Matter-antimatter asymmetry in the Universe

Size: px
Start display at page:

Download "Matter-antimatter asymmetry in the Universe"

Transcription

1 Matter-antimatter asymmetry in the Universe Wan-il Park (KIAS) APCTP-TRP, Nov Dec. 01 (2012), APCTP, Seoul 1

2 Plan Lecture 1 - Our universe - Birth of antimatter - Matter vs. antimatter - Baryon asymmetry in the universe - Symmetry breaking - The origin of the asymmetry Lecture 2 - Ingredients for baryogenesis - Mechanesms 2

3 Our universe Big: RH~3000Mpc~10 10 ly~10 28 cm~10 60 lp Old: th~10 17 sec~10 60 tp Flat: R cur 10H -1 Lots of matter(?): Stars, Galaxies, Clusters, Clusters of Clusters. 3

4 WMAP7 cosmological data Matter: ~27 %, Dark energy: ~73 % [PDG] m 10 6 GeV/cm g/cm 3 ) 1 proton/m 3 4

5 Universe seems made of matter, but our theories predict the existence of antimatter. 5

6 Birth of anti-matter Paul Dirac Relativistic quantum mechanics of free electron: = 0 { k = 0 k Two energy eigenvalues 6

7 Negative energy state? what is this? Dirac s interpretation Feynman-Stuckelberg(1948) A hole in the Dirac sea electron traveling backward in time 7

8 Matter vs. Antimatter A set of charges defines matter or anti-matter. Particle : (x µ ; m, q i ) Antiparticle : C (x µ ; m, q i ) If charge-neutral? particle = antiparticle Relativistic quantum field theories is invariant under CPT-transformation. (Lorentz invariance CPT invariance) m = m 8

9 Precision test of CPT invariance 9

10 Symmetric world # of Particles = # of antiparticles Amount of matter = amount of antimatter A particle meets its antiparticle, and annihilate, leaving only photons and neutrinos. So, in a symmetric world, only photons and neutrinos remain. No structure! (neutrino star? galaxy?) 10

11 Baryon asymmetry in the Universe Empirically, - Daily life: no proton-antiproton annihilation - Solar system: successes of satellite launches, lunar landings and planetary probes - Galaxy: only secondary production of antimatter in cosmic rays - Clusters: non-observation of detectable γ-ray background - Hubble size: no distortion of CMB radiation due to diffuse γ-ray From Big Bang Nucleosynthesis - The abundances of light elements are functions of BAU From cosmic microwave background radiation - CMB acoustic peaks are sensitive to BAU 11

12 Big Bang Nucleosynthesis [Kolb and Tuner] Number density of a nuclear species n A = g A ma T 2 3/2 exp µa T m A Mass fraction X A n AA n B, X X i =1 i µ A = Zµ p +(A Z)µ n B A Zm p +(A Z)m n m A X A / T m N 3(A 1)/2 A 1 X Z p X A Z n exp (B A /T ) Freeze-out of weak interactions p n ' G 2 F T 5 = H(T ) ) T fz 1MeV n n n p =exp mn m p T fz ' 1 6!

13 Determination of the abundances of light elements n A =(X A /A) n = n A (,n ) reaction = h vi n i = f(t ) n i reaction(,t A fz )=H(T A fz ) ) n A (,T A fz ) The abundance of a light element is determined by baryon number asymmetry (η). 13

14 14

15 Cosmic microwave background radiation (CMBR) Saha equation (for the equil. ionization fraction) 1 Xe eq (Xe eq ) 2 = 4 p 2 (3) p Recombination : X eq e T m e 3/2 exp(b H /T ) 0.1 ) T 0.3eV Decoupling of photon from free electrons = n e T e e (Thomson scattering) Decoupling : = H(T ) ) T 0.26eV CMBR = the photon released at decoupling 15

16 CMB from COBE 16

17 CMB from COBE T =2.73K 16

18 T T

19 Acoustic peaks in CMBR Odd peaks: compression Even peaks: rarefaction [ index.html] n B n '

20 Where is the asymmetry from? Theories are invariant under CPT, but... 19

21 Symmetry breaking 1954(Chinowski, Steinberger): An atomic decay: D(p + n)+! [n + n] L=0 L=1 { P tot = P (i) ( 1) L i P (D) =P (p) =P (n) =1 ) P ( )= 1 Pion parity is negative. Before 1956: General belief: Nature is symmetric w.r.t. C and P 1956(Lee, Yang)+1957(Wu, Ambler, Hayward, Hoppes, Hudson): P-violation from the β-decay of Cobalt-60 n! p (+W )! p + e + e C-violation from the non-existence of left-handed antineutrino C( L )= L? 20

