The Universe; the Whole Shebang
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Inflationary Cosmology: from Theory to Observations
Inflationary Cosmology: From Theory to Observations J. Alberto V´azquez1, 2, Luis, E. Padilla2, and Tonatiuh Matos2 1Instituto de Ciencias F´ısicas,Universidad Nacional Aut´onomade Mexico, Apdo. Postal 48-3, 62251 Cuernavaca, Morelos, M´exico. 2Departamento de F´ısica,Centro de Investigaci´ony de Estudios Avanzados del IPN, M´exico. February 10, 2020 Abstract The main aim of this paper is to provide a qualitative introduction to the cosmological inflation theory and its relationship with current cosmological observations. The inflationary model solves many of the fundamental problems that challenge the Standard Big Bang cosmology, such as the Flatness, Horizon, and the magnetic Monopole problems. Additionally, it provides an explanation for the initial conditions observed throughout the Large-Scale Structure of the Universe, such as galaxies. In this review, we describe general solutions to the problems in the Big Bang cosmology carry out by a single scalar field. Then, with the use of current surveys, we show the constraints imposed on the inflationary parameters (ns; r), which allow us to make the connection between theoretical and observational cosmology. In this way, with the latest results, it is possible to select, or at least to constrain, the right inflationary model, parameterized by a single scalar field potential V (φ). Abstract El objetivo principal de este art´ıculoes ofrecer una introducci´oncualitativa a la teor´ıade la inflaci´onc´osmica y su relaci´oncon observaciones actuales. El modelo inflacionario resuelve algunos problemas fundamentales que desaf´ıanal modelo est´andarcosmol´ogico,denominado modelo del Big Bang caliente, como el problema de la Planicidad, el Horizonte y la inexistencia de Monopolos magn´eticos.Adicionalmente, provee una explicaci´onal origen de la estructura a gran escala del Universo, como son las galaxias. -
The Matter – Antimatter Asymmetry of the Universe and Baryogenesis
The matter – antimatter asymmetry of the universe and baryogenesis Andrew Long Lecture for KICP Cosmology Class Feb 16, 2017 Baryogenesis Reviews in General • Kolb & Wolfram’s Baryon Number Genera.on in the Early Universe (1979) • Rio5o's Theories of Baryogenesis [hep-ph/9807454]} (emphasis on GUT-BG and EW-BG) • Rio5o & Trodden's Recent Progress in Baryogenesis [hep-ph/9901362] (touches on EWBG, GUTBG, and ADBG) • Dine & Kusenko The Origin of the Ma?er-An.ma?er Asymmetry [hep-ph/ 0303065] (emphasis on Affleck-Dine BG) • Cline's Baryogenesis [hep-ph/0609145] (emphasis on EW-BG; cartoons!) Leptogenesis Reviews • Buchmuller, Di Bari, & Plumacher’s Leptogenesis for PeDestrians, [hep-ph/ 0401240] • Buchmulcer, Peccei, & Yanagida's Leptogenesis as the Origin of Ma?er, [hep-ph/ 0502169] Electroweak Baryogenesis Reviews • Cohen, Kaplan, & Nelson's Progress in Electroweak Baryogenesis, [hep-ph/ 9302210] • Trodden's Electroweak Baryogenesis, [hep-ph/9803479] • Petropoulos's Baryogenesis at the Electroweak Phase Transi.on, [hep-ph/ 0304275] • Morrissey & Ramsey-Musolf Electroweak Baryogenesis, [hep-ph/1206.2942] • Konstandin's Quantum Transport anD Electroweak Baryogenesis, [hep-ph/ 1302.6713] Constituents of the Universe formaon of large scale structure (galaxy clusters) stars, planets, dust, people late ame accelerated expansion Image stolen from the Planck website What does “ordinary matter” refer to? Let’s break it down to elementary particles & compare number densities … electron equal, universe is neutral proton x10 billion 3⇣(3) 3 3 n =3 T 168 cm− neutron x7 ⌫ ⇥ 4⇡2 ⌫ ' matter neutrinos photon positron =0 2⇣(3) 3 3 n = T 413 cm− γ ⇡2 CMB ' anti-proton =0 3⇣(3) 3 3 anti-neutron =0 n =3 T 168 cm− ⌫¯ ⇥ 4⇡2 ⌫ ' anti-neutrinos antimatter What is antimatter? First predicted by Dirac (1928). -
Phy306 Introduction to Cosmology Homework 3 Notes
