Dark Universe II Prof. Lynn Cominsky Dept. of Physics and Astronomy

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Dark Universe II Prof. Lynn Cominsky Dept. of Physics and Astronomy Sonoma State University

Dark Universe – Part II Is the universe "open" or "closed“ ? How does dark energy change our view of the history and future of the universe? 11/19/2018 Prof. Lynn Cominsky

Old view: Density of the Universe determines its destiny Wtotal = WM where WM = matter density (including regular and dark matter) Wtot = density/critical density If Wtot = 1,Universe is flat, expansion coasts to a halt as Universe is critically balanced. If Wtot > 1, Universe is closed, collapses on itself. If Wtot < 1, Universe is open, expands forever. 11/19/2018 Prof. Lynn Cominsky

Cosmological curvature W = density of the universe / critical density < 1 hyperbolic geometry W = 1 flat or Euclidean W > 1 spherical geometry The Pleiades contains over 3000 stars, is about 400 light years away, and only 13 light years across. Quite evident in the above photograph are the blue reflection nebulae that surround the bright cluster stars. Low mass, faint, brown dwarfs have recently been found in the Pleiades. 11/19/2018 Prof. Lynn Cominsky

New view: Density of the Universe SN data After inflation ends, Wtotal = WM + WL= 1.0 where Wtotal = density/critical density WM = matter density (including regular and dark matter) = 0.27 So therefore….. WL = cosmological constant or dark energy density = 0.73 U R here Perlmutter et al. 40 supernovae 11/19/2018 Prof. Lynn Cominsky

Today’s Cosmology WTOT = 1.0 from CMB measurements (WMAP). We live in a flat Universe. WM <0.3 from extensive observations at various wavelengths. Includes dark matter as well as normal matter and light. WL ~ 0.7 derived from Type Ia SN data combined with WMAP and other measurements. Hubble constant = 70 km/sec/Mpc from HST observations. Age of Universe = 13.7 billion years. Universe accelerates and is open, even though it is geometrically flat. 11/19/2018 Prof. Lynn Cominsky

“Geometry is not Destiny” – R. Kolb In the (old) standard picture, a flat Universe would expand more slowly with time, eventually coasting to a stop However, the SN data (and other data e.g., from clusters of galaxies) show that the expansion of the universe is actually accelerating This supports the existence of mass-energy with a strong negative pressure, such as the cosmological constant (L) originated by Einstein 11/19/2018 Prof. Lynn Cominsky

Dark Energy History Dark Energy must have been insignificant at early times, otherwise its gravitational influence would have made it almost impossible for ordinary matter to form stars, galaxies and large-scale structure In the early Universe, gravity dominated and various structures formed. However as the Universe expanded, and self-gravitating structures (such as clusters of galaxies, etc.) grew further apart, the space between them expanded, and dark energy began to dominate gravity 11/19/2018 Prof. Lynn Cominsky

Expansion History of the Universe HST (Riess et al.) found most distant Type 1a It was so far away that it occurred during the period when the expansion was still slowing down due to gravity from the galaxies in a smaller Universe Ann Feild (STScI) 11/19/2018 Prof. Lynn Cominsky

Expansion history of the Universe Other dimensions 11/19/2018 Prof. Lynn Cominsky Ann Feild (STScI)

History and fate of the Universe Data from Supernova Cosmology Project (LBL) Graphic by Barnett, Linder, Perlmutter & Smoot 11/19/2018 Prof. Lynn Cominsky

Resources Inflationary Universe by Alan Guth (Perseus) A Short History of the Universe by Joseph Silk (Scientific American Library) Before the Beginning by Martin Rees (Perseus) Inflation for Beginners (John Gribbin) http://www.biols.susx.ac.uk/Home/John_Gribbin/cosmo.htm Ned Wright’s Cosmology Tutorial http://www.astro.ucla.edu/~wright/cosmolog.htm 11/19/2018 Prof. Lynn Cominsky

Resources Physics Web quintessence http://physicsweb.org/article/world/13/11/8 Big Bang Cosmology Primer http://cosmology.berkeley.edu/Education/IUP/Big_Bang_Primer.html Martin White’s Cosmology Pages http://astron.berkeley.edu/~mwhite/darkmatter/bbn.html Lindsay Clark’s Curvature of Space http://www.astro.princeton.edu/~clark/teachersguide.html Before the Beginning by Martin Rees (Perseus) 11/19/2018 Prof. Lynn Cominsky