22 1964(Cronin, Fitch, Christenson, Turlay): Decay of a long-lived Kaon to two pions K 0 = d s, K L = 1 p 2 K 0 K 0 [K L ] CP= 1! ( + + ) or ( ) CP=+1 CP is violated! Antiparticle does not behaves in a exactly same way as particle. 21

23 Origin of nb/nγ~10-10 Baryogenesis! 22

24 Summary-1 Our universe is made of matter. The asymmetry between matter and antimatter is nb/nγ~ The asymmetry should be generated after inflation dynamically, i.e., baryogenesis is necessary. 23

25 Backup [Wayne Hu, Maryland, Oct., 2002] 24

26 s = c s c 2 s = ṗ ' 1 3 [Wayne Hu, Maryland, Oct., 2002] 25

Brief Introduction to Cosmology

Brief Introduction to Cosmology Brief Introduction to Cosmology Matias Zaldarriaga Harvard University August 2006 Basic Questions in Cosmology: How does the Universe evolve? What is the universe made off? How is matter distributed? How

More information

Introduction to Cosmology

Introduction 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 information

Computational Applications in Nuclear Astrophysics using JAVA

Computational Applications in Nuclear Astrophysics using JAVA Computational Applications in Nuclear Astrophysics using JAVA Lecture: Friday 10:15-11:45 Room NB 7/67 Jim Ritman and Elisabetta Prencipe j.ritman@fz-juelich.de e.prencipe@fz-juelich.de Computer Lab: Friday

More information

Cosmology. 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 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 information

Hot Big Bang model: early Universe and history of matter

Hot Big Bang model: early Universe and history of matter Hot Big Bang model: early Universe and history of matter nitial soup with elementary particles and radiation in thermal equilibrium. adiation dominated era (recall energy density grows faster than matter

More information

Lecture 19 Nuclear Astrophysics. Baryons, Dark Matter, Dark Energy. Experimental Nuclear Physics PHYS 741

Lecture 19 Nuclear Astrophysics. Baryons, Dark Matter, Dark Energy. Experimental Nuclear Physics PHYS 741 Lecture 19 Nuclear Astrophysics Baryons, Dark Matter, Dark Energy Experimental Nuclear Physics PHYS 741 heeger@wisc.edu References and Figures from: - Haxton, Nuclear Astrophysics - Basdevant, Fundamentals

More information

Astr 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 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 information

Nucleosíntesis primordial

Nucleosíntesis primordial Tema 5 Nucleosíntesis primordial Asignatura de Física Nuclear Curso académico 2009/2010 Universidad de Santiago de Compostela Big Bang cosmology 1.1 The Universe today The present state of the Universe

More information

Ay1 Lecture 18. The Early Universe and the Cosmic Microwave Background

Ay1 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 information

Propagation in the Galaxy 2: electrons, positrons, antiprotons

Propagation in the Galaxy 2: electrons, positrons, antiprotons Propagation in the Galaxy 2: electrons, positrons, antiprotons As we mentioned in the previous lecture the results of the propagation in the Galaxy depend on the particle interaction cross section. If

More information

Astronomy 182: Origin and Evolution of the Universe

Astronomy 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 information

Antimatter. Jan Meier. Seminar: Experimental Methods in Atomic Physics May, 8th 2007

Antimatter. Jan Meier. Seminar: Experimental Methods in Atomic Physics May, 8th 2007 Antimatter Jan Meier Seminar: Experimental Methods in Atomic Physics May, 8th 27 Overview Antimatter and CPT theorie what is antimatter? what physics does it follow to? First observations of antimatter

More information

Lecture #24: Plan. Cosmology. Expansion of the Universe Olber s Paradox Birth of our Universe

Lecture #24: Plan. Cosmology. Expansion of the Universe Olber s Paradox Birth of our Universe Lecture #24: Plan Cosmology Expansion of the Universe Olber s Paradox Birth of our Universe Reminder: Redshifts and the Expansion of the Universe Early 20 th century astronomers noted: Spectra from most

