The Hubble Constant and the Expanding Universe

Total Page:16

File Type:pdf, Size:1020Kb

The Hubble Constant and the Expanding Universe A reprint from American Scientist the magazine of Sigma Xi, The Scientific Research Society This reprint is provided for personal and noncommercial use. For any other use, please send a request to Permissions, American Scientist, P.O. Box 13975, Research Triangle Park, NC, 27709, U.S.A., or by electronic mail to [email protected]. ©Sigma Xi, The Scientific Research Society and other rightsholders The Hubble Constant and the Expanding Universe A newly refined value of H0, the expansion rate of the universe, may herald a first step toward a new era of “precision“ cosmology Wendy Freedman may hold the distinction of being the fort. The goal of our work is nothing when the American astronomer Edwin Ionly astronomer to have been trapped less than trying to understand the for- Hubble discovered that our universe is in a cage at the top of a large telescope on mation and evolution of the universe. indeed expanding. He showed that the the 14,000-foot summit of Mauna Kea. (I We do this through observations and farther a galaxy is from us, the faster it know another astronomer who once fell experiments that ultimately provide is speeding away. This velocity- out of such a cage, but that is another sto- numbers as answers—the values of distance relation came to be called ry.) Twenty years ago, before most ob- cosmological parameters. These num- Hubble’s law, and the value that de- servers spent their nights in warm com- bers can tell us something important scribes its current rate of expansion is puter rooms, astronomers commonly about the universe: how much matter H0. Hubble was the first to measure H0 observed in very small cages at the there is, whether the universe is curved (which wasn’t named as such at the prime focus of giant telescopes. Al- or flat, and even how it might all end. time)—deriving a value of 500 kilome- though the long winter nights were al- Understanding the significance of these ters per second per megaparsec. (A most unbearably cold, we had spectacu- numbers and this curious cosmological parsec is equal to 3.26 light-years.) For lar views of the dark night sky, and we quest for parameters requires a brief di- various reasons, Hubble’s result was listened to music through headphones as version into some history. far off the mark, but even a couple of we recorded images and spectra of our The modern science of cosmology is years ago, estimates for H0 varied by a celestial targets. At the end of one night, founded on general relativity—Albert factor of two, generally ranging be- a faulty telescope position caused an ele- Einstein’s theory of gravity—whose tween 50 and 100 (the values are usual- vator to jam, making it impossible for me equations describe the global behavior ly stated without the units of measure). to leave the cage. This was no small in- of matter and energy, and space and This lack of precision was problem- convenience—the closest restroom time. Some solutions to these equa- atic because H0 is a key parameter was 40 feet below, and I was unpleas- tions, notably those devised by the needed to estimate both the age and antly confined within two snowsuits. Russian mathematician Alexander size of the universe. A twofold range in It was another seven hours before a Friedmann in the 1920s, suggest that H0 yields an unacceptably wide span group of engineers arrived from sea the universe originated from a very for the age of the universe—anywhere level (delayed by a flat tire), climbed hot, very dense state in a “big bang“ from 10 to 20 billion years. Such uncer- up the side of the telescope’s dome explosion and that it has been expand- tainty also puts few constraints on cos- and finally pried the elevator free with ing in size ever since. The dynamics of mological models. a crowbar. Now why would an as- the expansion are expressed by the so- But all of this is changing. The value tronomer want to subject herself to called Friedmann equation, which de- of the H0, along with some other cos- such indignities? scribes the evolution of the universe in mological parameters, is becoming in- As an observational cosmologist, I terms of its density and geometry (see creasingly accessible to accurate mea- can say that the rewards more than “Friedmann’s Equation and Cosmological surement as new technologies allow us compensate for the occasional discom- Parameters,” page 42). Applying Fried- to see farther into the universe than mann’s equation requires that we ever before. The Hubble Space Tele- Wendy Freedman is an astronomer at the Carnegie know something about a few parame- scope (HST), which was launched in Observatories in Pasadena, California. Her re- ters it contains—such as H, the Hubble 1990, is among these technological search interests include the evolution of galaxies parameter, which defines the expan- breakthroughs. One of the primary rea- and their stellar populations, and the extragalactic sion rate; Ω , the mass density of the sons the HST was built was to deter- distance scale and cosmology. She was recently m universe; and Ω , the curvature of the mine a more accurate value for H . elected a Fellow of the American Academy of Sci- k 0 ences, and this year was awarded the Magellanic universe. These numbers are not inher- This “Key Project” of the HST program Premium Award of the American Philosophical ently defined by the equation. Instead, was an enormous effort, involving 30 Society. Address: Carnegie Observatories, 813 they remain for us to measure. astronomers (I was one of three co- Santa Barbara Street, Pasadena, CA 91101. Inter- Some of the first efforts to make leaders), spanning eight years of work net: [email protected] these measurements date back to 1929, and about 1,000 hours of HST time. It © 2004 Sigma Xi, The Scientific Research Society. Reproduction 36 American Scientist, Volume 91 with permission only. Contact [email protected]. Figure 1. Spiral galaxy NGC 4414 is speeding away from us as it is carried by the expansion of the universe. The rate at which the universe is ex- panding, described by the Hubble constant, is determined simply by measuring the velocities and distances of galaxies. In practice, however, making accurate measurements to distant galaxies can be extremely difficult. The launch of the Hubble Space Telescope in 1990 made such mea- surements much easier, allowing astronomers to determine the distances to galaxies with an unprecedented level of accuracy. After nearly a decade of measurements, astronomers