Structures in early Universe 33
34 V(Φ) Reheating and particle creation Inflation ends when field reaches minimum of potential Transformation of potential energy to kinetic energy = reheating Scalar field decays in particles Lineweaver inflation Φ reheating Structures in early Universe 34
35 Summary Planck era When the field reaches the minimum, potential energy is transformed in kinetic energy This is reheating phase Relativistic particles are created Expansion is now radiation dominated Hot Big Bang evolution starts R GUT era Structures in early Universe 35 t kt
36 V(Φ) Chaotic inflation scenario (Linde, 198) Inflation starts at different field values in different locations Inflaton field is displaced from true minimum by some arbitrary mechanism, probably quantum fluctuations Total energy density associated with scalar field 1 c V During inflation the potential V( ) is only slowly varying with slow roll approximation Kinetic energy can be neglected Lineweaver inflation Φ reheating Structures in early Universe 36
37 01-13 Structures in early Universe 37
38 01-13 Structures in early Universe 38
39 Quantum fluctuations in early universe as seed for presentday structures: CMB and galaxies PART 4 PRIMORDIAL FLUCTUATIONS Structures in early Universe 39
40 quantum fluctuations in inflaton field Field starting in B needs more time to reach minimum than field starting in A Potential should vary slowly Reaches minimum Δt later Quantum fluctuations set randomly starting value in A or B Structures in early Universe 40
41 Quantum fluctuations as seed 1 Introduce quantum fluctuations in inflaton field This yields fluctuations in inflation end time Δt Inflation will end at different times in different locations of universe Hence : Fluctuations in kinetic energy at end of inflation Ekin c T t Hence different density of matter at different locations And different temperatures Kinetic Energy Potential Energy Structures in early Universe 41
42 Quantum fluctuations as seed Due to rapid expansion, particles and anti-particles are inflated away from each other One of (anti-)particles moves out of horizon no causal contact with other (anti-)particle no annihilation Energy balance is restored during reheating Fluctuations can be treated as classical perturbations & superposition of waves Structures in early Universe 4
43 Perturbations in the cosmic fluid density fluctuations modify the energy-momentum tensor and therefore also the curvature of space Change in curvature of space-time yields change in gravitation potential Particles and radiation created during reheating will fall in gravitational potential wells These perturbations remain as such till matter-radiation decoupling are imprinted in CMB Structures in early Universe 43 T T ~ 10 5 x
44 Gravitational potential fluctuations gravitational potential Φ due to energy density ρ spherical symmetric case cases G r 3 Global background potential from average field within horizon Potential change due to fluctuation Δρ over arbitrary scale λ r G 3 H Fractional perturbation in gravitational potential at certain location H G Structures in early Universe 44
45 Spectrum of fluctuations During inflation Universe is effectively in stationary state Fluctuation amplitudes will not depend on space and time ~ cst H ~ cst Define rms amplitude of fluctuation rms H 1 Amplitude is independent of horizon size independent of epoch at which it enters horizon is scale-invariant Structures in early Universe 45
46 Clustering of particles at end of inflation Evolution of fluctuations during radiation dominated era Evolution of fluctuations during matter dominated era Damping effects PART 5 GROWTH OF STRUCTURE Structures in early Universe 46
47 Introduction We assume that the structures observed today in the CMB originate from tiny fluctuations in the cosmic fluid during the inflationary phase These perturbations grow in the expanding universe Will the primordial fluctuations of matter density survive the expansion? Structures in early Universe 47
48 Jeans length = critical dimension After reheating matter condensates around primordial density fluctuations universe = gas of relativistic particles x Consider a cloud of gas around fluctuation Δρ When will this lead to condensation? 1 Compare cloud size L to Jeans length λ J J v s G Depends on density and sound speed v s Sound wave in gas = pressure wave Sound velocity in an ideal gas v s P C C p V Structures in early Universe 48
49 Jeans length = critical dimension Compare cloud size L with Jeans length when L << λ J : sound wave travel time < gravitational collaps time no condensation L t v s When L >> λ J : sound cannot travel fast enough from one side to the other cloud condenses around the density perturbations Start of structure formation Structures in early Universe 49