More information

Astronomy 182: Origin and Evolution of the Universe

Astronomy 182: Origin and Evolution of the Universe Astronomy 182: Origin and Evolution of the Universe Prof. Josh Frieman Lecture 10 Nov. 11, 2015 Today Hot Big Bang I: Cosmic Microwave Background Assignments This week: read Hawley and Holcomb, Chapter

More information

Lecture 09. The Cosmic Microwave Background. Part II Features of the Angular Power Spectrum

Lecture 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 information

Physics 661. Particle Physics Phenomenology. October 2, Physics 661, lecture 2

Physics 661. Particle Physics Phenomenology. October 2, Physics 661, lecture 2 Physics 661 Particle Physics Phenomenology October 2, 2003 Evidence for theory: Hot Big Bang Model Present expansion of the Universe Existence of cosmic microwave background radiation Relative abundance

More information

\ \ \/ \\// (o) (o) U. February 11, UT Saturday Morning Physics. Yuri Kamyshkov University of Tennessee

\ \ \/ \\// (o) (o) U. February 11, UT Saturday Morning Physics. Yuri Kamyshkov University of Tennessee \ \ \/ \\// (o) (o) U February 11, 2017 @ UT Saturday Morning Physics Yuri Kamyshkov University of Tennessee kamyshkov@utk.edu 1 2 Large Hadron Collider CERN European Centre for Particle Physics Geneva,

More information

ASTR 1120 General Astronomy: Stars & Galaxies. OUR Universe: Accelerating Universe

ASTR 1120 General Astronomy: Stars & Galaxies. OUR Universe: Accelerating Universe ASTR 1120 General Astronomy: Stars & Galaxies FINAL: Saturday, Dec 12th, 7:30pm, HERE ALTERNATE FINAL: Monday, Dec 7th, 5:30pm in Muenzinger E131 Last OBSERVING session, Tue, Dec.8th, 7pm Please check

More information

VU lecture Introduction to Particle Physics. Thomas Gajdosik, FI & VU. Big Bang (model)

VU 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 information

John Ellison University of California, Riverside. Quarknet 2008 at UCR

John Ellison University of California, Riverside. Quarknet 2008 at UCR Overview of Particle Physics John Ellison University of California, Riverside Quarknet 2008 at UCR 1 Particle Physics What is it? Study of the elementary constituents of matter And the fundamental forces

More information

3 Observational Cosmology Evolution from the Big Bang Lecture 2

3 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 information

n=0 l (cos θ) (3) C l a lm 2 (4)

n=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 information

Chapter 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 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 information

Astronomy 182: Origin and Evolution of the Universe

Astronomy 182: Origin and Evolution of the Universe Astronomy 182: Origin and Evolution of the Universe Prof. Josh Frieman Lecture 12 Nov. 18, 2015 Today Big Bang Nucleosynthesis and Neutrinos Particle Physics & the Early Universe Standard Model of Particle

More information

Lecture notes 21: Nucleosynthesis. Measuring Cosmological Parameters

Lecture notes 21: Nucleosynthesis. Measuring Cosmological Parameters Lecture notes : Nucleosynthesis. Measuring Cosmological Parameters In the last lecture, using the fluid equation, we derived a relation between the energy density of a material obeying an equation of state

More information

What is the 'cosmological principle'?

What is the 'cosmological principle'? What is the 'cosmological principle'? Modern cosmology always starts from this basic assumption the Universe is homogeneous and isotropic. This idea seems strange there's empty space between me and the

More information

Early (Expanding) Universe. Average temperature decreases with expansion.

Early (Expanding) Universe. Average temperature decreases with expansion. Early (Expanding) Universe Average temperature decreases with expansion. Particles & Anti-Particles Very short wavelength photons collide and form electron-positron pairs. E=mc 2 electron=matter positron=antimatter

More information

Announcements. Homework. Set 8now open. due late at night Friday, Dec 10 (3AM Saturday Nov. 11) Set 7 answers on course web site.

Announcements. Homework. Set 8now open. due late at night Friday, Dec 10 (3AM Saturday Nov. 11) Set 7 answers on course web site. Homework. Set 8now. due late at night Friday, Dec 10 (3AM Saturday Nov. 11) Set 7 answers on course web site. Review for Final. In class on Thursday. Course Evaluation. https://rateyourclass.msu.edu /

More information

Big Bang Nucleosynthesis

Big Bang Nucleosynthesis Big Bang Nucleosynthesis George Gamow (1904-1968) 5 t dec ~10 yr T dec 0.26 ev Neutrons-protons inter-converting processes At the equilibrium: Equilibrium holds until 0 t ~14 Gyr Freeze-out temperature

More information

Cosmology: Building the Universe.

