Alan Guth, Inflationary Cosmology: Is Our Universe Part of a Multiverse, AAA Lecture, November 6, 2009, p. 1.

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Alan Guth, Inflationary Cosmology: Is Our Universe Part of a Multiverse, AAA Lecture, November 6, 2009, p. 1. The Standard Big Bang What it is: Theory that the universe as we know it began 13-15 billion years ago. (Latest estimate: 13.7 ± 0.2 billion years!) Initial state was a hot, dense, uniform soup of particles that filled space uniformly, and was expanding rapidly. What it describes: How the early universe expanded and cooled How the light chemical elements formed How the matter congealed to form stars, galaxies, and clusters of galaxies Alan Guth Astronomers Association, November 6, 2009 1 Cosmic Inflation Inflation is a modification of the standard big bang theory, providing a very brief prequel. Inflation can explain the bang of the big bang (i.e, the outward propulsion), in terms of What it doesn't describe: What caused the expansion? (The big bang theory describes only the aftermath of the bang.) Where did the matter come from? (The theory assumes that all matter existed from the very beginning.) Miracle of Physics #1: Gravitational Repulsion! The combination of general relativity and modern particle theories predicts that, at very high energies, there exists forms of matter that create a gravitational repulsion! Alan Guth Astronomers Association, November 6, 2009 Alan Guth 2 Astronomers Association, November 6, 2009 3

Alan Guth, Inflationary Cosmology: Is Our Universe Part of a Multiverse, AAA Lecture, November 6, 2009, p. 2. Technical Note: Accordingto general relativity, a repulsive gravitational field is produced by a material with a negative pressure. Modern particle physics predicts that at high energies there exist states of matter with negative pressure in particular, states for which the energy is dominated by the potential energy of a scalar field. Inflation proposes that a patch of repulsive gravity material existed in the early universe for inflation at the grand unified theory scale ( 10 16 GeV), the patch needs to be only as large as 10 28 cm. (Since any such patch is enlarged fantastically by inflation, the initial density or probability of such patches can be very low.) The gravitational repulsion created by this material was the drivingforce behind the bigbang. The repulsion drove it into exponential expansion, doublingin size every 10 37 second or so! The patch expanded exponentially by a factor of at least 10 28 (65 time constants), but it could have expanded much more. Inflation lasted maybe 10 35 second, and at the end, the region destined to become the presently observed universe was about the size of amarble. The repulsive-gravity material is unstable, so it decayed like a radioactive substance, endinginflation. The decay released energy which produced ordinary particles, forming a hot, dense primordial soup. Standard cosmology began. Caveat: The decay happens in most places, but not everywhere we will come back to this SUBTLE point. Astronomers Association, November 6, 2009 4 Astronomers Association, November 6, 2009 5 The density of the repulsive gravity material was not lowered as it expanded! Although more and more mass/energy appeared as the repulsivegravity material expanded, total energy was conserved! Miracle of Physics #2: The energy of a gravitational field is negative! The positive energy of the repulsive gravity material was compensated by the negative energy of gravity. The TOTAL ENERGY of the universe may very well be zero. KEY SUCCESSES OF INFLATION Horizon/Homogeneity Problem: Can explain the observed uniformity of the universe. 1) Cosmic background radiation is uniform to 1 pt in 100,000. To achieve this uniformity without inflation, information and energy must travel 100 times the speed of light. SOLUTION: Uniformity is established in a tiny region before inflation, and then inflation magnifies this region to encompass the entire observed universe and more. Astronomers Association, November 6, 2009 6 Astronomers Association, November 6, 2009 7