50 Evolution of fluctuations in radiation era After inflation : photons and relativistic particles Radiation dominated till decoupling at z 1100 Velocity of sound is relativistic P c 3 horizon distance ~ Jeans length : no condensation of matter DH t ct v s λj Density fluctuations inside horizon survive fluctuations continue to grow in amplitude as R(t) 5 3 P v s ~ G P v 1 1 ct 3 9 s c Structures in early Universe 50
51 Evolution of fluctuations in matter era After decoupling: dominated by non-relativistic matter Neutral atoms (H) are formed sound velocity drops v s ideal gas 5 P 5 kt 3 3 m v s 5kT c 3M c mat H Jeans length becomes smaller 1 Horizon grows therefore faster gravitational collapse Matter structures can grow J v s G Cold dark matter plays vital role in growth of structures Structures in early Universe 51
52 Damping by photons Fluctuations are most probably adiabatic: baryon and photon densities fluctuate together Photons have nearly light velocity - have higher energy density than baryons and dark matter If time to stream away from denser region of size λ is shorter than life of universe move to regions of low density Result : reduction of density contrast diffusion damping (Silk damping) Structures in early Universe 5
53 Damping by neutrinos Neutrinos = relativistic hot dark matter In early universe: same number of neutrinos as photons Have only weak interactions no interaction with matter as soon as kt below 3 MeV Stream away from denser regions = collisionless damping Velocity close to c : stream up to horizon new perturbations coming into horizon are not able to grow iron out fluctuations Structures in early Universe 53
54 Observations lumpy smooth rms CMB λ (Mpc) Structures in early Universe 54
55 From density contrast to temperature anisotropy Angular power spectrum of anisotropies PART 6 OBSERVATIONS IN CMB Structures in early Universe 55
56 CMB temperature map dipole T 10 T 3 O mk T 5 10 O µk T Contrast enhanced to make 10-5 variations visible! Structures in early Universe 56
57 Small angle anisotropies Adiabatic fluctuations at end of radiation domination : photons & matter fluctuate together Photons keep imprint of density contrast T T Adiab horizon at decoupling is seen now within an angle of 1 temperature correlations at angles < 1 are due to primordial density fluctuations Seen as acoustic peaks in CMB angular power distribution Peaks should all have same amplitude but: Silk damping by photons Structures in early Universe 57
58 1 rms Scientific American Feb 004 x Structures in early Universe 58
59 Angular spectrum of anisotropies 1 CMB map = map of temperatures after subtraction of dipole and galactic emission extra-galactic photons Statistical analysis of the temperature variations in CMB map multipole analysis In given direction n measure difference with average of.7k T n T n T 0 C(θ) = correlation between temperature fluctuations in directions (n,m) separated by angle θ average over all pairs with given θ Structures in early Universe 59
60 Angular spectrum of anisotropies Expand in Legendre polynomials, integrate over C l describes intensity of correlations Temperature fluctuations ΔT are superposition of fluctuations at different scales λ Decompose in spherical harmonics C l T T 0, a lm 1 C l 1 C l Pl cos 4 l l 0 m l a Y lm 1 l 1 lm l m a, lm Structures in early Universe 60
61 Angular spectrum of CMB anisotropies Coefficients C l = angular power spectrum - measure level of structure found at angular separation of Large l means small angles l = 00 corresponds to 1 = horizon at decoupling as seen today Amplitudes seen today depend on: primordial density fluctuations Baryon/photon ratio Amount of dark matter. 00 degrees Fit of C l as function of l yields cosmological parameters Structures in early Universe 61
62 Physics of Young universe Large wavelengths Physics of primordial fluctuations Short wavelengths Silk damping WMAP result 1 = horizon at decoupling Structures in early Universe 6
63 Position and height of peaks Position and heigth of acoustic peaks depend on curvature, matter and energy content and other cosmological parameters Dependence on curvature Flat universe Dependence on baryon content Structures in early Universe 63
64 overview Part 1: problems in Standard Model of Cosmology: horizon and flatness problems presence of structures Part : Need for an exponential expansion in the early universe Part 3 : Inflation scenarios scalar inflaton field Part 4 : Primordial fluctuations in inflaton field Part 5 : Growth of density fluctuations during radiation and matter dominated eras Part 6 : CMB observations related to primordial fluctuations Structures in early Universe 64
65 Examen Book Perkins nd edition chapters 5, 6, 7, 8, + slides Few examples worked out : ex5.1, ex5.3, ex6.1, ex7. Open book examination Structures in early Universe 65
Structures in the early Universe. Particle Astrophysics chapter 8 Lecture 4
Structures in the early Universe Particle Astrophysics chapter 8 Lecture 4 overview problems in Standard Model of Cosmology: horizon and flatness problems presence of structures Need for an exponential