Cosmology: Building the Universe. Cosmology: Building the Universe. The term has several different meanings. We are interested in physical cosmology - the study of the origin and development of the physical universe, and all the structure

More information

We can check experimentally that physical constants such as α have been sensibly constant for the past ~12 billion years

We can check experimentally that physical constants such as α have been sensibly constant for the past ~12 billion years ² ² ² The universe observed ² Relativistic world models ² Reconstructing the thermal history ² Big bang nucleosynthesis ² Dark matter: astrophysical observations ² Dark matter: relic particles ² Dark matter:

More information

Cosmology. Thornton and Rex, Ch. 16

Cosmology. Thornton and Rex, Ch. 16 Cosmology Thornton and Rex, Ch. 16 Expansion of the Universe 1923 - Edwin Hubble resolved Andromeda Nebula into separate stars. 1929 - Hubble compared radial velocity versus distance for 18 nearest galaxies.

More information

IoP. An Introduction to the Science of Cosmology. Derek Raine. Ted Thomas. Series in Astronomy and Astrophysics

IoP. An Introduction to the Science of Cosmology. Derek Raine. Ted Thomas. Series in Astronomy and Astrophysics Series in Astronomy and Astrophysics An Introduction to the Science of Cosmology Derek Raine Department of Physics and Astronomy University of Leicester, UK Ted Thomas Department of Physics and Astronomy

More information

Fundamental Particles

Fundamental 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 information

Hubble's Law. H o = 71 km/s / Mpc. The further a galaxy is away, the faster it s moving away from us. V = H 0 D. Modern Data.

Hubble's Law. H o = 71 km/s / Mpc. The further a galaxy is away, the faster it s moving away from us. V = H 0 D. Modern Data. Cosmology Cosmology is the study of the origin and evolution of the Universe, addressing the grandest issues: How "big" is the Universe? Does it have an "edge"? What is its large-scale structure? How did

More information

Physics 133: Extragalactic Astronomy and Cosmology. Week 8

Physics 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 information

Mass (Energy) in the Universe:

Mass (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 information

Origin of the Universe - 2 ASTR 2120 Sarazin. What does it all mean?

Origin of the Universe - 2 ASTR 2120 Sarazin. What does it all mean? Origin of the Universe - 2 ASTR 2120 Sarazin What does it all mean? Fundamental Questions in Cosmology 1. Why did the Big Bang occur? 2. Why is the Universe old? 3. Why is the Universe made of matter?

More information

Astroparticle physics the History of the Universe

Astroparticle physics the History of the Universe Astroparticle physics the History of the Universe Manfred Jeitler and Wolfgang Waltenberger Institute of High Energy Physics, Vienna TU Vienna, CERN, Geneva Wintersemester 2016 / 2017 1 The History of

More information

A Brief History of Modern Physics

A Brief History of Modern Physics A Brief History of Modern Physics Modern Physics rests on two pillars: 1. Theory of Relativity (Einstein) Special Relativity 1905 General Relativity 1915 nature of space and time (phenomena at high speed)

More information

Lecture 03. The Cosmic Microwave Background

Lecture 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 information

i>clicker Quiz #14 Which of the following statements is TRUE?

i>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 information

Cosmology. Jörn Wilms Department of Physics University of Warwick.

Cosmology. Jörn Wilms Department of Physics University of Warwick. Cosmology Jörn Wilms Department of Physics University of Warwick http://astro.uni-tuebingen.de/~wilms/teach/cosmo Contents 2 Old Cosmology Space and Time Friedmann Equations World Models Modern Cosmology

More information

The Big Bang The Beginning of Time

The Big Bang The Beginning of Time The Big Bang The Beginning of Time What were conditions like in the early universe? The early universe must have been extremely hot and dense Photons converted into particle-antiparticle pairs and vice-versa

More information

Energy Density: u = ρc 2 ( kt) 1 Pressure: p = u. 3 ζ kt, π 2 ( hc) 3. Entropy density:

Energy Density: u = ρc 2 ( kt) 1 Pressure: p = u. 3 ζ kt, π 2 ( hc) 3. Entropy density: Alan Guth, Cosmic Microwave Background (CMB) Spectrum and the Cosmological Constant, Lecture 18, November 14, 2013, p. 1. : Black-Body Radiation Lecture 18 14, 2013 November π 2 Energy Density: u = ρc

