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Chapter 27: The Early Universe The plan: 1. A brief survey of the entire history of the big bang universe. 2. A more detailed discussion of each phase, or “epoch”, from the Planck era through particle production, nucleosynthesis, recombination, and the growth of structure. 3. Then back to the (near) beginning, and “inflation.” 4. Finally the demonstration from the WMAP CBR map that the universe is almost perfectly flat. This ties together several separate strands of the big bang model for history of the universe. It also shows that inflation probably did occur, and dark matter and dark energy exist, whether or not we know what they are made of.

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Page 1: Chapter 27: The Early Universe - · PDF fileChapter 27: The Early Universe The plan: 1. A brief survey of the entire history of the big bang universe. 2. A more detailed discussion

Chapter 27: The Early Universe

The plan: 1. A brief survey of the entire history of thebig bang universe.

2. A more detailed discussion of each phase, or“epoch”, from the Planck era through particle production, nucleosynthesis, recombination,and the growth of structure.

3. Then back to the (near) beginning, and “inflation.”

4. Finally the demonstration from the WMAP CBR map that the universe is almost perfectlyflat. This ties together several separate strandsof the big bang model for history of the universe.

It also shows that inflation probably did occur, and dark matter and dark energy exist, whether or not we know what they are made of.

Page 2: Chapter 27: The Early Universe - · PDF fileChapter 27: The Early Universe The plan: 1. A brief survey of the entire history of the big bang universe. 2. A more detailed discussion

27.1 Back to the Big Bang

27.2 The Evolution of the Universe

More on Fundamental Forces

27.3 The Formation of Nuclei and Atoms

27.4 The Inflationary Universe

27.5 The Formation of Structure in the Universe

27.6 Cosmic Structure and the Microwave Background

Units of Chapter 27

Page 3: Chapter 27: The Early Universe - · PDF fileChapter 27: The Early Universe The plan: 1. A brief survey of the entire history of the big bang universe. 2. A more detailed discussion

The total energy of the universe consists of both radiation and matter.

As the Universe cooled, itwent from being radiationdominated to being matterdominated.

Dark energy becomes moreimportant as the Universeexpands.

27.1 Back to the Big Bang

Page 4: Chapter 27: The Early Universe - · PDF fileChapter 27: The Early Universe The plan: 1. A brief survey of the entire history of the big bang universe. 2. A more detailed discussion

In the very early Universe, one of the mostimportant processes was pair production:Virtual particles and photons were createdfrom the high-energy vacuum state, fromnothing. The temperature and densitywere trillions of times their current values.

The upper diagrams show how twogamma rays can unite to make anelectron–positron pair, and vice versa.Electron-positron pairs are matter-antimatter pairs, and annihilate, producinggamma rays again. These two processescome into balance, or equilibrium.

The lower picture is of such an eventoccurring at a high-energy particleaccelerator.

27.1 Back to the Big Bang

Page 5: Chapter 27: The Early Universe - · PDF fileChapter 27: The Early Universe The plan: 1. A brief survey of the entire history of the big bang universe. 2. A more detailed discussion

When the temperature haddecreased to about 1billion K, the photons nolonger had enough energyfor pair production, andwere “frozen out.” Thismeans the remainingphotons (still gamma rays)were now permanent,although still frequentlyscattered by the electronsin the surrounding gas.

We now see these photons, greatly redshifted,as the cosmic background radiation.

27.1 Back to the Big Bang

In the very earlyUniverse, the pairproduction andrecombinationprocesses were inequilibrium: Equalrates of productionand destruction, noparticle or photonpermanent.

Page 6: Chapter 27: The Early Universe - · PDF fileChapter 27: The Early Universe The plan: 1. A brief survey of the entire history of the big bang universe. 2. A more detailed discussion

This table lists the main events in the different epochs of the Universe. You don’t have tomemorize the numbers, or even all the epochs (I’ll tell you which ones are important toremember), but you should be able to read from the top to the bottom and understand itis a summary of the primary components of the universe at each time.

27.2 The Evolution of the Universe

Page 7: Chapter 27: The Early Universe - · PDF fileChapter 27: The Early Universe The plan: 1. A brief survey of the entire history of the big bang universe. 2. A more detailed discussion

Current understanding of the forcesbetween elementary particles is thatthey are accomplished by exchangeof a third particle.