More informationINFLATION. - EARLY EXPONENTIAL PHASE OF GROWTH OF SCALE FACTOR (after T ~ TGUT ~ GeV)
INFLATION - EARLY EXPONENTIAL PHASE OF GROWTH OF SCALE FACTOR (after T ~ TGUT ~ 10 15 GeV) -Phenomenologically similar to Universe with a dominant cosmological constant, however inflation needs to end
More informationThe cosmic background radiation II: The WMAP results. Alexander Schmah
The cosmic background radiation II: The WMAP results Alexander Schmah 27.01.05 General Aspects - WMAP measures temperatue fluctuations of the CMB around 2.726 K - Reason for the temperature fluctuations
More informationCosmology and particle physics
Cosmology and particle physics Lecture notes Timm Wrase Lecture 9 Inflation - part I Having discussed the thermal history of our universe and in particular its evolution at times larger than 10 14 seconds
More informationGalaxies 626. Lecture 3: From the CMBR to the first star
Galaxies 626 Lecture 3: From the CMBR to the first star Galaxies 626 Firstly, some very brief cosmology for background and notation: Summary: Foundations of Cosmology 1. Universe is homogenous and isotropic
More informationThe Growth of Structure Read [CO 30.2] The Simplest Picture of Galaxy Formation and Why It Fails (chapter title from Longair, Galaxy Formation )
WMAP Density fluctuations at t = 79,000 yr he Growth of Structure Read [CO 0.2] 1.0000 1.0001 0.0001 10 4 Early U. contained condensations of many different sizes. Current large-scale structure t = t 0
More informationXIII. The Very Early Universe and Inflation. ASTR378 Cosmology : XIII. The Very Early Universe and Inflation 171
XIII. The Very Early Universe and Inflation ASTR378 Cosmology : XIII. The Very Early Universe and Inflation 171 Problems with the Big Bang The Flatness Problem The Horizon Problem The Monopole (Relic Particle)
More informationConnecting Quarks to the Cosmos
Connecting Quarks to the Cosmos Institute for Nuclear Theory 29 June to 10 July 2009 Inflationary Cosmology II Michael S. Turner Kavli Institute for Cosmological Physics The University of Chicago Michael
More informationLicia Verde. Introduction to cosmology. Lecture 4. Inflation
Licia Verde Introduction to cosmology Lecture 4 Inflation Dividing line We see them like temperature On scales larger than a degree, fluctuations were outside the Hubble horizon at decoupling Potential
More informationAstronomy 182: Origin and Evolution of the Universe
Astronomy 182: Origin and Evolution of the Universe Prof. Josh Frieman Lecture 14 Dec. 2, 2015 Today The Inflationary Universe Origin of Density Perturbations Gravitational Waves Origin and Evolution of
More informationInflation. By The amazing sleeping man, Dan the Man and the Alices
Inflation By The amazing sleeping man, Dan the Man and the Alices AIMS Introduction to basic inflationary cosmology. Solving the rate of expansion equation both analytically and numerically using different
More informationPhysics 133: Extragalactic Astronomy and Cosmology. Week 8
Physics 133: Extragalactic Astronomy and Cosmology Week 8 Outline for Week 8 Primordial Nucleosynthesis Successes of the standard Big Bang model Olbers paradox/age of the Universe Hubble s law CMB Chemical/Physical
More informationIntroduction to Cosmology
Introduction to Cosmology Subir Sarkar CERN Summer training Programme, 22-28 July 2008 Seeing the edge of the Universe: From speculation to science Constructing the Universe: The history of the Universe:
More informationAstr 2320 Thurs. May 7, 2015 Today s Topics Chapter 24: New Cosmology Problems with the Standard Model Cosmic Nucleosynthesis Particle Physics Cosmic
Astr 2320 Thurs. May 7, 2015 Today s Topics Chapter 24: New Cosmology Problems with the Standard Model Cosmic Nucleosynthesis Particle Physics Cosmic Inflation Galaxy Formation 1 Chapter 24: #3 Chapter
More informationLecture 03. The Cosmic Microwave Background
The Cosmic Microwave Background 1 Photons and Charge Remember the lectures on particle physics Photons are the bosons that transmit EM force Charged particles interact by exchanging photons But since they
More informationAnalyzing the CMB Brightness Fluctuations. Position of first peak measures curvature universe is flat
Analyzing the CMB Brightness Fluctuations (predicted) 1 st rarefaction Power = Average ( / ) 2 of clouds of given size scale 1 st compression 2 nd compression (deg) Fourier analyze WMAP image: Measures
More informationModern Cosmology Final Examination Solutions 60 Pts
Modern Cosmology Final Examination Solutions 6 Pts Name:... Matr. Nr.:... February,. Observable Universe [4 Pts] 6 Pt: Complete the plot of Redshift vs Luminosity distance in the range < z < and plot (i)
More informationFrom inflation to the CMB to today s universe. I - How it all begins
From inflation to the CMB to today s universe I - How it all begins Raul Abramo Physics Institute - University of São Paulo abramo@fma.if.usp.br redshift Very brief cosmic history 10 9 200 s BBN 1 MeV
More informationA5682: Introduction to Cosmology Course Notes. 11. CMB Anisotropy