PHY306 INTRODUCTION TO COSMOLOGY HOMEWORK 3 NOTES 1. Show that, for a universe which is not flat, 1 − Ω 1 − Ω = , where Ω = Ω r + Ω m + Ω Λ and the subscript 0 refers to the present time. [2] This was generally quite well done, although rather lacking in explanation. You should really define the Ωs, and you need to explain that you divide the expression for t by that for t0. 2. Suppose that inflation takes place around 10 −35 s after the Big Bang. Assume the following simplified properties of the universe: ● it is matter dominated from the end of inflation to the present day; ● at the present day 0.9 ≤ Ω ≤ 1.1; ● the universe is currently 10 10 years old; ● inflation is driven by a cosmological constant. Using these assumptions, calculate the minimum amount of inflation needed to resolve the flatness problem, and hence determine the value of the cosmological constant required if the inflation period ends at t = 10 −34 s. [4] This was not well done at all, although it is not really a complicated calculation. I think the principal problem was that people simply did not think it through—not only do you not explain what you’re doing to the marker, you frequently don’t explain it to yourself! Some people therefore got hopelessly confused between the two time periods involved—the matter-dominated epoch from 10 −34 s to 10 10 years, and the inflationary period from 10 −35 to 10 −34 s. The most common error—in fact, considerably more common than the right answer—was simply assuming that during the post-inflationary epoch 1 − . -
Scalar Correlation Functions in De Sitter Space from the Stochastic Spectral Expansion
IMPERIAL/TP/2019/TM/03 Scalar correlation functions in de Sitter space from the stochastic spectral expansion Tommi Markkanena;b , Arttu Rajantiea , Stephen Stopyrac and Tommi Tenkanend aDepartment of Physics, Imperial College London, Blackett Laboratory, London, SW7 2AZ, United Kingdom bLaboratory of High Energy and Computational Physics, National Institute of Chemical Physics and Biophysics, R¨avala pst. 10, Tallinn, 10143, Estonia cDepartment of Physics and Astronomy, UCL, Gower Street, London WC1E 6BT, United Kingdom dDepartment of Physics and Astronomy, Johns Hopkins University, Baltimore, MD 21218, United States of America E-mail: [email protected], tommi.markkanen@kbfi.ee, [email protected], [email protected], [email protected] Abstract. We consider light scalar fields during inflation and show how the stochastic spec- tral expansion method can be used to calculate two-point correlation functions of an arbitrary local function of the field in de Sitter space. In particular, we use this approach for a massive scalar field with quartic self-interactions to calculate the fluctuation spectrum of the density contrast and compare it to other approximations. We find that neither Gaussian nor linear arXiv:1904.11917v2 [gr-qc] 1 Aug 2019 approximations accurately reproduce the power spectrum, and in fact always overestimate it. For example, for a scalar field with only a quartic term in the potential, V = λφ4=4, we find a blue spectrum with spectral index n 1 = 0:579pλ. − Contents 1 Introduction1 2 The stochastic approach2 2.1 -
The High Redshift Universe: Galaxies and the Intergalactic Medium
The High Redshift Universe: Galaxies and the Intergalactic Medium Koki Kakiichi M¨unchen2016 The High Redshift Universe: Galaxies and the Intergalactic Medium Koki Kakiichi Dissertation an der Fakult¨atf¨urPhysik der Ludwig{Maximilians{Universit¨at M¨unchen vorgelegt von Koki Kakiichi aus Komono, Mie, Japan M¨unchen, den 15 Juni 2016 Erstgutachter: Prof. Dr. Simon White Zweitgutachter: Prof. Dr. Jochen Weller Tag der m¨undlichen Pr¨ufung:Juli 2016 Contents Summary xiii 1 Extragalactic Astrophysics and Cosmology 1 1.1 Prologue . 1 1.2 Briefly Story about Reionization . 3 1.3 Foundation of Observational Cosmology . 3 1.4 Hierarchical Structure Formation . 5 1.5 Cosmological probes . 8 1.5.1 H0 measurement and the extragalactic distance scale . 8 1.5.2 Cosmic Microwave Background (CMB) . 10 1.5.3 Large-Scale Structure: galaxy surveys and Lyα forests . 11 1.6 Astrophysics of Galaxies and the IGM . 13 1.6.1 Physical processes in galaxies . 14 1.6.2 Physical processes in the IGM . 17 1.6.3 Radiation Hydrodynamics of Galaxies and the IGM . 20 1.7 Bridging theory and observations . 23 1.8 Observations of the High-Redshift Universe . 23 1.8.1 General demographics of galaxies . 23 1.8.2 Lyman-break galaxies, Lyα emitters, Lyα emitting galaxies . 26 1.8.3 Luminosity functions of LBGs and LAEs . 26 1.8.4 Lyα emission and absorption in LBGs: the physical state of high-z star forming galaxies . 27 1.8.5 Clustering properties of LBGs and LAEs: host dark matter haloes and galaxy environment . 30 1.8.6 Circum-/intergalactic gas environment of LBGs and LAEs . -