Different forces “freeze out” whenthe energy of the Universe becomestoo low for the exchanged particle tobe formed through pair production.

27.2 The Evolution of the Universe

Page 8: Chapter 27: The Early Universe - · PDF fileChapter 27: The Early Universe The plan: 1. A brief survey of the entire history of the big bang universe. 2. A more detailed discussion

If we extrapolate the Big Bang back to the beginning, it yields a singularity—infinitedensity and temperature.

This result is probably artificial, reflecting our lack of understanding concerning matter attemperatures and densities so large that gravity had not yet “frozen out” from the otherforces. Any occurrence in physics or math of a “singularity,” where physical quantitiesappear to become infinite, is a sign of missing physics (or a mistake).

This is called the era of “quantum gravity,” when quantum effects and gravitational effectswere important on the same size scales.

This is the same reason we can’t say what happens when something falls into a black hole--another “singularity.”

We can only (hope we) understand what happens back to 10−43 seconds after the Big Bang.Therefore, we cannot predict anything about what happened before the Big Bang; indeed,the question may be meaningless. We don’t even understand whether “time” would havebeen relevant during these earliest of times, in which case talk of “before” and “afterwould not even make sense.

However a lot happens after that time, and theories of big bang cosmology predict certaincrucial events that can be observationally tested.

Time = 0 ? No singularity, just ignorance

Page 9: Chapter 27: The Early Universe - · PDF fileChapter 27: The Early Universe The plan: 1. A brief survey of the entire history of the big bang universe. 2. A more detailed discussion

This first 10−43 seconds after the Big Bang are called the Planck era.

This is called the era of “quantum gravity,” when quantum effects andgravitational effects were important on the same size scale. Therewere no separate forces.

At the end of that era, the gravitational force “freezes out” from allthe others, becomes separate. That is why today we can speak of“gravity” as if it acted independently from other forces.

Planck era, GUT era, …

The next era is the GUT (Grand Unified Theory) era. Here, the strongnuclear force, the weak nuclear force, and electromagnetism are allunified. At the end of it, there was not enough energy for thecorresponding production of heavy particles, and the forces (whichwere just one unified force before this time) became separate forces.

Page 10: Chapter 27: The Early Universe - · PDF fileChapter 27: The Early Universe The plan: 1. A brief survey of the entire history of the big bang universe. 2. A more detailed discussion

The next era is called the quark era; during this era all the elementaryparticles were in equilibrium with radiation.

About 10−4 s after the Big Bang, the Universe had cooled enough thatphotons could no longer produce the heavier elementary particles; the onlyones still in equilibrium were electrons, positrons, muons, and neutrinos.This is called the lepton era.

…quark era, lepton era

About 1 second after the Big Bang, the Universe became transparent toneutrinos. (Note: this is the equivalent of the era of recombination forphotons, to come much later; so there should be a “cosmic neutrinobackground” all around us, those same neutrinos from when theuniverse was 1 second old; no one has proposed a way to detect them.)

After 100 seconds, photons became too low in energy forelectron–positron pair creation—this marks the end of the radiationera, and the end of particle creation.

Page 11: Chapter 27: The Early Universe - · PDF fileChapter 27: The Early Universe The plan: 1. A brief survey of the entire history of the big bang universe. 2. A more detailed discussion

Epochs in cosmic historyThe evolution of the universe in a single graph--look at it slowly, especially as a reviewtool. Yellow and grey bands show how the density and temperature decreased as afunction of time (horizontal axis). Notice, on the bottom right, the transformation fromfundamental particles, to atoms, and finally to galaxies and stars.Meanwhile the mysterious “dark energy” has been increasing in importance.

Page 12: Chapter 27: The Early Universe - · PDF fileChapter 27: The Early Universe The plan: 1. A brief survey of the entire history of the big bang universe. 2. A more detailed discussion

The next major era occurs when photons no longer are able to ionize atoms assoon as they form. This allows the formation of hydrogen and helium atoms toform, taking out the free electrons. This “era of recombination,” about a millionyears after the big bang, frees the photons because their former interactions withelectrons no longer occur (the electrons are “recombined” in atoms).