Reading: Chapter 8, sections 8.4 and 8.5 11. CMB Anisotropy Gravitational instability and structure formation Today s universe shows structure on scales from individual galaxies to galaxy groups and clusters
More informationAstro 507 Lecture 28 April 2, 2014
Astro 507 Lecture 28 April 2, 2014 Announcements: PS 5 due now Preflight 6 posted today last PF! 1 Last time: slow-roll inflation scalar field dynamics in an expanding universe slow roll conditions constrain
More informationLecture 12. Inflation. What causes inflation. Horizon problem Flatness problem Monopole problem. Physical Cosmology 2011/2012
Lecture 1 Inflation Horizon problem Flatness problem Monopole problem What causes inflation Physical Cosmology 11/1 Inflation What is inflation good for? Inflation solves 1. horizon problem. flatness problem
More informationPhysical Cosmology 12/5/2017
Physical Cosmology 12/5/2017 Alessandro Melchiorri alessandro.melchiorri@roma1.infn.it slides can be found here: oberon.roma1.infn.it/alessandro/cosmo2017 Structure Formation Until now we have assumed
More informationMASAHIDE YAMAGUCHI. Quantum generation of density perturbations in the early Universe. (Tokyo Institute of Technology)
Quantum generation of density perturbations in the early Universe MASAHIDE YAMAGUCHI (Tokyo Institute of Technology) 03/07/16@Symposium: New Generation Quantum Theory -Particle Physics, Cosmology, and
More informationInflationary Cosmology and Alternatives
Inflationary Cosmology and Alternatives V.A. Rubakov Institute for Nuclear Research of the Russian Academy of Sciences, Moscow and Department of paricle Physics abd Cosmology Physics Faculty Moscow State
More informationCOSMIC INFLATION AND THE REHEATING OF THE UNIVERSE
COSMIC INFLATION AND THE REHEATING OF THE UNIVERSE Francisco Torrentí - IFT/UAM Valencia Students Seminars - December 2014 Contents 1. The Friedmann equations 2. Inflation 2.1. The problems of hot Big
More informationFundamental Particles
Fundamental Particles Standard Model of Particle Physics There are three different kinds of particles. Leptons - there are charged leptons (e -, μ -, τ - ) and uncharged leptons (νe, νμ, ντ) and their
More informationVU lecture Introduction to Particle Physics. Thomas Gajdosik, FI & VU. Big Bang (model)
Big Bang (model) What can be seen / measured? basically only light _ (and a few particles: e ±, p, p, ν x ) in different wave lengths: microwave to γ-rays in different intensities (measured in magnitudes)
More informationThe Concept of Inflation
The Concept of Inflation Introduced by Alan Guth, circa 1980, to provide answers to the following 5 enigmas: 1. horizon problem. How come the cosmic microwave background radiation is so uniform in very
More informationAy1 Lecture 18. The Early Universe and the Cosmic Microwave Background
Ay1 Lecture 18 The Early Universe and the Cosmic Microwave Background 18.1 Basic Ideas, and the Cosmic Microwave background The Key Ideas Pushing backward in time towards the Big Bang, the universe was
More informationGravitation et Cosmologie: le Modèle Standard Cours 8: 6 fevrier 2009
Particules Élémentaires, Gravitation et Cosmologie Année 2008-09 Gravitation et Cosmologie: le Modèle Standard Cours 8: 6 fevrier 2009 Le paradigme inflationnaire Homogeneity and flatness problems in HBB
More informationPhysics 463, Spring 07. Formation and Evolution of Structure: Growth of Inhomogenieties & the Linear Power Spectrum
Physics 463, Spring 07 Lecture 3 Formation and Evolution of Structure: Growth of Inhomogenieties & the Linear Power Spectrum last time: how fluctuations are generated and how the smooth Universe grows
More informationLecture 36: The First Three Minutes Readings: Sections 29-1, 29-2, and 29-4 (29-3)
Lecture 36: The First Three Minutes Readings: Sections 29-1, 29-2, and 29-4 (29-3) Key Ideas Physics of the Early Universe Informed by experimental & theoretical physics Later stages confirmed by observations
More informationCosmology: An Introduction. Eung Jin Chun
Cosmology: An Introduction Eung Jin Chun Cosmology Hot Big Bang + Inflation. Theory of the evolution of the Universe described by General relativity (spacetime) Thermodynamics, Particle/nuclear physics
More informationThe Once and Future CMB
The Once and Future CMB DOE, Jan. 2002 Wayne Hu The On(c)e Ring Original Power Spectra of Maps 64º Band Filtered Ringing in the New Cosmology Gravitational Ringing Potential wells = inflationary seeds
More informationModern Cosmology / Scott Dodelson Contents
Modern Cosmology / Scott Dodelson Contents The Standard Model and Beyond p. 1 The Expanding Universe p. 1 The Hubble Diagram p. 7 Big Bang Nucleosynthesis p. 9 The Cosmic Microwave Background p. 13 Beyond
More informationn=0 l (cos θ) (3) C l a lm 2 (4)
Cosmic Concordance What does the power spectrum of the CMB tell us about the universe? For that matter, what is a power spectrum? In this lecture we will examine the current data and show that we now have
More informationCosmic Inflation Lecture 16 - Monday Mar 10