More information

Chapter 22 Back to the Beginning of Time

Chapter 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 information

The Early Universe: A Journey into the Past

The 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 information

Concordance Cosmology and Particle Physics. Richard Easther (Yale University)

Concordance 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 information

ASTR 101 General Astronomy: Stars & Galaxies

ASTR 101 General Astronomy: Stars & Galaxies ASTR 101 General Astronomy: Stars & Galaxies ANNOUNCEMENTS FINAL EXAM: THURSDAY, May 14 th, 11:15am Last Astronomy public talk, May 8 th (up to 3% Extra class credit (see Blackboard announcement for details)

More information

. Thus his equation would have to be of the form. 2 t. but must also satisfy the relativistic energy-momentum relation. H 2 φ = ( p 2 + m 2 )φ (3)

. Thus his equation would have to be of the form. 2 t. but must also satisfy the relativistic energy-momentum relation. H 2 φ = ( p 2 + m 2 )φ (3) 1 Antiparticles The Klein-Gordon equation 2 φ t 2 + 2 φ = m 2 φ 1 that we derived in the previous lecture is not satisfactory for dealing with massive particles that have spin. Such an equation must take

More information

Big Bang Nucleosynthesis and Particle Physics

Big Bang Nucleosynthesis and Particle Physics New Generation Quantum Theory -Particle Physics, Cosmology and Chemistry- Kyoto University Mar.7-9 2016 Big Bang Nucleosynthesis and Particle Physics Masahiro Kawasaki (ICRR & Kavli IPMU, University of

More information

Rapid Inflation of the Early Universe. 27. Exploring the Early Universe. The Isotropy Problem. Possible Causes of Cosmic Inflation

Rapid Inflation of the Early Universe. 27. Exploring the Early Universe. The Isotropy Problem. Possible Causes of Cosmic Inflation 27. Exploring the Early Universe Rapid inflation of the early Universe Mass & energy formed during inflation Most matter & antimatter annihilated each other Neutrinos & helium are primordial fireball relics

More information

The Early Universe: A Journey into the Past

The Early Universe: A Journey into the Past The Early Universe A Journey into the Past Texas A&M University March 16, 2006 Outline Galileo and falling bodies Galileo Galilei: all bodies fall at the same speed force needed to accelerate a body is

More information

Lecture 8. CPT theorem and CP violation

Lecture 8. CPT theorem and CP violation Lecture 8 CPT theorem and CP violation We have seen that although both charge conjugation and parity are violated in weak interactions, the combination of the two CP turns left-handed antimuon onto right-handed

More information

Fundamentals of Neutrino Physics and Astrophysics

Fundamentals of Neutrino Physics and Astrophysics Fundamentals of Neutrino Physics and Astrophysics Carlo Giunti Istituto Nazionale di Fisica Nucleare, Sezione di Torino and Dipartimento di Fisica Teorica, Universita di Torino, Italy Chung W. Kim Korea

More information

One of elements driving cosmological evolution is the presence of radiation (photons) Early universe

One of elements driving cosmological evolution is the presence of radiation (photons) Early universe The Frontier Matter and Antimatter One of elements driving cosmological evolution is the presence of radiation (photons) Early universe Matter and antimatter But we live in universe full of matter -- where

More information

Astro-2: History of the Universe. Lecture 12; May

Astro-2: History of the Universe. Lecture 12; May Astro-2: History of the Universe Lecture 12; May 23 2013 Previously on astro-2 The four fundamental interactions are? Strong, weak, electromagnetic and gravity. We think they are unified at high energies,

More information

Lecture 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 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 information

Introduction. How did the universe evolve to what it is today?

Introduction. How did the universe evolve to what it is today? Cosmology 8 1 Introduction 8 2 Cosmology: science of the universe as a whole How did the universe evolve to what it is today? Based on four basic facts: The universe expands, is isotropic, and is homogeneous.

More information

Elementary Particles, Flavour Physics and all that...

