30 The Early Universe Goals Goals 1 Introduce

30. The Early Universe Goals: Goals 1. Introduce the various concepts associated with studies of the early universe, despite questions about applicability. 2. Discuss the various simulations computed as models of the universe, asking the question “can cosmology be an observational science? ” 3. Present the various analyses of the cosmic microwave background as well as more recent related observations.

Your instructor is uncomfortable with much of this chapter of the textbook, for various reasons. Comments in the text such as: “Although the foregoing argument is only little better than a dimensional analysis…” “The moral is that specific predictions based on grand unified theories should be viewed with some caution. ” “This is the earliest time that can be probed experimentally. ” leave the impression of considerable uncertainty in what is being presented. So much is presented as background only.

Many cosmologists Your instructor

Subatomic Physics Background This section is best left as a reading exercise, although it is relevant to many of the ideas about the early universe.

There is perhaps undue concern about the existence of dark matter, either in “hot” form (relativistic particles, HDM) or “cold” form (CDM). The latter could simply consist of a high proportion of low mass stellar objects of low luminosity, brown dwarfs or stellar-mass black holes (MACHOs − massive compact halo objects) in the Galactic halo, although searches in the ’ 90 s found far fewer than predicted. Alternate candidates include WIMPs (weakly interacting massive particles) that interact with matter only through their gravitational effects. HDM is not favoured because of the difficulties of forming structure in the early universe, so most current models include both cold dark matter and a cosmological constant Λ, i. e. ΛCDM models. There is no guarantee that the real universe matches expectations from such models. Modellers can model just about anything, without regard to reality.

The Planck time is the only combination of fundamental constants with units of time, and is defined using Planck’s constant, the gravitational constant, and the speed of light: Another parameter arises from Heisenberg’s uncertainty principle, which is panned by Marmet. A black hole represents the most compact region within which mass can be contained, as defined by the Schwarzschild radius RS. So, for an uncertainty in position given by: the corresponding uncertainty in momentum is:

which implies a very large uncertainty in momentum for low-mass primordial black holes formed in the early universe. At the relativistic limit, E pc, so the uncertainty in energy is: which describes the approximate kinetic energy of such a black hole. The gravitational potential energy of such a hole is given by: The Planck mass corresponds to the limit where the sum of kinetic and potential energies is identically zero, i. e. :

and is therefore defined as: The Planck length is generated from the Schwarzschild radius: by neglecting the factor of “ 2” and inserting the Planck mass into the relation: although it is noted that such arguments are little more than dimensional analyses.

Various epochs in the early universe are characterized by transitions from one basic parameter to another.

It is an article of faith for physicists that before the Planck time the four fundamental forces of nature (gravity, electromagnetism, strong and weak nuclear forces) were merged, and separated through spontaneous symmetry breaking at that instant. Some physicists do not consider gravity as a force, e. g. Roy Bishop.

Problems with the Standard Model of the Big Bang Why is the CBR so smooth? This is known as the horizon problem, arising from the time when light decoupled from matter.

Why is the universe so nearly flat? This is known as the flatness problem, arising from the relationship considered earlier (example problems): If, at the time of decoupling when [z. WMAP] = 1089, the density parameter had been Ω = 0. 9991 rather than 1, then we would have Ω 0 = 0. 5 today. If, on the other hand, the density parameter had been as small as Ω = 0. 5 at that instant, then it would not be long before the density of the universe had decreased to a point where stars and galaxies could not be formed. It seems that a fine-tuning is required.

Why are there no magnetic monopoles? This is known as the monopole problem, Magnetic monopoles are a single magnetic charge, i. e. an isolated magnetic pole. It implies a lack of defects in the early universe in which magnetic monopoles might have been formed. Inflation. This concept dates from 1980, when Alan Guth proposed that in the first fraction of a second of the universe it spontaneously expanded at superluminal speed in such a fashion as to smooth out any initial irregularities in the distribution of matter. The concept does solve many of the problems described previously, but introduces one of its own, namely how to explain the introduction of a non-physical “fudge factor” to resolve problems arising from a physical analysis of the early universe.

An example of the concept of inflation in cosmology.