Alan Guth, Inflationary Cosmology: Is Our Universe Part of a Multiverse, AAA Lecture, November 6, 2009, p. 3. 2) Flatness problem:" Why was the early universe so FLAT? What is meant by flat? Flat does not mean 2-dimensional. Flat means Euclidean, as opposed to the non-euclidean curved spaces that are also allowed by Einstein s general relativity. 3-dimensional curved spaces are hard to visualize, but they are analogous to the 2-dimensional curved surfaces shown on the right. Accordingto general relativity, the flatness of the universe is related to its mass density: Ω(Omega) = actual mass density critical mass density, where the critical density depends on the expansion rate. Ω = 1 is flat, Ω greater than 1 is closed, Ω less than 1 is open. Astronomers Association, November 6, 2009 8 Astronomers Association, November 6, 2009 9 A universe at the critical density is like a pencil balancingon its tip: If Ω in the early universe was slightly below 1, it would rapidly fall to zero and no galaxies would form. If Ω was slightly greater than 1, it would rapidly rise to infinity, the universe would recollapse, and no galaxies would form. To be as close to critical density as we measure today, at one second after the bigbang, Ω must have been equal to one to 15 decimal places! 10 Solution: Since inflation makes gravity become Inflationary repulsive, the evolution of Ω changes, too. Ω is driven towards one, extremely rapidly. It could begin at almost any value. Since the mechanism by which inflation explains the flatness of the early universe almost always overshoots, it predicts that even today the universe should have a critical density. Until 10 years ago, observation pointed to Ω 0.2 0.3. Latest observation by WMAP satellite (with 2DF and SDSS galaxy surveys, and supernova Ia observations): Ω = 1.0052 ± 0.0064 New ingredient: Dark Energy. In 1998 it was discovered that the expansion of the universe has been acceleratingfor about the last 5 billion years. The Dark Energy is the energy causing this to happen. of Technology Institute 11 Association, November 6, 2009 Astronomers

CMB: Comparison Theory of and CMB: Comparison Theory of and Alan Guth, Inflationary Cosmology: Is Our Universe Part of a Multiverse, AAA Lecture, November 6, 2009, p. 4. Density Fluctuation Problem: Can explain how the early universe 3) acquired very weak ripples in its mass density which later grew in intensity to form large scale structure (galaxies, clusters of galaxies, etc.) In inflationary models, these ripples arise from quantum fluctuations at the end of inflation. The quantum fluctuation model makes a generic prediction for the shape of the spectrum of the fluctuations. These predictions compare beautifully with the measurements of the cosmic background radiation. 12 13 Experiment Experiment Graph by Max Tegmark, for A. Guth & D. Kaiser, Science 307, 884 (Feb 11, 2005), updated to include WMAP 3-year data. Graph by Max Tegmark, for A. Guth & D. Kaiser, Science 307, 884 (Feb 11, 2005), updated to include WMAP 3-year data. Astronomers Association, November 6, 2009 14 Astronomers Association, November 6, 2009 15

ENERGY DARK Mystery of the Universe Key Alan Guth, Inflationary Cosmology: Is Our Universe Part of a Multiverse, AAA Lecture, November 6, 2009, p. 5. WMAP 5-YEAR FLUCTUATION SPECTRUM 2008 ACBAR, WMAP 3yr, BOOMERANG '03 Astronomers Association, November 6, 2009 16 Astronomers Association, November 6, 2009 17 In 1998, astronomers discovered that the universe has been acceleratingfor about the last 5 billion years (out of its 14 billion year history). IMPLICATION: Inflation is happeningtoday, so the universe today is filled with a repulsive gravity material. (Within general relativity, this requires negative pressure.) The repulsive gravity material, which apparently fills space, is called the Dark Energy. WHAT IS THE DARK ENERGY? Who knows? SIMPLEST EXPLANATION: Dark energy = vacuum energy, also known as a cosmological constant. of Technology 18 Institute Association, November 6, 2009 Astronomers The NIGHTMARE of DARK ENERGY The quantum vacuum is far from empty, so a nonzero energy density is no problem. In quantum field theory, the energy density of quantum fluctuations diverges. A plausible cutoff for the fluctuations is the Planck scale, E p 10 19 GeV, the scale of quantum gravity. Usingthis cutoff, the estimated vacuum energy density is too large It is too large by 120 orders of magnitude! Astronomers Association, November 6, 2009 19