Elementary Particles, Flavour Physics and all that... Elementary Particles, Flavour Physics and all that... 1 Flavour Physics The term Flavour physics was coined in 1971 by Murray Gell-Mann and his student at the time, Harald Fritzsch, at a Baskin-Robbins

More information

Inflationary Universe and. Quick survey about iclickers Review of Big Bang model of universe Review of Evidence for Big Bang Examining Inflation

Inflationary Universe and. Quick survey about iclickers Review of Big Bang model of universe Review of Evidence for Big Bang Examining Inflation Inflationary Universe and Quick survey about iclickers Review of Big Bang model of universe Review of Evidence for Big Bang Examining Inflation Survey questions 1. The iclickers used in class encouraged

More information

Survey questions. Inflationary Universe and. Survey Questions. Survey questions. Survey questions

Survey questions. Inflationary Universe and. Survey Questions. Survey questions. Survey questions Inflationary Universe and Quick survey about iclickers Review of Big Bang model of universe Review of Evidence for Big Bang Examining Inflation Survey questions 1. The iclickers used in class encouraged

More information

Lecture 19 Big Bang Nucleosynthesis

Lecture 19 Big Bang Nucleosynthesis Lecture 19 Big Bang Nucleosynthesis As with all course material (including homework, exams), these lecture notes are not be reproduced, redistributed, or sold in any form. The CMB as seen by the WMAP satellite.!2

More information

A100 Exploring the Universe Big Bang Theory and the Early Universe. Martin D. Weinberg UMass Astronomy

A100 Exploring the Universe Big Bang Theory and the Early Universe. Martin D. Weinberg UMass Astronomy A100 Exploring the Universe and the Martin D. Weinberg UMass Astronomy astron100-mdw@courses.umass.edu December 02, 2014 Read: Chap 23 12/04/14 slide 1 Assignment on Chaps 22 23, at the end of next week,

More information

El 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 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 information

OUSSEP Final Week. If we run out of time you can look at uploaded slides Pearson Education, Inc.

OUSSEP Final Week. If we run out of time you can look at uploaded slides Pearson Education, Inc. OUSSEP Final Week Last week hopefully read Holiday-Week 23rd November Lecture notes Hand in your Hubble Deep Field Reports today! (If not today then in my mail box @ International College.) Today we will

More information

BIG BANG SUMMARY NOTES

BIG BANG SUMMARY NOTES BIG BANG SUMMARY NOTES BIG BANG THEORY Studies of red-shifts of distant galaxies show that the universe is expanding. This and other observations has led to the Big Bang Theory The Big Bang Theory claims

More information

Lecture 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) 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 information

Text. References and Figures from: - Basdevant et al., Fundamentals in Nuclear Physics - Henley et al., Subatomic Physics

Text. References and Figures from: - Basdevant et al., Fundamentals in Nuclear Physics - Henley et al., Subatomic Physics Lecture 8 Experimental Nuclear Physics PHYS 741 Text heeger@wisc.edu References and Figures from: - Basdevant et al., Fundamentals in Nuclear Physics - Henley et al., Subatomic Physics 1 Review: Parity

More information

The slides with white background you need to know. The slides with blue background just have some cool information.

The slides with white background you need to know. The slides with blue background just have some cool information. The slides with white background you need to know. The slides with blue background just have some cool information. The Big Bang cosmology the study of the origin, properties, processes, and evolution

More information

Modern Cosmology / Scott Dodelson Contents

Modern 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 information

Particle Physics. Dr Victoria Martin, Spring Semester 2012 Lecture 14: CP and CP Violation

Particle Physics. Dr Victoria Martin, Spring Semester 2012 Lecture 14: CP and CP Violation Particle Physics Dr Victoria Martin, Spring Semester 01 Lecture 14: CP and CP Violation!Parity Violation in Weak Decay!CP and CPT!Neutral meson mixing!mixing and decays of kaons!cp violation in K 0 and

More information

Project Paper May 13, A Selection of Dark Matter Candidates

Project Paper May 13, A Selection of Dark Matter Candidates A688R Holly Sheets Project Paper May 13, 2008 A Selection of Dark Matter Candidates Dark matter was first introduced as a solution to the unexpected shape of our galactic rotation curve; instead of showing

More information

the astrophysical formation of the elements

the astrophysical formation of the elements the astrophysical formation of the elements Rebecca Surman Union College Second Uio-MSU-ORNL-UT School on Topics in Nuclear Physics 3-7 January 2011 the astrophysical formation of the elements lecture

More information

The Beginning of the Universe 8/11/09. Astronomy 101

The Beginning of the Universe 8/11/09. Astronomy 101 The Beginning of the Universe 8/11/09 Astronomy 101 Astronomy Picture of the Day Astronomy 101 Outline for Today Astronomy Picture of the Day Return Lab 11 Astro News Q&A Session Dark Energy Cosmic Microwave