How the “scale factor” changes with time

Virtual particles and vacuum energy are used as possible explanations for the concept of inflation. See the discussion of the Casimir effect and virtual particles. Much of the discussion is governed by order of magnitude estimates, but the end result is the same: inflation does solve both the horizon problem and the flatness problem. See plots in Fig. 30. 4.

Matter-Antimatter Asymmetry Why is the universe dominated by matter instead of antimatter? Existing antiparticles are explained by highenergy collisions with normal matter, e. g. pair production (proton-antiproton pair) through the collision of two energetic protons or via rare ultra-high-energy cosmic rays. The discrepancy implies that the formation of matter particles was slightly more likely than the formation of antimatter particles in the early universe.

The Origin of Structure Presumably stars and galaxies formed from the existence of density inhomogeneities in the early universe that reached the Jean’s mass for a star or galaxy.

The textbook adopts the approach that many such inhomogeneities developed during the brief “inflationary” epoch, when baryonic matter was coupled with photons, the expansion being so rapid that the sizes of overdense and underdense regions vastly exceeded the particle horizon, inhibiting particle motion (Fig. 30. 6). In overdense regions ρ' > ρ, so the Hubble flow in such regions is described by: whereas: for the flat region of the surrounding universe. The equations can be combined to yield:

So that density fluctuations at that stage can be written as: During the radiation era: and the scale factor varied as: so the density fluctuations then must correlate with time and initial values in the radiation era as:

During the matter era, however: while the scale factor in a flat early universe varied as: so the density fluctuations must correlate with time and initial values during the matter era as: At some later time in the radiation era the particle horizon expanded to include the entire region of enhanced adiabatic density perturbation, making all parts of the region causally connected. The fate of such fluctuations then depended upon the relative values of their masses with respect to the Jean’s mass.

For a static (non-expanding) medium, the minimum mass required for the density fluctuation δρ/ρ to increase with time is the Jean’s mass: The same expression is valid in an expanding universe, although with different consequences for values falling below the above minimum. The expression can be rewritten using the speed of sound: and the adiabatic expression for pressure as a function of density: where C is a constant, and the ideal gas law.

Namely: with γ = 5/3 for an ideal monotonic gas. The expression for the Jean’s mass then becomes: The two density terms are different. Prior to recombination the numerator value of ρ corresponded to the baryonic mass density. During that era the temperatures of matter and radiation were equal, so:

The value of ρ in the denominator, however, is dominated by photons, so: and, prior to recombination: so the speed of sound was: The Jean’s mass at that time was therefore proportional to 1/T 3 until recombination.

The supposed variation of Jean’s mass with decreasing temperature T of the universe is depicted in Fig. 30. 7.

In the Big Bang model of cosmology, the formation of galaxies like the Milky Way occurred only after several previous stages in which the first stars were formed and galaxy mergers occurred.

Until recombination occurred, adiabatic density fluctuations in the early universe underwent acoustic oscillations much like pulsations in stars, with the sound waves traversing the medium at ~58% of light speed. Such oscillations produced regions of compression and rarefaction that were imprinted on the CMB when recombination occurred. Smaller adiabatic fluctuations did not survive that phase. The minimum mass required to survive damping by photon leakage can be estimated, and works out to be about 7. 7 × 1013 M , roughly the dimensions of a c. D galaxy or a rich cluster of galaxies. Following recombination, less massive density fluctuations existed from previously ”frozen” isothermal fluctuations unaffected by the dissipation effects of acoustic oscillations. The Jean’s mass at that time was about 1. 6 × 106 M , roughly the dimensions of a globular cluster.

The Gunn-Peterson trough in the Lyman-α forest for high redshift quasars, indicating less ionized H from z ~ 5 -6.

It has also been suggested that galaxy formation is biased towards regions of overdensity in the early universe. Former faculty member Michael West was one of the first to suggest the point. It would explain the separation of galaxy strands from galactic voids in the observable universe, which has been recognized for many years.

A Simple Model of Acoustic Oscillations Consider a simple cylinder of cross-sectional area A and length 2 L filled with gas (below). Let a movable piston be located in its centre. The equilibrium values of pressure and density are P 0 and ρ0, so that the mass of the piston is m = 2 LAρ0.