Alan Guth, Inflationary Cosmology: Is Our Universe Part of a Multiverse, AAA Lecture, November 6, 2009, p. 6. The repulsive gravity material that drives the inflation is metastable. In any one location, the probability of remaining in an inflatingstate decreases with time usually exponentially. BUT, the universe in the meantime is expandingexponentially. In any successful version of inflation, the exponential expansion is faster than the exponential decay! Therefore, The volume that is inflatingincreases with time, even though the inflating material is decaying! The inflation becomes eternal once it starts, it never stops. The inflating region never disappears, but pieces of it undergo decay and produce pocket universes," ad infinitum. Instead of one universe, inflation produces an infinite number LANDSCAPE OF STRING THEORY THE Since the inception of stringtheory, theorists have sought to find the vacuum of stringtheory with no success. Within the past 10 years or so, most stringtheorists have come to the belief that there is no unique vacuum. Instead, there are maybe 10 500 long-lived metastable states, any of which could serve as a substrate for a pocket universe. This is the landscape! Eternal inflation can presumably produce an infinite number of pocket universes of every type, populatingthe landscape. Although string theory would govern everywhere, each type of vacuum would have its own low-energy physics its own standard model, its own constants of nature, etc. Universe to Multiverse 20 Astronomers Association, November 6, 2009 21 A Multiverse Selection Environmental The Anthropic Principle AKA: Consider, as an example, the local density of matter in which we find ourselves it is about 10 30 times larger than the mean density of the universe. Why is this so? Chance? Luck? Divine Providence? Most of us would presumably accept this as a selection effect: life can evolve only in those rare regions of the universe where the density of matter is unusually high. As early as 1987, Steve Weinbergpointed out that the cosmological constant might be explained in the same way. Maybe the cosmological constant IS huge in most pocket universes. Nonetheless, we must remember that a cosmological constant causes the expansion of the universe to accelerate. If negative, the universe quickly collapses. If large and positive, the universe flies apart before galaxies can form. It is plausible, therefore, that life can arise only if the cosmological constant is very near zero. In 1998 Martel, Shapiro, and Weinbergmade a serious calculation of the effect of the cosmological constant on galaxy formation. They found that to within a factor of order 5, they could explain why the cosmological constant is as small as what we measure. Astronomers Association, November 6, 2009 22 Astronomers Association, November 6, 2009 23

Alan Guth, Inflationary Cosmology: Is Our Universe Part of a Multiverse, AAA Lecture, November 6, 2009, p. 7. The Controversy A number of physicists regard these anthropic arguments as ridiculous. My recommendation is that the anthropic explanation (for anything) should be considered the explanation of last resort. Until we actually understand the landscape, and the initiation of life, we can only give plausibility arguments for anthropic explanations. Hence, the anthropic arguments only become attactive when the search for more deterministic explanations has failed, as so far is the case for the cosmological constant. (Anthropic explanations are also discussed for many other quantities, including the Higgs mass, the top quark mass, the magnitude of density perturbations.) 24 It Time to Accept Is Explanation of Last Resort? The guess is as good as mine! Your For the cosmological constant, because it seems so hard to explain any other way, it seems like it is time to strongly consider the selection-effect explanation. It is even hard to deny that, as of now, the selection-effect explanation is by far the most plausible that is known. Astronomers Association, November 6, 2009 25 SUMMARY The inflationary paradigm is in great shape! In earlier years, there was a widespread hope that eventually string theory would be able to predict the parameters of the standard model. From the point of view of theorists, this would be great. If the landscape picture is correct, it could be that all these values are determined, at least in part, by historical accidents which means that we have much less predictive power than we hoped. This is not the first time somethinglike this has happened. Kepler thought the radii of planetary orbits should be calculable from geometry. Now we treat planetary orbits as historical accidents. Inflation can explain why the universe is so smooth and homogenous when averaged over large regions, why its mass density is so close to the critical value, and it can also explain the ripples that we see in the cosmic background radiation. Almost all inflationary models are eternal into the future: multiverse of pocket universes. they produce a Stringtheorists mostly agree that stringtheory has no unique vacuum, but instead a landscape of perhaps 10 500 long-lived metastable states, any of which could be our vacuum. Eternal inflation can populate the stringtheory landscape. The combination provides a natural settingfor anthropic arguments: perhaps we see a small cosmological constant, for example, because conscious beings only form in those parts of the multiverse where the cosmological constant is small. The Disappointment Astronomers Association, November 6, 2009 26 Astronomers Association, November 6, 2009 27

Alan Guth, Inflationary Cosmology: Is Our Universe Part of a Multiverse, AAA Lecture, November 6, 2009, p. 8. Bottom Line: We have never had a model of the universe that works so well (homogeneity, mass density, spectrum of density fluctuations), orthat is so mysterious. Dark Energy Astronomers Association, November 6, 2009 28