Outline of Lecture 2 Baryon Asymmetry of the Universe. What's
Outline of Lecture 2 Baryon asymmetry of the Universe. What’s the problem? Electroweak baryogenesis. Electroweak baryon number violation Electroweak transition What can make electroweak mechanism work? Dark energy Baryon asymmetry of the Universe There is matter and no antimatter in the present Universe. Baryon-to-photon ratio, almost constant in time: nB 10 ηB = 6 10− ≡ nγ · Baryon-to-entropy, constant in time: n /s = 0.9 10 10 B · − What’s the problem? Early Universe (T > 1012 K = 100 MeV): creation and annihilation of quark-antiquark pairs ⇒ n ,n n q q¯ ≈ γ Hence nq nq¯ 9 − 10− nq + nq¯ ∼ How was this excess generated in the course of the cosmological evolution? Sakharov conditions To generate baryon asymmetry, three necessary conditions should be met at the same cosmological epoch: B-violation C-andCP-violation Thermal inequilibrium NB. Reservation: L-violation with B-conservation at T 100 GeV would do as well = Leptogenesis. & ⇒ Can baryon asymmetry be due to electroweak physics? Baryon number is violated in electroweak interactions. Non-perturbative effect Hint: triangle anomaly in baryonic current Bµ : 2 µ 1 gW µνλρ a a ∂ B = 3colors 3generations ε F F µ 3 · · · 32π2 µν λρ ! "Bq a Fµν: SU(2)W field strength; gW : SU(2)W coupling Likewise, each leptonic current (n = e, µ,τ) g2 ∂ Lµ = W ε µνλρFa Fa µ n 32π2 · µν λρ a 1 Large field fluctuations, Fµν ∝ gW− may have g2 Q d3xdt W ε µνλρFa Fa = 0 ≡ 32 2 · µν λρ ' # π Then B B = d3xdt ∂ Bµ =3Q fin− in µ # Likewise L L =Q n, fin− n, in B is violated, B L is not. -
AST4220: Cosmology I
AST4220: Cosmology I Øystein Elgarøy 2 Contents 1 Cosmological models 1 1.1 Special relativity: space and time as a unity . 1 1.2 Curvedspacetime......................... 3 1.3 Curved spaces: the surface of a sphere . 4 1.4 The Robertson-Walker line element . 6 1.5 Redshifts and cosmological distances . 9 1.5.1 Thecosmicredshift . 9 1.5.2 Properdistance. 11 1.5.3 The luminosity distance . 13 1.5.4 The angular diameter distance . 14 1.5.5 The comoving coordinate r ............... 15 1.6 TheFriedmannequations . 15 1.6.1 Timetomemorize! . 20 1.7 Equationsofstate ........................ 21 1.7.1 Dust: non-relativistic matter . 21 1.7.2 Radiation: relativistic matter . 22 1.8 The evolution of the energy density . 22 1.9 The cosmological constant . 24 1.10 Some classic cosmological models . 26 1.10.1 Spatially flat, dust- or radiation-only models . 27 1.10.2 Spatially flat, empty universe with a cosmological con- stant............................ 29 1.10.3 Open and closed dust models with no cosmological constant.......................... 31 1.10.4 Models with more than one component . 34 1.10.5 Models with matter and radiation . 35 1.10.6 TheflatΛCDMmodel. 37 1.10.7 Models with matter, curvature and a cosmological con- stant............................ 40 1.11Horizons.............................. 42 1.11.1 Theeventhorizon . 44 1.11.2 Theparticlehorizon . 45 1.11.3 Examples ......................... 46 I II CONTENTS 1.12 The Steady State model . 48 1.13 Some observable quantities and how to calculate them . 50 1.14 Closingcomments . 52 1.15Exercises ............................. 53 2 The early, hot universe 61 2.1 Radiation temperature in the early universe . -
What Did the Early Universe Look Like? Key Stage 5