Physics 224 Spring 2008 Origin and Evolution of the Universe Cosmic Inflation Lecture 16 - Monday Mar 10 Joel Primack University of California, Santa Cruz Outline L15 L16 WMAP 5-year Data and Papers Released
More informationInflation. Week 9. ASTR/PHYS 4080: Introduction to Cosmology
Inflation ASTR/PHYS 4080: Intro to Cosmology Week 9 1 Successes of the Hot Big Bang Model Consists of: General relativity Cosmological principle Known atomic/nuclear/particle physics Explains: dark night
More informationLecture 09. The Cosmic Microwave Background. Part II Features of the Angular Power Spectrum
The Cosmic Microwave Background Part II Features of the Angular Power Spectrum Angular Power Spectrum Recall the angular power spectrum Peak at l=200 corresponds to 1o structure Exactly the horizon distance
More informationAstronomy 182: Origin and Evolution of the Universe
Astronomy 182: Origin and Evolution of the Universe Prof. Josh Frieman Lecture 11 Nov. 13, 2015 Today Cosmic Microwave Background Big Bang Nucleosynthesis Assignments This week: read Hawley and Holcomb,
More informationIntroduction to Inflation
Introduction to Inflation Miguel Campos MPI für Kernphysik & Heidelberg Universität September 23, 2014 Index (Brief) historic background The Cosmological Principle Big-bang puzzles Flatness Horizons Monopoles
More informationCosmic Microwave Background Introduction
Cosmic Microwave Background Introduction Matt Chasse chasse@hawaii.edu Department of Physics University of Hawaii at Manoa Honolulu, HI 96816 Matt Chasse, CMB Intro, May 3, 2005 p. 1/2 Outline CMB, what
More informationLab Monday optional: review for Quiz 3. Lab Tuesday optional: review for Quiz 3.
Announcements SEIs! Quiz 3 Friday. Lab Monday optional: review for Quiz 3. Lab Tuesday optional: review for Quiz 3. Lecture today, Wednesday, next Monday. Final Labs Monday & Tuesday next week. Quiz 3
More informationLecture notes 20: Inflation
Lecture notes 20: Inflation The observed galaxies, quasars and supernovae, as well as observations of intergalactic absorption lines, tell us about the state of the universe during the period where z
More informationCosmology II: The thermal history of the Universe
.. Cosmology II: The thermal history of the Universe Ruth Durrer Département de Physique Théorique et CAP Université de Genève Suisse August 6, 2014 Ruth Durrer (Université de Genève) Cosmology II August
More informationThe Early Universe. 1. Inflation Theory: The early universe expanded enormously in a brief instance in time.
The Early Universe The Early Universe 1. Inflation Theory: The early universe expanded enormously in a brief instance in time. 2. The fundamental forces change during the first second after the big bang.
More informationConcordance Cosmology and Particle Physics. Richard Easther (Yale University)
Concordance Cosmology and Particle Physics Richard Easther (Yale University) Concordance Cosmology The standard model for cosmology Simplest model that fits the data Smallest number of free parameters
More informationCosmology in a nutshell + an argument against
Cosmology in a nutshell + an argument against Ω Λ = based on the inconsistency of the CMB and supernovae results Charles H Lineweaver arxiv:astro-ph/983v Mar 998 University of New South Wales, Sydney,
More informationExtending classical big bang theory
Chapter 21 Extending classical big bang theory The big bang is our standard model for the origin of the Universe and has been for almost half a century. This place in well earned. At a broader conceptual
More informationA5682: Introduction to Cosmology Course Notes. 11. CMB Anisotropy
Reading: Chapter 9, sections 9.4 and 9.5 11. CMB Anisotropy Gravitational instability and structure formation Today s universe shows structure on scales from individual galaxies to galaxy groups and clusters
More informationTriple unification of inflation, dark matter and dark energy
Triple unification of inflation, dark matter and dark energy May 9, 2008 Leonard Susskind, The Anthropic Landscape of String Theory (2003) A. Liddle, A. Ureña-López, Inflation, dark matter and dark energy
More informationAstro-2: History of the Universe
Astro-2: History of the Universe Lecture 11; May 21 2013 Previously on astro-2 In an expanding universe the relationship between redshift and distance depends on the cosmological parameters (i.e. the geometry
More informationA100H Exploring the Universe: Big Bang Theory. Martin D. Weinberg UMass Astronomy
A100H Exploring the : Martin D. Weinberg UMass Astronomy astron100h-mdw@courses.umass.edu April 21, 2016 Read: Chap 23 04/26/16 slide 1 Early Final Exam: Friday 29 Apr at 10:30 am 12:30 pm, here! Emphasizes
More informationInflation. Jo van den Brand, Chris Van Den Broeck, Tjonnie Li Nikhef: April 23, 2010
Inflation Jo van den Brand, Chris Van Den Broeck, Tjonnie Li Nikhef: April 23, 2010 Limitations of standard cosmology Horizon problem, flatness problem, missing exotic particles Horizon: largest distance