More information

12 Big Bang Nucleosynthesis. introduc)on to Astrophysics, C. Bertulani, Texas A&M-Commerce 1

12 Big Bang Nucleosynthesis. introduc)on to Astrophysics, C. Bertulani, Texas A&M-Commerce 1 12 Big Bang Nucleosynthesis introduc)on to Astrophysics, C. Bertulani, Texas A&M-Commerce 1 12.1 The Early Universe According to the accepted cosmological theories: The Universe has cooled during its expansion

More information

Cosmology. Big Bang and Inflation

Cosmology. Big Bang and Inflation Cosmology Big Bang and Inflation What is the Universe? Everything we can know about is part of the universe. Everything we do know about is part of the universe. Everything! The Universe is expanding If

More information

Lecture #25: Plan. Cosmology. The early Universe (cont d) The fate of our Universe The Great Unanswered Questions

Lecture #25: Plan. Cosmology. The early Universe (cont d) The fate of our Universe The Great Unanswered Questions Lecture #25: Plan Cosmology The early Universe (cont d) The fate of our Universe The Great Unanswered Questions Announcements Course evaluations: CourseEvalUM.umd.edu Review sheet #3 was emailed to you

More information

COSMOLOGY AND GRAVITATIONAL WAVES. Chiara Caprini (APC)

COSMOLOGY AND GRAVITATIONAL WAVES. Chiara Caprini (APC) COSMOLOGY AND GRAVITATIONAL WAVES Chiara Caprini (APC) the direct detection of GW by the LIGO interferometers has opened a new era in Astronomy - we now have a new messenger bringing complementary informations

More information

Matter vs. Antimatter in the Big Bang. E = mc 2

Matter vs. Antimatter in the Big Bang. E = mc 2 Matter vs. Antimatter in the Big Bang Threshold temperatures If a particle encounters its corresponding antiparticle, the two will annihilate: particle + antiparticle ---> radiation * Correspondingly,

More information

Licia Verde. Introduction to cosmology. Lecture 4. Inflation

Licia 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 information

Option 212: UNIT 2 Elementary Particles

Option 212: UNIT 2 Elementary Particles Department of Physics and Astronomy Option 212: UNIT 2 Elementary Particles SCHEDULE 26-Jan-15 13.pm LRB Intro lecture 28-Jan-15 12.pm LRB Problem solving (2-Feb-15 1.am E Problem Workshop) 4-Feb-15 12.pm

More information

4 The Big Bang, the genesis of the Universe, the origin of the microwave background

4 The Big Bang, the genesis of the Universe, the origin of the microwave background 4 The Big Bang, the genesis of the Universe, the origin of the microwave background a(t) = 0 The origin of the universe: a(t) = 0 Big Bang coined by Fred Hoyle he calculated the ratio of elements created

More information

CPT Symmetry and Symmetry-Breaking in the Scale-Symmetric Theory

CPT Symmetry and Symmetry-Breaking in the Scale-Symmetric Theory Copyright 2015 by Sylwester Kornowski All rights reserved CPT Symmetry and Symmetry-Breaking in the Scale-Symmetric Theory Sylwester Kornowski Abstract: During the inflation, to eliminate turbulences in

More information

Plasma Universe. The origin of CMB

Plasma Universe. The origin of CMB Plasma Universe As we go back in time, temperature goes up. T=2.73(1+z) K At z~1100, T~3000 K About the same temperature as M-dwarfs Ionization of hydrogen atoms H + photon! p + e - Inverse process: recombination

More information

Lecture 17: the CMB and BBN

Lecture 17: the CMB and BBN Lecture 17: the CMB and BBN As with all course material (including homework, exams), these lecture notes are not be reproduced, redistributed, or sold in any form. Peering out/back into the Universe As

More information

Week 3 - Part 2 Recombination and Dark Matter. Joel Primack

Week 3 - Part 2 Recombination and Dark Matter. Joel Primack Astro/Phys 224 Spring 2012 Origin and Evolution of the Universe Week 3 - Part 2 Recombination and Dark Matter Joel Primack University of California, Santa Cruz http://pdg.lbl.gov/ In addition to the textbooks

More information

Astr 102: Introduction to Astronomy. Lecture 16: Cosmic Microwave Background and other evidence for the Big Bang