The cosmic background radiation is then “frozen,” never to interact with matteragain, and available for observation by us. It contains an imprint of thevibrations or waves of spacetime that were to become galaxies and largerstructures.

This formation of cosmic structure from these waves probably took a tenth of abillion years or so. It had to wait until the temperatures in some regions haddropped low enough for gravity to dominate pressure.

For the next 3 billion years, galaxies begin to form. These correspond to thegalaxies we see at the highest redshifts (distances).

After that, they merge; larger and larger structures arise, galaxies evolve into theones we see now, and star formation goes through many generations.

The era of recombination releases the cosmic background radiation;formation of structure like galaxies follows

Page 13: Chapter 27: The Early Universe - · PDF fileChapter 27: The Early Universe The plan: 1. A brief survey of the entire history of the big bang universe. 2. A more detailed discussion

More Precisely 27-1: More on Fundamental ForcesYou do NOT have to know this terminology for the exam, except for the

four kinds of forces.Table 27-2 lists the four fundamental forces and the particles on which they act.There are six types of quarks (up, down, charm, strange, top, bottom) and sixtypes of leptons (electron, muon, tau, and neutrinos associated with each). Allmatter is made of quarks and leptons.

Dark matter is believed to be made of particles created when the universe wasvery young, but it is still “matter,” created by interactions of fundamentalparticles.

We don’t know where dark energy fits in at all, only that it probably exists.

Page 14: Chapter 27: The Early Universe - · PDF fileChapter 27: The Early Universe The plan: 1. A brief survey of the entire history of the big bang universe. 2. A more detailed discussion

More Precisely 27-1: More on Fundamental Forces(Again, not on exam--read for your own interest)

The theories of the weak and electromagnetic forces havebeen successfully unified in what is called the electroweaktheory. At a temperature of 1015 K, these forces should haveequal strength.

Considerable work has been done on unifying the strongand electroweak theories; these forces should have equalstrength at a temperature of 1028 K. One prediction of manysuch theories is supersymmetry—the idea that every knownparticle has a supersymmetric partner.

Page 15: Chapter 27: The Early Universe - · PDF fileChapter 27: The Early Universe The plan: 1. A brief survey of the entire history of the big bang universe. 2. A more detailed discussion

More Precisely 27-1: More on Fundamental Forces (cont’d)(Again, not on exam--read for your own interest)

Unification of the other three forces with gravity has beenproblematic. One theory that showed early promise is stringtheory—the idea that elementary particles are oscillations of littleloops of “string,” rather than being point particles. This avoids theunphysical results that arise when point particles interact. It does,however, require that the strings exist in 11-dimensional space.The extra seven dimensions are assumed to be very small.

Page 16: Chapter 27: The Early Universe - · PDF fileChapter 27: The Early Universe The plan: 1. A brief survey of the entire history of the big bang universe. 2. A more detailed discussion

Hydrogen was the first atomic nucleus to be formed, as it is just a proton, so itwas there from the very early time when particles as massive as protons werecreated.

Much later, a few minutes after the big bang, the average temperature of theuniverse fell to about a billion degrees, and for a short time temperatures wereright for nuclear fusion. This is the era of nucleosynthesis. However only oneelement was produced in appreciable quantities, helium.

Helium can form through fusion reactions that are just the proton-proton cyclethat occurs in stars:

2H + 1H → 3He + energy2H + 2H → 3He + neutron + energy

3He + neutron → 4He + energy

Your textbook has a great derivation of the fraction of He produced from protonsduring this era: 25 percent (by mass; 8 percent by number). It is difficult to get amuch different answer! This is a major prediction of big bang model. Everythingin the universe should have at least 25 percent helium. At the time it was made,no one was sure what the helium abundance was in, say, distant galaxies.Note: Helium is the only major element that was not primarily produced by fusion inside ofstars: stars produce only a few percent.

27.3 The Formation of Nuclei and AtomsThe era of nucleosynthesis

Page 17: Chapter 27: The Early Universe - · PDF fileChapter 27: The Early Universe The plan: 1. A brief survey of the entire history of the big bang universe. 2. A more detailed discussion

This diagram illustrates that fusion process: Note that it is not thesame as the fusion process that now goes on in the Sun’s core.