If the piston is displaced one way or the other, the density on one side will change by an amount Δρ accompanied by a pressure change of: where we can approximate: and: It follows that: Examine a displacement x of the piston, where the total mass of gas on either side does not change.

i. e. : likewise: So: Therefore, to first order:

The resulting equation of motion with Newton’s second law becomes: or: which, when simplified, becomes: The result is simple harmonic motion of the piston: with angular frequency:

If a gravitational field is now added in one direction, say the positive x-axis: The resulting equation of motion is: To solve this equation, set: So: which gives rise to simple harmonic motion with angular frequency ω = vs/L about y = 0, where the equilibrium position is:

It means that the compressions in region 2 along the direction of the gravitational field are of greater magnitude than the rarefactions in region 2. The equilibrium density in region 2 (i. e. when y = 0) is: The implication is that local concentrations of matter should fall inward rather than expand outward with the Hubble flow, i. e. collapsing initial configurations were preferred to expanding ones in the early universe. It is now possible to examine the angular power spectrum of the CMB and interpret the peaks and troughs in terms of fluctuations in the early universe.

The 3 K microwave background with the Doppler shift removed, as recorded by WMAP.

Given that

Sources: Wilkinson Microwave Anisotropy Probe (WMAP) Arcminute Cosmology Bolometer Array Receiver (ACBAR) BOOMERan. G experiment (Balloon Observations Of Millimetric Extragalactic Radiation ANd Geophysics) Cosmic Background Imager (CBI) Very Small Array (VSA) 65 experiments in total

The first peak is attributed to the compression of a large region (large L) that reached maximum compression at the time of decoupling. The first trough is attributed to a smaller region (smaller L) that began oscillating earlier, when it was sub-horizon sized. It could oscillate faster so it arrived with δT = 0 at the time of decoupling. The second peak (second harmonic) is attributed to oscillation of a still smaller region that reached maximum rarefaction at the time of decoupling. The relative heights of the first and second peaks is used to estimate the density of baryonic matter in the universe. The third peak (third harmonic) is assumed to arise from an oscillation reaching second compression at the time of decoupling. The superhorizon is attributed to a vast fluctuation that remained over the particle horizon until recombination.

Comparisons with model universes.

Potentials snags? The coincidence of high latitude nearby atomic hydrogen clouds (i. e. mapped in 21 -cm radiation) noted by Gerrit Verschuur in several papers. “Echoes of the Big Bang Misinterpreted? ” Seeing is believing, except when you don’t believe what you see. That is according to veteran radio astronomer Gerrit Verschuur, of the University of Memphis, who has an outrageously unorthodox theory that, if true, would turn modern cosmology upside down. He proposes that at least some of the fine structure seen in the all-sky plot of the universe’s cosmic microwave background is really the imprint of our local interstellar neighborhood. It has nothing to do with how the universe looked 380, 000 years after the Big Bang, but how nearby clouds of cold hydrogen looked a few hundred years ago.

The idea is so unbelievable that it is little wonder that cosmologists have largely ignored his work that has been published over the last few years. “Science is supposed to be about the excitement of making new discoveries. But this discovery terrifies me, ” he told reporters at the recent meeting of the American Astronomical Society in Anchorage, Alaska. Verschuur’s radio maps of hydrogen surrounding our local stellar neighborhood out to a few hundred lightyears appear to have an uncanny match-up to the mottled structure of the cosmic microwave background that is 13. 7 billion light-years away. NASA’s Wilkinson Microwave Anisotropy Probe (WMAP) mapped the CMB in exquisite detail in 2003, revealing slight temperature fluctuations in the early universe believed to be the seeds of galaxy formation. It is a landmark observation that is considered the “blueprint” for the subsequent evolution of the universe.

Verschuur is quick to applaud the WMAP team for a “brilliant experiment” to attempt to resolve the structure of the primeval universe as encoded in ancient microwave radiation. But he suggests that the team failed to subtract all the foreground radio phenomena that may have contaminated the data. In a moment of serendipity, Verschuur found that his contour radio maps of cold hydrogen in interstellar space seem to fit the false-colour speckled microwave background pattern. It is like a child putting a puzzle piece into a pre-shaped slot. Peaks in the foreground radio emission appear to overlay the peaks in the warmest region of the background, or slightly offset at best. In 2007 and 2010 Verschuur published a list of over 100 apparent matches between the CMB pattern and his interstellar hydrogen pattern.