More informationLecture 24: Cosmology: The First Three Minutes. Astronomy 111 Monday November 27, 2017
Lecture 24: Cosmology: The First Three Minutes Astronomy 111 Monday November 27, 2017 Reminders Last star party of the semester tomorrow night! Online homework #11 due Monday at 3pm The first three minutes
More informationAST5220 lecture 2 An introduction to the CMB power spectrum. Hans Kristian Eriksen
AST5220 lecture 2 An introduction to the CMB power spectrum Hans Kristian Eriksen Cosmology in ~five slides The basic ideas of Big Bang: 1) The Big Bang model The universe expands today Therefore it must
More informationA873: Cosmology Course Notes. VII. Inflation
Readings VII. Inflation Alan Guth s Inflationary Universe paper (Phys Rev D, Vol. 23, p. 347, 1981) is a classic, well worth reading. The basics are well covered by Ryden, Chapter 11. For more physics
More informationAstronomy 182: Origin and Evolution of the Universe
Astronomy 182: Origin and Evolution of the Universe Prof. Josh Frieman Lecture 13 Nov. 20, 2015 Today Particle Physics & the Early Universe Baryogenesis The Inflationary Scenario Assignments Today: Essay
More informationLarge Scale Structure
Large Scale Structure L2: Theoretical growth of structure Taking inspiration from - Ryden Introduction to Cosmology - Carroll & Ostlie Foundations of Astrophysics Where does structure come from? Initial
More informationAST5220 lecture 2 An introduction to the CMB power spectrum. Hans Kristian Eriksen
AST5220 lecture 2 An introduction to the CMB power spectrum Hans Kristian Eriksen Cosmology in ~five slides The basic ideas of Big Bang: 1) The Big Bang model The universe expands today Therefore it must
More informationLecture 20 Cosmology, Inflation, dark matter
The Nature of the Physical World November 19th, 2008 Lecture 20 Cosmology, Inflation, dark matter Arán García-Bellido 1 News Exam 2: good job! Ready for pick up after class or in my office Average: 74/100
More informationChapter 22 Back to the Beginning of Time
Chapter 22 Back to the Beginning of Time Expansion of Universe implies dense, hot start: Big Bang Back to the Big Bang The early Universe was both dense and hot. Equivalent mass density of radiation (E=mc
More informationThe Early Universe John Peacock ESA Cosmic Vision Paris, Sept 2004
The Early Universe John Peacock ESA Cosmic Vision Paris, Sept 2004 The history of modern cosmology 1917 Static via cosmological constant? (Einstein) 1917 Expansion (Slipher) 1952 Big Bang criticism (Hoyle)
More informationAbout the format of the literature report
About the format of the literature report Minimum 3 pages! Suggested structure: Introduction Main text Discussion Conclusion References Use bracket-number (e.g. [3]) or author-year (e.g. Zackrisson et
More informationGeneral Relativity Lecture 20
General Relativity Lecture 20 1 General relativity General relativity is the classical (not quantum mechanical) theory of gravitation. As the gravitational interaction is a result of the structure of space-time,
More informationPriming the BICEP. Wayne Hu Chicago, March BB
Priming the BICEP 0.05 0.04 0.03 0.02 0.01 0 0.01 BB 0 50 100 150 200 250 300 Wayne Hu Chicago, March 2014 A BICEP Primer How do gravitational waves affect the CMB temperature and polarization spectrum?
More information4 Evolution of density perturbations
Spring term 2014: Dark Matter lecture 3/9 Torsten Bringmann (torsten.bringmann@fys.uio.no) reading: Weinberg, chapters 5-8 4 Evolution of density perturbations 4.1 Statistical description The cosmological
More informationEl Universo en Expansion. Juan García-Bellido Inst. Física Teórica UAM Benasque, 12 Julio 2004
El Universo en Expansion Juan García-Bellido Inst. Física Teórica UAM Benasque, 12 Julio 2004 5 billion years (you are here) Space is Homogeneous and Isotropic General Relativity An Expanding Universe
More informationMass (Energy) in the Universe:
Mass (Energy) in the Universe: smooth (vacuum) clumping Parameters of our Universe present values H = (71±4)km/s/Mpc = 1.0±0.0 m = 0.7±0.0 incl. b = 0.044±0.004 and < 0.014 photons r = 4.9-5 dark energy
More information20 Lecture 20: Cosmic Microwave Background Radiation continued
PHYS 652: Astrophysics 103 20 Lecture 20: Cosmic Microwave Background Radiation continued Innocent light-minded men, who think that astronomy can be learnt by looking at the stars without knowledge of
More informationThe cosmic microwave background radiation
The cosmic microwave background radiation László Dobos Dept. of Physics of Complex Systems dobos@complex.elte.hu É 5.60 May 18, 2018. Origin of the cosmic microwave radiation Photons in the plasma are
More informationisocurvature modes Since there are two degrees of freedom in
isocurvature modes Since there are two degrees of freedom in the matter-radiation perturbation, there must be a second independent perturbation mode to complement the adiabatic solution. This clearly must
More informationReally, really, what universe do we live in?