Backups follow 11/19/2018 Prof. Lynn Cominsky

Multiverses Universe was originally defined to include everything However, the possibility exists that our “bubble universe” is only one of many such regions that could have formed, with the parameters arranged as in the concordance model so that we can be here having this discussion Other universes could have very different physical conditions and we will never see them – they may be on different “branes” or in other dimensions that we cannot measure 11/19/2018 Prof. Lynn Cominsky

A Humbling Thought Not only do we not occupy a preferred place in our Universe, we may not occupy any preferred universe in the Multiverse! 11/19/2018 Prof. Lynn Cominsky

11/19/2018 Prof. Lynn Cominsky

Recall the Uncertainty Principle The uncertainty principle states that you cannot know both the position x and the momentum p of a particle more precisely than Planck’s constant h/2p  “h-bar” When dimensions are small, particles must therefore move in order to satisfy the uncertainty principle This motion creates a “zero point energy” > 0 Uncertainty Principle Dx Dp = h/2 11/19/2018 Prof. Lynn Cominsky

Uncertainty Principle Another version of the uncertainty principle relates the energy of a particle pair to lifetime This version explains the “virtual particles” that appear as quantum fluctuations They do not violate the uncertainty principle as long as their lifetimes are very short, and they are created in pairs which conserve charge, spin and other quantum properties Uncertainty Principle DE Dt = h/2 11/19/2018 Prof. Lynn Cominsky

Quantum fluctuations? Virtual particle pairs continually emerge and disappear into the quantum vacuum If you observe the particles (hit them with a photon), you give them enough energy to become real The particles can also get energy from any nearby force field (like a BH) 11/19/2018 Prof. Lynn Cominsky

The shape of the Universe The shape of the Universe is determined by a struggle between the momentum of expansion and the pull of gravity. The rate of expansion is determined by the Hubble Constant, Ho The strength of gravity depends on the density and pressure of the matter in the Universe. G is proportional to r + 3P r is the density and P is the pressure For normal matter, P is negligible, so the fate of a universe filled with normal matter is governed by the density r 11/19/2018 Prof. Lynn Cominsky

The fate of the Universe As the universe expands, the matter spreads out, with its density decreasing in inverse proportion to the volume. (V = 4pr3/3 for a sphere) The strength of the curvature effect decreases less rapidly, as the inverse of the surface area. (A = 4pr2 for a sphere) So, in the (pre-1998) standard picture of cosmology, geometry (curvature) ultimately gains control of the expansion of the universe. 11/19/2018 Prof. Lynn Cominsky

Properties of Dark Energy Einstein’s cosmological constant L has the property that P = - r = -1. Significant quantities of matter-energy with “negative pressure” will cause the expansion of the universe to accelerate. The quantity P/r = w is known as the “equation of state” parameter. Best measurements right now (WMAP and others) find that w = -1, consistent with the value expected for the “concordance model” aka L-CDM (cosmological constant + cold dark matter) 11/19/2018 Prof. Lynn Cominsky

Concordance Model From Spergel et al. 2006 Parameter Value Description Basic parameters H0          km s-1 Mpc-1 Hubble parameter Ωb               Baryon density Ωm             Total matter density Derived parameters ρ0                   kg/m3 Critical density ΩΛ Dark energy density t0                   years Age of the universe 11/19/2018 Prof. Lynn Cominsky

Vacuum Energy = Dark Energy? The cosmological constant L may be related to the “zero-point energy” of the Universe which comes from the quantum fluctuations of the vacuum. However, the vacuum energy density is 10120 too high to allow structure formation to occur Something must be canceling almost all of the vacuum energy in order for us to be here And that something must have arranged for the ~73% of critical density to be left over at our current time, 13.7 billion years later 11/19/2018 Prof. Lynn Cominsky

Quintessence Quintessence is another theory for dark energy that involves a dynamic, time-evolving and spatially dependent form of energy. It makes slightly different predictions for the acceleration It’s name refers to a “fifth essence” or force 11/19/2018 Prof. Lynn Cominsky

Gravity and pressure Relativistic G = r +3P P = r/3 G = 4r > 0 Non-relativistic G = r +3P P = 0 G = r > 0 L G = r +3P P = -r < 0 G = - 2r <0 Quintessence G = r +3P P = -2r/3 < 0 G = - r <0 11/19/2018 Prof. Lynn Cominsky