The Formation of Nuclei and Atoms

Page 18: Chapter 27: The Early Universe - · PDF fileChapter 27: The Early Universe The plan: 1. A brief survey of the entire history of the big bang universe. 2. A more detailed discussion

This would lead one to expect that ¼ of the mass of atomsin the universe would be helium, which is consistent withobservation (remembering that nucleosynthesis is ongoingin stellar cores).

The Formation of Nuclei and Atoms

Page 19: Chapter 27: The Early Universe - · PDF fileChapter 27: The Early Universe The plan: 1. A brief survey of the entire history of the big bang universe. 2. A more detailed discussion

Most deuterium fused into helium as soon as it wasformed, but some did not.

Deuterium is not formed in stars, so any deuteriumwe see today must be primordial.

This gives us a very sensitive way to estimate thepresent-day matter density of the universe.

Deuterium as a probe of “Omega”

Page 20: Chapter 27: The Early Universe - · PDF fileChapter 27: The Early Universe The plan: 1. A brief survey of the entire history of the big bang universe. 2. A more detailed discussion

As with galaxy measurements,the total matter densitydetermined by deuteriumabundance shows that thematter density is only a fewpercent of the critical density.

Today’s deuterium abundance tells us the averagedensity of baryonic matter in the universe.

Recall that we needed that in order to estimate “omega nought” in discussing the future ofthe universe and the shape of spacetime.

Page 21: Chapter 27: The Early Universe - · PDF fileChapter 27: The Early Universe The plan: 1. A brief survey of the entire history of the big bang universe. 2. A more detailed discussion

The time during which nucleiand electrons combined toform atoms is referred to asthe decoupling epoch. This iswhen the cosmic backgroundradiation originated.

The era of decoupling: nuclei become atoms, electrons are nolonger free, CBR “released” for us to see today

Page 22: Chapter 27: The Early Universe - · PDF fileChapter 27: The Early Universe The plan: 1. A brief survey of the entire history of the big bang universe. 2. A more detailed discussion

The horizon problem:When observed indiametrically oppositedirections from Earth,cosmic backgroundradiation appears the sameeven though there hasn’tbeen enough time sincethe Big Bang for them tobe in thermal contact.

27.4 The Inflationary Universe

Page 23: Chapter 27: The Early Universe - · PDF fileChapter 27: The Early Universe The plan: 1. A brief survey of the entire history of the big bang universe. 2. A more detailed discussion

The flatness problem: Inorder for the Universe tohave survived this long, itsdensity in the early stagesmust have differed from thecritical density by no morethan 1 part in 1015.

The Inflationary Universe

Page 24: Chapter 27: The Early Universe - · PDF fileChapter 27: The Early Universe The plan: 1. A brief survey of the entire history of the big bang universe. 2. A more detailed discussion

Between the GUT epochand the quark epoch, someparts of the Universe mayhave found themselvesstuck in the unifiedcondition longer than theyshould have been. Thisresulted in an extremeperiod of inflation, asshown on the graph.Between 10−35 s and 10−32

s, this part of the Universeexpanded by a factor of1050!

The Inflationary Universe

Page 25: Chapter 27: The Early Universe - · PDF fileChapter 27: The Early Universe The plan: 1. A brief survey of the entire history of the big bang universe. 2. A more detailed discussion

Inflation, if correct, would solve both the horizonand the flatness problems.

This diagram shows how the horizon problem issolved—the points diametrically opposite fromEarth were, in fact, in contact at one time:

The Inflationary Universe

Page 26: Chapter 27: The Early Universe - · PDF fileChapter 27: The Early Universe The plan: 1. A brief survey of the entire history of the big bang universe. 2. A more detailed discussion

The flatness problem is solved as well—after theinflation, the need to be exceedingly close to thecritical density is much more easily met:

The Inflationary Universe

Page 27: Chapter 27: The Early Universe - · PDF fileChapter 27: The Early Universe The plan: 1. A brief survey of the entire history of the big bang universe. 2. A more detailed discussion

Cosmologists realized that galaxies could not haveformed just from instabilities in normal matter:

• Before decoupling, background radiation keptclumps from forming.

• Variations in the density of matter beforedecoupling would have led to variations in thecosmic microwave background.

• Galaxies, or quasars, must have begun formingby a redshift of 6, and possibly as long ago as aredshift of 10 to 20.