Astr 102: Introduction to Astronomy. Lecture 16: Cosmic Microwave Background and other evidence for the Big Bang Astr 102: Introduction to Astronomy Fall Quarter 2009, University of Washington, Željko Ivezić Lecture 16: Cosmic Microwave Background and other evidence for the Big Bang 1 Outline Observational Cosmology:

More information

Parity violation. no left-handed ν$ are produced

Parity violation. no left-handed ν$ are produced Parity violation Wu experiment: b decay of polarized nuclei of Cobalt: Co (spin 5) decays to Ni (spin 4), electron and anti-neutrino (spin ½) Parity changes the helicity (H). Ø P-conservation assumes a

More information

Cosmology II: The thermal history of the Universe

Cosmology 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 information

Cosmic Microwave Background Introduction

Cosmic 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 information

Physics of the hot universe!

Physics of the hot universe! Cosmology Winter School 5/12/2011! Lecture 2:! Physics of the hot universe! Jean-Philippe UZAN! The standard cosmological models! a 0!! Eq. state! Scaling Scale factor! radiation! w=1/3! a -4! t 1/2! Matter

More information

Cosmic Microwave Background. Eiichiro Komatsu Guest Lecture, University of Copenhagen, May 19, 2010

Cosmic Microwave Background. Eiichiro Komatsu Guest Lecture, University of Copenhagen, May 19, 2010 Cosmic Microwave Background Eiichiro Komatsu Guest Lecture, University of Copenhagen, May 19, 2010 1 Cosmology: The Questions How much do we understand our Universe? How old is it? How big is it? What

More information

Astronomy 113. Dr. Joseph E. Pesce, Ph.D Joseph E. Pesce, Ph.D.

Astronomy 113. Dr. Joseph E. Pesce, Ph.D Joseph E. Pesce, Ph.D. Astronomy 113 Dr. Joseph E. Pesce, Ph.D. The Big Bang & Matter 17-2 Cosmology ³ The study of the origins, structure, and evolution of the universe ³ Key moments: ² Einstein General Theory of Relativity

More information

Astronomy 113. Dr. Joseph E. Pesce, Ph.D. The Big Bang & Matter. Olber s Paradox. Cosmology. Olber s Paradox. Assumptions 4/20/18

Astronomy 113. Dr. Joseph E. Pesce, Ph.D. The Big Bang & Matter. Olber s Paradox. Cosmology. Olber s Paradox. Assumptions 4/20/18 Astronomy 113 Dr. Joseph E. Pesce, Ph.D. The Big Bang & Matter Cosmology ³The study of the origins, structure, and evolution of the universe ³Key moments: ²Einstein General Theory of Relativity ²Hubble

More information

Timeline 5/4/17. Our Schedule and Topics

Timeline 5/4/17. Our Schedule and Topics ASTR 1040: Stars & Galaxies Cosmic Web Prof. Juri Toomre TAs: Piyush Agrawal, Connor Bice Lecture 30 Thur 4 May 2017 zeus.colorado.edu/astr1040-toomre Our Schedule and Topics Final Exam on Wed May 10,

More information

ASTR 101 General Astronomy: Stars & Galaxies

ASTR 101 General Astronomy: Stars & Galaxies ASTR 101 General Astronomy: Stars & Galaxies ANNOUNCEMENTS MIDTERM III: Tuesday, Nov 24 th Midterm alternate day: Fri, Nov 20th, 11am, ESS 450 At LAST: In the very Beginning BIG BANG: beginning of Time

More information

Cosmology and particle physics

Cosmology and particle physics Fedora GNU/Linux; LATEX 2ɛ; xfig Cosmology and particle physics Mark Alford Washington University Saint Louis, USA Outline I Particle physics: What the universe is made of. quarks, leptons, and the forces

More information

Astronomy 422. Lecture 20: Cosmic Microwave Background

Astronomy 422. Lecture 20: Cosmic Microwave Background Astronomy 422 Lecture 20: Cosmic Microwave Background Key concepts: The CMB Recombination Radiation and matter eras Next time: Astro 422 Peer Review - Make sure to read all 6 proposals and send in rankings

More information

The Origin of Matter

The Origin of Matter The Origin of Matter ---- Leptogenesis ---- Tsutomu T. Yanagida (IPMU, Tokyo) Shoichi Sakata Centennial Symposium Energy Content of the Universe いいい From Wikipedia F FF Galaxy and Cluster of galaxies No

More information