Verschuur would have dismissed it as an odd coincidence until he realized that small interstellar clouds of hydrogen collide and jostle electrons to generate high-frequency radio emissions. Like other foreground sources they would overlay the CMB. Because the WMAP team did not consider or know about the contribution of such a phenomenon, they did not try to subtract it as they did when removing numerous other electromagnetic “contaminants” in their data reduction, says Verschuur. If Verschuur’s theory is correct, the consequences would send seismic waves through the cosmology community. It implies that at least some of the small-scale structure in the CMB map does not exist at all.

But hold on. Detailed analysis of the angular diameter of CMB blobs yield a power spectrum that exactly fits theoretical predictions. The first peak in the spectrum shows a geometrically flat universe. The next peak determines the density of normal matter. The third peak provides information about the density of dark matter. And it all fits together beautifully. Verschuur shrugs off the interpretation, saying that astronomers can analyze the data and then stop when, “they find what they are looking for. ” Cosmologists have also said that Verschuur’s claim needs a detailed statistical analysis. But Verschuur is equally dismissive: “astronomers who study interstellar structure do not use statistics to show associations between different forms of matter … they go by what the data look like. ”

Others:

Astrophysicists Kate Land Anze Slosar conducted an analysis of Verschuur’s study published in the Dec. 10, 2007, edition of The Astrophysical Journal. In an email they concluded that Verschuur’s correlation of the radio emissions from nearby hydrogen and the WMAP data was nothing more than a coincidence. “Notoriously, by eye, one can often think they see correlations between patterns, ” Land explained. “But one does not truly see the anti-correlations. So two maps (of the sky) that just fluctuate randomly can appear correlated. ” It would not be the first time that random fluctuations in the CMB have led researchers to claim that they have seen patterns, only for their claims to be refuted and found flawed.

Observations from the European Space Agency’s Planck mission that is now measuring the CMB promises to yield a more detailed all-sky map than WMAP. If the datasets between the missions agree at some level, it would rule out Verschuur’s claim as simply an over-interpretation of his radio observations — agreeing with Land’s 2007 rebuttal. However, if Verschuur is right, WMAP cosmologists might not have seen the forest for the trees. Actually, the Land & Slosar article was published in Phys. Rev. D, 76. 087301, 2007, not Ap. J, and Verschuur was aware of the article when he wrote subsequent papers on the controversy. The comparison was also made with respect to a different H I survey than that used by Verschuur.

There are interesting details in the Land & Sloser article, namely that one can spot Stephen Hawking’s initials in the WMAP images at (l, b) = (60°, 10°).

Prominent in the WMAP images is the clumping of cool dust along the Magellanic Stream.

Resolution differences in the maps.

Further analysis of WMAP.

Other evidence: the concordance of results from different cosmological experiments.

Details are in the smaller peaks displaying polarization.

Results from Planck.

Planck angular power spectrum.

Planck best fit ΛCDM model.

Sample Question 1. Chapter 9 derives a value for the number density of black body photons: Use that result with the baryon density ρb, 0 to estimate the proportion of baryons to photons in the present universe. Assume for convenience that the universe is composed entirely of hydrogen. Answer: With T = 2. 725 K the present number density of black body photons is:

The present number density of baryons composed of pure hydrogen is: The ratio of the two is: or roughly 1. 6 billion photons for every baryon in the universe. Would the universe be closed if photons had a small amount of mass?

Chibisov (1976, Sov. Phys. Usp. , 19, 624) proposed an upper limit on the mass of the photon of: using wisps in the Crab Nebula and other cosmic indicators. Bartlett (2010) proposes a slightly larger mass of: in order for photons to have a Compton wavelength of 400 pc, matching the spacing he proposes in his cosinusoidal model of the Galaxy. Note that both values are at least 30 orders of magnitude smaller than the electron mass, unlikely to be enough to close the universe.