1 What did the early Universe look like? Key Stage 5 Topics covered: Cosmic Microwave Background Radiation, Wien’s displacement law, Doppler Effect Watch the video “What makes the Universe colourful?” https://vimeo.com/213990458 Scientists theorise that the Universe began with the Big Bang around 13.8 billion years ago. Space has been expanding ever since and the initial Big Bang energy has spread out. As a result the temperature of the Universe has fallen and the wavelength of light has stretched out. The history of the Universe can be split into different epochs – see the handout ‘TIMELINE OF THE UNIVERSE’. If we treat the Universe as a black body* then we can work out the peak wavelength of light travelling through the Universe at different epochs by using Wien’s law: 2.898 × 10−3 휆 = 푚푎푥 푇 휆푚푎푥 – peak wavelength emitted by the black body (m - metres) 푇 – temperature of the black body (K – Kelvin) * A black body is an ideal case of an object or system which perfectly absorbs and emits radiation and light and does not reflect any of it. 2 1. Use the ‘TIMELINE OF THE UNIVERSE’ handout to help. For each of the following epochs: 350,000 years (t1 - near the end of the photon epoch) 380,000 years (t2 - at recombination) 13.8 billion years (t3 - present day) a) Complete the table below to work out the peak wavelength (휆푚푎푥) of light that would be travelling through the Universe at that time. epoch Temperature Peak wavelength t1 350,000 years t2 380,000 years t3 13.8 billion years b) Mark these three wavelengths (as vertical lines / arrows) on the diagram below as t1, t2 and t3. -
Big Bang Nucleosynthesis Finally, Relative Abundances Are Sensitive to Density of Normal (Baryonic Matter)
Big Bang Nucleosynthesis Finally, relative abundances are sensitive to density of normal (baryonic matter) Thus Ωb,0 ~ 4%. So our universe Ωtotal ~1 with 70% in Dark Energy, 30% in matter but only 4% baryonic! Case for the Hot Big Bang • The Cosmic Microwave Background has an isotropic blackbody spectrum – it is extremely difficult to generate a blackbody background in other models • The observed abundances of the light isotopes are reasonably consistent with predictions – again, a hot initial state is the natural way to generate these • Many astrophysical populations (e.g. quasars) show strong evolution with redshift – this certainly argues against any Steady State models The Accelerating Universe Distant SNe appear too faint, must be further away than in a non-accelerating universe. Perlmutter et al. 2003 Riese 2000 Outstanding problems • Why is the CMB so isotropic? – horizon distance at last scattering << horizon distance now – why would causally disconnected regions have the same temperature to 1 part in 105? • Why is universe so flat? – if Ω is not 1, Ω evolves rapidly away from 1 in radiation or matter dominated universe – but CMB analysis shows Ω = 1 to high accuracy – so either Ω=1 (why?) or Ω is fine tuned to very nearly 1 • How do structures form? – if early universe is so very nearly uniform Astronomy 422 Lecture 22: Early Universe Key concepts: Problems with Hot Big Bang Inflation Announcements: April 26: Exam 3 April 28: Presentations begin Astro 422 Presentations: Thursday April 28: 9:30 – 9:50 _Isaiah Santistevan__________ 9:50 – 10:10 _Cameron Trapp____________ 10:10 – 10:30 _Jessica Lopez____________ Tuesday May 3: 9:30 – 9:50 __Chris Quintana____________ 9:50 – 10:10 __Austin Vaitkus___________ 10:10 – 10:30 __Kathryn Jackson__________ Thursday May 5: 9:30 – 9:50 _Montie Avery_______________ 9:50 – 10:10 _Andrea Tallbrother_________ 10:10 – 10:30 _Veronica Dike_____________ 10:30 – 10:50 _Kirtus Leyba________________________ Send me your preference. -
Cosmology and Dark Matter Lecture 3
1 Cosmology and Dark Matter V.A. Rubakov Lecture 3 2 Outline of Lecture 3 Baryon asymmetry of the Universe Generalities. Electroweak baryon number non-conservation What can make electroweak mechanism work? Leptogenesis and neutrino masses Before the hot epoch 3 Baryon asymmetry of the Universe There is matter and no antimatter in the present Universe. Baryon-to-photon ratio, almost constant in time: nB 10 ηB = 6 10− ≡ nγ · 10 Baryon-to-entropy, constant in time: nB/s = 0.9 10 · − What’s the problem? Early Universe (T > 1012 K = 100 MeV): creation and annihilation of quark-antiquark pairs nq,nq¯ nγ Hence ⇒ ≈ nq nq¯ 9 − 10− nq + nq¯ ∼ Very unlikely that this excess is initial condition. Certainly not, if inflation. How was this excess generated in the course of the cosmological evolution? Sakharov’67, Kuzmin’70 4 Sakharov conditions To generate baryon asymmetry from symmetric initial state, three necessary conditions should be met at the same cosmological epoch: B-violation C- and CP-violation Thermal inequilibrium NB. Reservation: L-violation with B-conservation at T 100 GeV would do as well = Leptogenesis. ≫ ⇒ Can baryon asymmetry be due to 5 electroweak physics? Baryon number is violated in electroweak interactions. “Sphalerons”. Non-perturbative effect Hint: triangle anomaly in baryonic current Bµ : 2 µ 1 gW µνλρ a a ∂µ B = 3 3 ε Fµν F 3 colors generations 32π2 λρ Bq · · · a Fµν : SU(2)W field strength; gW : SU(2)W coupling Likewise, each leptonic current (n = e, µ,τ) 2 µ gW µνλρ a a ∂µ L = ε Fµν Fλρ n 32π2 · B is violated, B L B Le Lµ Lτ is not. -
