Major Epochs in the Early Universe t<3x10 5 years: Universe radiation dominated t>3x10 5 years: Universe matter dominated Why? Let R be the scale length.

Slides:



Advertisements
Similar presentations
The Expanding Universe!
Advertisements

A Scientific History of the Universe. How do we predict the conditions of the early universe? What are the different eras in the early universe? What.
Chapter 17 The Beginning of Time
Chapter 17: The Birth of the Universe
The Big Bang Necessary? –Expansion of the Universe –Origin of CMBR 400 photons/cc Black body temperature profile –Helium content Universal nucleosynthesis.
ORIGIN OF THE UNIVERSE P In the beginning, God created the heaven and the earth; and the earth was without form and void; and darkness was upon the face.
Cosmology The Origin and Future of the Universe Part 2 From the Big Bang to Today.
The Big Bang Or… The Standard Model. Precepts of the standard model The laws of Physics are the same throughout the Universe. The Universe is expanding.
Big Bang …..was actually very small and quiet. Atoms are mostly empty space.
Chapter 27: The Early Universe Expansion Fundamental forces Creation of matter and antimatter Density fluctuations and the structure of the universe 11.
Advances in contemporary physics and astronomy --- our current understanding of the Universe Lecture 5: Evolution of Early Universe April 30 th, 2003.
Galaxy Evolution 1) Density fluctuations in the primordial matter 2) galaxies grew by repeated merging of smaller objects - evidence: galaxies at large.
Physics 133: Extragalactic Astronomy and Cosmology Lecture 15; March
© 2010 Pearson Education, Inc. Chapter 23 The Beginning of Time.
Chapter 29 Exploring the Early Universe. Guiding Questions 1.Has the universe always expanded as it does today? 2.What is antimatter? How can it be created,
Background radiation (light) from Big Bang (visible) freely streaming from universe since atoms formed at temperature ~ 3,000 K (cf. sun = 6000 K)
Do your course evaluations.
Introductory Video: The Big Bang Theory Objectives  Understand the Hubble classification scheme of galaxies and describe the structure of the Milky.
Universe: Space-time, Matter, Energy Very little matter-energy is observable Critical matter-energy density balances expansion and gravitational collapse.
Astro-2: History of the Universe Lecture 12; May
The Big Bang Or… The Standard Model. Precepts of the standard model The laws of Physics are the same throughout the Universe. The Universe is expanding.
The Big Bang. CMBR Discussion Why can’t the CMBR be from a population of unresolved stars at high redshift?
Pop-quiz #21 Which of the following statements is TRUE? A.Black holes can emit particles and thereby lose mass — this is called Hawking radiation B.John.
Hubble’s Law Our goals for learning What is Hubble’s Law?
Cosmology and Dark Matter II: The inflationary Universe Jerry Sellwood.
Cosmic Microwave Background Radiation (CMBR) Relic of the Big Bang (“afterglow” of initial fireball) predicted in late 1940s Discovered by Penzias & Wilson.
Cosmology The Origin, Evolution, and Destiny of the Universe.
Exploring the Early Universe Chapter Twenty-Nine.
Intro to Cosmology! OR What is our Universe?. The Latest High Resolution Image of the Cosmic Microwave Background Radiation Low Energy RegionHigh Energy.
© 2010 Pearson Education, Inc. Chapter 23 The Beginning of Time.
The Birth of the Universe. Hubble Expansion and the Big Bang The fact that more distant galaxies are moving away from us more rapidly indicates that the.
Today: “Nucleosynthesis… another phase change in early universe… and why is the Universe so Flat?” HW for next time: Onion, “the nucleus and forces of.
BIG BANG TIMELINE FILL IN YOUR MISSING DATA. THE BIG BANG 0 to seconds Temperature- theorized to be infinite Infinitely small, Infinitely Dense,
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.
FRW-models, summary. Properties of the Universe set by 3 parameters:  m,  ,  k of Which only 2 are Independent:  m +   +  k = 1.
Universe Scale We can’t measure size of universe (especially if infinite), so compare distances at different times in history: Distances between non-moving.
PHY th century cosmology 1920s – 1990s (from Friedmann to Freedman)  theoretical technology available, but no data  20 th century: birth of observational.
The Life of the Universe From Beginning to End.
Chapter 17 The Beginning of Time. Running the Expansion Backward Temperature of the Universe from the Big Bang to the present (10 10 years ~ 3 x
Week 9 (11/13) – Quiz #22 Which of the following statements is TRUE? A.Inflation is the astronomical term used to describe the transformation our bellies.
The CMBR Horizon Problem The CMBR has the same properties in all directions. Consider two portions of the Universe from opposite ends of the sky. These.
The Beginning of Time: Evidence for the Big Bang & the Theory of Inflation.
Goal: To understand the history of the universe especially the beginning Objectives: 1)To learn about the beginning of the Big bang! 2)To explore the Big.
Cosmology -- the Origin and Structure of the Universe Cosmological Principle – the Universe appears the same from all directions. There is no preferred.
1 Cosmology HNRT 227 Chapter October 2015 Great Idea: The universe began billions of years ago in the big bang and it has been expanding ever since.
1 Cosmic Microwave Background Radiation (CMBR) Relic of the Big Bang ( “ afterglow ” of initial fireball) predicted in late 1940s Discovered by Penzias.
Universe Tenth Edition Chapter 26 Exploring the Early Universe Roger Freedman Robert Geller William Kaufmann III.
The Beginning of Time Review: evidence for dark matter evidence for dark matter comes from  motions of stars and gas in galaxies  motions of galaxies.
The Fate of the Universe What property determines the ultimate fate of the universe?
4/29/16 How can the darkness of the sky lead you to conclude that the universe had a beginning?
 Pinning down the date of creation with such precision is impressive, but we have gone much further. We have begun to piece together the whole history.
ASTR368 Cosmology Timeline Loren Anderson – Shanghai – May 14, 2013.
Discovering the Universe Eighth Edition Discovering the Universe Eighth Edition Neil F. Comins William J. Kaufmann III CHAPTER 18 Cosmology Cosmology.
Lecture 24: The Epochs of the Universe Astronomy 1143 – Spring 2014.
Important Stuff (Section 3) The Final Exam is Monday, December 19, 1:30 pm – 3:30 pm The Final Exam room is Physics 150 Bring 2 pencils and a photo-id.
Pop-quiz #13 Which of the following statements is TRUE? A.Inflation started right after Planck time when the Universe was seconds old B.Gravity.
First Million Years Today’s Lecture: First Million Years History of the Universe Particle Era Nucleosynthesis Atoms CMB Anisotropies Problems with Standard.
Chapter 23 The Beginning of Time
Georges LeMaitre theorized The Big Bang in 1927 two years before
Alternative to Big Bang theory: Steady State Cosmology
Universe! Early Universe.
Introduction To Modern Astronomy II
The Beginning of Time (Birth Of The Universe)
Learning Goals: I will:
Cosmology Chapter 15 Great Idea:
Early Universe.
History of the Universe
Homework #10 is due tonight, 9:00 pm.
A step by step guide to The Big Bang.
Recombination t = 380 ky T = 4000 K
Presentation transcript:

Major Epochs in the Early Universe t<3x10 5 years: Universe radiation dominated t>3x10 5 years: Universe matter dominated Why? Let R be the scale length of the Universe (the separation between your favorite pair of galaxies, say). Energy density of matter α 1/R 3 since volume α R 3 Energy density of radiation α 1/R 4 since λ “stretched out” α R. By Wien's Law, T decreases as 1/R, and by the blackbody eqn. energy density decreases as T 4 α 1/R 4

Unification of Forces All four fundamental forces of Nature unified at t< s, the Planck time. Gravity `froze' out separate from the other three forces at this time. Next the strong nuclear force froze out at t= s Weak and electromagnetic forces unified until t= s Electroweak unification confirmed in the laboratory during the 1980s at CERN particle accelerator in Europe.

Baryon Asymmetry Extremely hot radiation in the few seconds after the Big Bang Very energetic photons → continuous interchange of radiation into matter and vice versa (via pair production and pair annihilation). Observable Universe is made up of mostly matter (as opposed to anti-matter) Implies a slight asymmetry between matter and anti-matter in the very early Universe (a little more matter than antimatter) This is referred to as the `baryon asymmetry' of the Universe..

Confinement and Recombination Quarks are the basic particles that protons and neutrons are thought to be composed of. t=10 -6 sec (T=10 13 K), quarks were able to combine to form protons and neutrons → the epoch of confinement. After t= 3x10 5 years the temperature dropped to T=3000 K Protons and electrons (and neutrons) were able to combine to form neutral atoms. Matter and radiation practically ceased to interact with each other (i.e., the Universe became transparent to radiation → CMBR). The epoch of decoupling of matter and radiation or the epoch of recombination.

Big Bang Nucleosynthesis Almost all the hydrogen we see in the present Universe was formed at the epoch of recombination Most of the light elements (helium, deuterium, lithium, etc.) were formed shortly thereafter The efficiency with which these light elements were formed depends on what the density of protons and neutrons was (baryonic matter). Studying the abundance of light elements (relative to hydrogen) is a good way of determining the baryon content of the Universe. There is a fairly strong indication that most of the matter in the Universe is non-baryonic, in addition to being non- luminous.

The CMBR Horizon Problem The CMBR has the same properties in all directions. Consider two portions of the Universe from opposite ends of the sky. These two portions are within our observable Universe (horizon), but they are outside each other's horizons. Light has not yet had time to travel from one of these portions to the other. If they have never been in communication, how do they know to be at the same temperature?

Inflation Very early phase of extremely rapid expansion (Guth, Linde, 1980s). During this inflationary phase, the Universe expands by a factor of in the time span t= sec to t= sec. Inflationary phase is immediately after the epoch at which the strong nuclear force froze out, and before the weak nuclear force and electromagnetic force froze apart from each other. All of our observable Universe was an infinitesimally small volume x10 50 x10 50 = times smaller than we would have guessed from a simple extrapolation of the expansion we observe today.

Solving the Horizon Problem Two parts of the Universe on opposite sides of the sky now outside each other's horizons. Prior to inflationary epoch, these two patches would have been within each other's horizons and therefore `known' to acquire the same temperature. Inflation caused them to expand out of each other's horizon. Inflation requires the universe to expand faster than the speed of light. Does not violate special relativity — STR only applies in flat spacetime (i.e., in weak gravitational fields) Special relativity is a special case of General relativity; inflation does obey the equations of General relativity.

Inflation, continued Why is the density of the present Universe so close to critical (or why is the geometry of the observable Universe so close to flat)? The scale of the observable Universe is much smaller than its `radius of curvature'. What causes the rapid expansion during the inflationary era? Inflation may be thought of as a phase transition in the Universe (as in a transition from a liquid to solid phase). The `latent heat' in this phase transition builds up into an extremely high vacuum energy density, and this drives the expansion (analogous to the repulsive effect of Einstein's cosmological constant Λ).