27.5 The Formation of Structure in theUniverse

Page 28: Chapter 27: The Early Universe - · PDF fileChapter 27: The Early Universe The plan: 1. A brief survey of the entire history of the big bang universe. 2. A more detailed discussion

• Because of the overall expansion of the universe,any clumps formed by normal matter could onlyhave had 50–100 times the density of theirsurroundings.

Dark matter, being unaffected by radiation, wouldhave started clumping long before decoupling.

27.5 The Formation of Structure in theUniverse (cont.)

Page 29: Chapter 27: The Early Universe - · PDF fileChapter 27: The Early Universe The plan: 1. A brief survey of the entire history of the big bang universe. 2. A more detailed discussion

Galaxies could thenform around the dark-matter clumps,resulting in theUniverse we see.

27.5 The Formation of Structure in theUniverse

Page 30: Chapter 27: The Early Universe - · PDF fileChapter 27: The Early Universe The plan: 1. A brief survey of the entire history of the big bang universe. 2. A more detailed discussion

This figure is the result of simulations, beginningwith a mixture of 4% normal matter, 23% colddark matter, and 73% dark energy:

27.5 The Formation of Structure in theUniverse

Page 31: Chapter 27: The Early Universe - · PDF fileChapter 27: The Early Universe The plan: 1. A brief survey of the entire history of the big bang universe. 2. A more detailed discussion

Although dark matter does not interact directly withradiation, it will interact through the gravitationalforce, leading to tiny “ripples” in the cosmicbackground radiation.

These ripples havenow beenobserved.

27.6 Cosmic Structure and the MicrowaveBackground

Page 32: Chapter 27: The Early Universe - · PDF fileChapter 27: The Early Universe The plan: 1. A brief survey of the entire history of the big bang universe. 2. A more detailed discussion

This is a much higher-precision map of the cosmic background radiation,and the crowning achievement of current-day observational cosmology.

(Until the Planck telescope, just launched, collects its data…)

27.6 Cosmic Structure and the MicrowaveBackground

Page 33: Chapter 27: The Early Universe - · PDF fileChapter 27: The Early Universe The plan: 1. A brief survey of the entire history of the big bang universe. 2. A more detailed discussion

Here, the red dots are measurements derived from the data in the last image, andthe blue curve is a prediction for a universe with Ω0 = 1, showing excellentagreement. The placement of the large peak is particularly sensitive to Ω0. Noticethe secondary peaks, which are sensitive to additional combinations of parameters(like the age of the universe, and the contributions of dark energy and dark matter.

The strongest (and strangest) evidence that we live in a flat universe,and that inflation remains a likely (if bizarre) event that is

responsible for the existence of all structure in the universe

Page 34: Chapter 27: The Early Universe - · PDF fileChapter 27: The Early Universe The plan: 1. A brief survey of the entire history of the big bang universe. 2. A more detailed discussion

• At present the Universe is matter dominated; at itscreation it was radiation dominated.

• Matter was created by pair production.

• We do not understand the physics of the universebefore 10−43 seconds after it was created.

• Before that, we believe all four forces were unified.

• Gravity “froze out” first, then the strong force, thenthe weak and electromagnetic forces.

Summary of Chapter 27

Page 35: Chapter 27: The Early Universe - · PDF fileChapter 27: The Early Universe The plan: 1. A brief survey of the entire history of the big bang universe. 2. A more detailed discussion

• Most helium, and nearly all deuterium, in theUniverse was created during primordialnucleosynthesis.

• When the temperature became low enough foratoms to form, radiation and matter decoupled.

• The cosmic background radiation we see datesfrom that time.

• Horizon and flatness problems can be solved byinflation.

Summary of Chapter 27, (cont.)

Page 36: Chapter 27: The Early Universe - · PDF fileChapter 27: The Early Universe The plan: 1. A brief survey of the entire history of the big bang universe. 2. A more detailed discussion

• The density of the Universe appears to be thecritical density; 2/3 of the density comes fromdark energy, and dark matter makes up most ofthe rest.

• Structure of Universe today could not havecome from fluctuations in ordinary matter.

• Fluctuations in dark matter can account forwhat we see now.

Summary of Chapter 27 (cont.)