Really, really, what universe do we live in? Fluctuations in cosmic microwave background Origin Amplitude Spectrum Cosmic variance CMB observations and cosmological parameters COBE, balloons WMAP Parameters
More informationChapter 22 Lecture. The Cosmic Perspective. Seventh Edition. The Birth of the Universe Pearson Education, Inc.
Chapter 22 Lecture The Cosmic Perspective Seventh Edition The Birth of the Universe The Birth of the Universe 22.1 The Big Bang Theory Our goals for learning: What were conditions like in the early universe?
More informationLecture 37 Cosmology [not on exam] January 16b, 2014
1 Lecture 37 Cosmology [not on exam] January 16b, 2014 2 Structure of the Universe Does clustering of galaxies go on forever? Looked at very narrow regions of space to far distances. On large scales the
More informationCosmology. Thermal history of the universe Primordial nucleosynthesis WIMPs as dark matter Recombination Horizon problem Flatness problem Inflation
Cosmology Thermal history of the universe Primordial nucleosynthesis WIMPs as dark matter Recombination Horizon problem Flatness problem Inflation Energy density versus scale factor z=1/a-1 Early times,
More informationi>clicker Quiz #14 Which of the following statements is TRUE?
i>clicker Quiz #14 Which of the following statements is TRUE? A. Hubble s discovery that most distant galaxies are receding from us tells us that we are at the center of the Universe B. The Universe started
More informationComputational Physics and Astrophysics
Cosmological Inflation Kostas Kokkotas University of Tübingen, Germany and Pablo Laguna Georgia Institute of Technology, USA Spring 2012 Our Universe Cosmic Expansion Co-moving coordinates expand at exactly
More informationThe Early Universe: A Journey into the Past
Gravity: Einstein s General Theory of Relativity The Early Universe A Journey into the Past Texas A&M University March 16, 2006 Outline Gravity: Einstein s General Theory of Relativity Galileo and falling
More informationThe Theory of Inflationary Perturbations
The Theory of Inflationary Perturbations Jérôme Martin Institut d Astrophysique de Paris (IAP) Indian Institute of Technology, Chennai 03/02/2012 1 Introduction Outline A brief description of inflation
More informationFinal Exam. String theory. What are these strings? How big are they? Types of strings. String Interactions. Strings can vibrate in different ways
Final Exam Monday, May 8: 2:45-4:45 pm 2241 Chamberlin Note sheet: two double-sided pages Cumulative exam-covers all material, 40 questions 11 questions from exam 1 material 12 questions from exam 2 material
More informationArchaeology of Our Universe YIFU CAI ( 蔡一夫 )
Archaeology of Our Universe YIFU CAI ( 蔡一夫 ) 2013-11-05 Thermal History Primordial era 13.8 billion years by WMAP/NASA Large Scale Structure (LSS) by 2MASS Cosmic Microwave Background (CMB) by ESA/Planck
More informationCMB Anisotropies: The Acoustic Peaks. Boom98 CBI Maxima-1 DASI. l (multipole) Astro 280, Spring 2002 Wayne Hu
CMB Anisotropies: The Acoustic Peaks 80 T (µk) 60 40 20 Boom98 CBI Maxima-1 DASI 500 1000 1500 l (multipole) Astro 280, Spring 2002 Wayne Hu Physical Landscape 100 IAB Sask 80 Viper BAM TOCO Sound Waves
More informationCosmological Structure Formation Dr. Asa Bluck
Cosmological Structure Formation Dr. Asa Bluck Week 6 Structure Formation in the Linear Regime II CMB as Rosetta Stone for Structure Formation Week 7 Observed Scale of the Universe in Space & Time Week
More informationGalaxy Formation Seminar 2: Cosmological Structure Formation as Initial Conditions for Galaxy Formation. Prof. Eric Gawiser
Galaxy Formation Seminar 2: Cosmological Structure Formation as Initial Conditions for Galaxy Formation Prof. Eric Gawiser Cosmic Microwave Background anisotropy and Large-scale structure Cosmic Microwave
More informationSchool Observational Cosmology Angra Terceira Açores 3 rd June Juan García-Bellido Física Teórica UAM Madrid, Spain
School Observational Cosmology Angra Terceira Açores 3 rd June 2014 Juan García-Bellido Física Teórica UAM Madrid, Spain Outline Lecture 1 Shortcomings of the Hot Big Bang The Inflationary Paradigm Homogeneous