Cosmic Initial Conditions for a Habitable Universe
MNRAS 470, 3095–3102 (2017) doi:10.1093/mnras/stx1448 Cosmic initial conditions for a habitable universe Sohrab Rahvar‹ Physics Department, Sharif University, PO Box 11365-9161, Azadi Avenue, Tehran, Iran Accepted 2017 June 8. Received 2017 May 31; in original form 2016 August 5 ABSTRACT Downloaded from https://academic.oup.com/mnras/article/470/3/3095/3956582 by guest on 23 September 2021 Within the framework of an eternal inflationary scenario, a natural question regarding the production of eternal bubbles is the essential conditions required to have a universe capable of generating life. In either an open or a closed universe, we find an anthropic lower bound on the amount of e-folding in the order of 60 for the inflationary epoch, which results in the formation of large-scale structures in both linear and non-linear regimes. We extend the question of the initial condition of the universe to the sufficient condition in which we have enough initial dark matter and baryonic matter asymmetry in the early universe for the formation of galactic halos, stars, planets and consequently life. We show that the probability of a habitable universe is proportional to the asymmetry of dark and baryonic matter, while the cosmic budget of baryonic matter is limited by astrophysical constraints. Key words: inflation – large-scale structure of Universe. tion of large-scale structures. These small density fluctuations in 1 INTRODUCTION the dark matter fluid, of order ∼10−5, eventually grow and pro- The habitability of the Universe is one of the fundamental issues duce potential wells and, through gravitational condensation and of cosmology. -
Hot Big Bang Model: Early Universe and History of Matter Initial „Soup“ with Elementary Particles and Radiation in Thermal Equilibrium
Hot Big Bang model: early Universe and history of matter Initial „soup“ with elementary particles and radiation in thermal equilibrium. Radiation dominated era (recall energy density grows faster than matter density going back in time (~ a-4 rather than a-3). Thermal equilbrium maintained by electroweak interactions between individual particle species and between them and radiation field --- interaction rate G=n<vs>, where n is the number density of a type of particles, s the cross section and v the relative velocity (s depends on v in general). Key concepts: (1) At any given time particles can be created if their rest mass energy is such that kBT >> mc2, where T is the temperature of radiation. As the Universe expands T ~ a-1 (radiation dominated) so only increasingly lighter particles can be created. Important example: pair production from g + g < - -> e- + e+ (requires T > 5.8 x 109 K), which Immediately thermalize with electrons via Compton scattering and produce electronic - neutrinos via e- + e+ < --> ne + n e , also in thermal equilibrium with radiation. (2) As the Universe expands G decreases because n and v decrease -! when G < H(t) particle species decouples from photon fluid and n „freezes-out“ to the value at first decoupling(subsequently diluted only by expansion of Universe if particle stable). Present-day elementary particles are „thermal relics“ that have decoupled from photon 2 fluid at different times, some when they were still relativistic („hot relics“, kBT >> mc , T 2 is temperature of radiation field), some when they were non-relativistic (kBT <<mc ,“cold relics“) In the early Universe the very high temperatures (T ~ 1010 K a t ~ 1 s) guarantee that all elementary particles are relativistic and in thermal equilibrium with radiation.