More informationTheory of galaxy formation
Theory of galaxy formation Bibliography: Galaxy Formation and Evolution (Mo, van den Bosch, White 2011) Lectures given by Frank van den Bosch in Yale http://www.astro.yale.edu/vdbosch/teaching.html Theory
More informationOutline. Walls, Filaments, Voids. Cosmic epochs. Jeans length I. Jeans length II. Cosmology AS7009, 2008 Lecture 10. λ =
Cosmology AS7009, 2008 Lecture 10 Outline Structure formation Jeans length, Jeans mass Structure formation with and without dark matter Cold versus hot dark matter Dissipation The matter power spectrum
More information3 Observational Cosmology Evolution from the Big Bang Lecture 2
3 Observational Cosmology Evolution from the Big Bang Lecture 2 http://www.sr.bham.ac.uk/~smcgee/obscosmo/ Sean McGee smcgee@star.sr.bham.ac.uk http://www.star.sr.bham.ac.uk/~smcgee/obscosmo Nucleosynthesis
More informationCosmology (Cont.) Lecture 19
Cosmology (Cont.) Lecture 19 1 General relativity General relativity is the classical theory of gravitation, and as the gravitational interaction is due to the structure of space-time, the mathematical
More informationContents. Part I The Big Bang and the Observable Universe
Contents Part I The Big Bang and the Observable Universe 1 A Historical Overview 3 1.1 The Big Cosmic Questions 3 1.2 Origins of Scientific Cosmology 4 1.3 Cosmology Today 7 2 Newton s Universe 13 2.1
More informationThe oldest science? One of the most rapidly evolving fields of modern research. Driven by observations and instruments
The oldest science? One of the most rapidly evolving fields of modern research. Driven by observations and instruments Intersection of physics (fundamental laws) and astronomy (contents of the universe)
More informationThe early and late time acceleration of the Universe
The early and late time acceleration of the Universe Tomo Takahashi (Saga University) March 7, 2016 New Generation Quantum Theory -Particle Physics, Cosmology, and Chemistry- @Kyoto University The early
More informationLecture 12 Cosmology III. Inflation The beginning?
Lecture 12 Cosmology III Inflation The beginning? Unsolved issues in the standard model Horizon problem: Why is the CMB so smooth? The flatness problem: Why is Ω~1? Why is the universe flat? The structure
More informationMODERN COSMOLOGY LECTURE FYTN08
1/43 MODERN COSMOLOGY LECTURE Lund University bijnens@thep.lu.se http://www.thep.lu.se/ bijnens Lecture Updated 2015 2/43 3/43 1 2 Some problems with a simple expanding universe 3 4 5 6 7 8 9 Credit many
More informationCosmological Signatures of a Mirror Twin Higgs
Cosmological Signatures of a Mirror Twin Higgs Zackaria Chacko University of Maryland, College Park Curtin, Geller & Tsai Introduction The Twin Higgs framework is a promising approach to the naturalness
More informationPAPER 71 COSMOLOGY. Attempt THREE questions There are seven questions in total The questions carry equal weight
MATHEMATICAL TRIPOS Part III Friday 31 May 00 9 to 1 PAPER 71 COSMOLOGY Attempt THREE questions There are seven questions in total The questions carry equal weight You may make free use of the information
More informationGravitational waves from the early Universe
Gravitational waves from the early Universe Part 2 Sachiko Kuroyanagi (Nagoya University) 26 Aug 2017 Summer Institute 2017 GWs from inflation Inflation Accelerated expansion in the early Universe Solves
More informationPOST-INFLATIONARY HIGGS RELAXATION AND THE ORIGIN OF MATTER- ANTIMATTER ASYMMETRY
POST-INFLATIONARY HIGGS RELAXATION AND THE ORIGIN OF MATTER- ANTIMATTER ASYMMETRY LOUIS YANG ( 楊智軒 ) UNIVERSITY OF CALIFORNIA, LOS ANGELES (UCLA) DEC 27, 2016 NATIONAL TSING HUA UNIVERSITY OUTLINE Big
More informationWhat is cosmic inflation? A short period of fast expansion, happening very early in the history of the Universe. Outline.
Outline Covers chapters 1 & 11 in Ryden Grand Unification Grand Unification II Gravity? Theory of Everything? Strong force Weak force EM t Planck : ~1-43 s t GUT : ~1-36 s t EW : ~1-12 s t Phase Transitions
More information