have derived a value for the Hubble constant that is accurate enough to be used meaningfully in various cosmological and astrophysical calculations. NGC 4414 is nearly 19.1 megaparsecs away (roughly 62 million light-years), and it is receding from us with a speed of about 1,400 kilometers per second. (Image courtesy of NASA, Hubble Heritage Team, STSci/AURA and Wendy Freedman.) was the largest project tackled by HST ing universe and this effect must be ac- number of galaxies distributed across in its first decade, and it was finally counted for or minimized. the sky so that the peculiar motions completed in 2001. A galaxy’s velocity is calculated can be averaged out. from the observed shift of lines in its Measuring distances presents a A Variable and a Constant spectrum (the pattern of electromag- greater challenge. The universe is so In principle, the Hubble constant netic radiation it emits at different large that there is no direct way to should be a straightforward calcula- wavelengths). Galaxies that are mov- measure its full size. There is no cos- tion. It only requires the measurement ing away from us emit light that is mological equivalent to a land survey- of a galaxy’s distance and velocity. In shifted to longer (redder) wavelengths or’s rangefinder—no single method practice, however, devising a method because it is stretched, or “redshifted,” can provide a measure of the uni- to measure distances over cosmologi- by the recession. The greater the shift verse’s absolute size. Instead, as- cal scales is far from trivial. Even rela- in wavelength, the faster the galaxy’s tronomers rely on a series of tech- tively simple velocity measurements velocity. Since the velocity of recession niques, each of which is suitable for a are complicated by the fact that galax- is proportional to its distance (Hub- certain range of distances, and together ies tend to have other galaxies as ble’s law again), the farther the dis- these methods constitute the “cosmo- neighbors, and so they interact gravita- tance measurements can be made, the logical distance ladder.” tionally, perturbing one another’s mo- smaller the proportional impact of pe- For the nearest stars, distances can tions. These peculiar velocities are dis- culiar velocities on the overall expan- be measured by trigonometric parallax, tinct from the recession velocities (the sion velocity. Astronomers can further which uses the baseline of the Earth’s Hubble flow) of galaxies in the expand- reduce the uncertainty by observing a orbit for triangulating a star’s distance © 2004 Sigma Xi, The Scientific Research Society. Reproduction with permission only. Contact [email protected]. 2003 January–February 37 A Distant Candle in the Dark luminosity faint bright a Cepheid’s periodicity Cepheid period-luminosity relation time (days) 131030 100 period (days) Cepheids are massive stars (at least three times greater than the Sun) that have reached an unstable point in their evolution. During the Cepheid phase, the outer atmospheres of these stars pulsate—changing in size and color (left)—and therefore in their brightness, or luminosity, over a very regular period, ranging from 2 to more than 100 days.
Recommended publications
  • The Age of the Universe Transcript
    The Age of the Universe Transcript Date: Wednesday, 6 February 2013 - 1:00PM Location: Museum of London 6 February 2013 The Age of The Universe Professor Carolin Crawford Introduction The idea that the Universe might have an age is a relatively new concept, one that became recognised only during the past century. Even as it became understood that individual objects, such as stars, have finite lives surrounded by a birth and an end, the encompassing cosmos was always regarded as a static and eternal framework. The change in our thinking has underpinned cosmology, the science concerned with the structure and the evolution of the Universe as a whole. Before we turn to the whole cosmos then, let us start our story nearer to home, with the difficulty of solving what might appear a simpler problem, determining the age of the Earth. Age of the Earth The fact that our planet has evolved at all arose predominantly from the work of 19th century geologists, and in particular, the understanding of how sedimentary rocks had been set down as an accumulation of layers over extraordinarily long periods of time. The remains of creatures trapped in these layers as fossils clearly did not resemble any currently living, but there was disagreement about how long a time had passed since they had died. The cooling earth The first attempt to age the Earth based on physics rather than geology came from Lord Kelvin at the end of the 19th Century. Assuming that the whole planet would have started from a completely molten state, he then calculated how long it would take for the surface layers of Earth to cool to their present temperature.
    [Show full text]
  • Hubble's Law and the Expanding Universe
    COMMENTARY COMMENTARY Hubble’s Law and the expanding universe Neta A. Bahcall1 the expansion rate is constant in all direc- Department of Astrophysical Sciences, Princeton University, Princeton, NJ 08544 tions at any given time, this rate changes with time throughout the life of the uni- verse. When expressed as a function of cos- In one of the most famous classic papers presented the observational evidence for one H t in the annals of science, Edwin Hubble’s of science’s greatest discoveries—the expand- mic time, ( ), it is known as the Hubble 1929 PNAS article on the observed relation inguniverse.Hubbleshowedthatgalaxiesare Parameter. The expansion rate at the pres- between distance and recession velocity of receding away from us with a velocity that is ent time, Ho, is about 70 km/s/Mpc (where 1 Mpc = 106 parsec = 3.26 × 106 light-y). galaxies—the Hubble Law—unveiled the proportional to their distance from us: more The inverse of the Hubble Constant is the expanding universe and forever changed our distant galaxies recede faster than nearby gal- Hubble Time, tH = d/v = 1/H ; it reflects understanding of the cosmos. It inaugurated axies. Hubble’s classic graph of the observed o the time since a linear cosmic expansion has the field of observational cosmology that has velocity vs. distance for nearby galaxies is begun (extrapolating a linear Hubble Law uncovered an amazingly vast universe that presented in Fig. 1; this graph has become back to time t = 0); it is thus related to has been expanding and evolving for 14 bil- a scientific landmark that is regularly repro- the age of the Universe from the Big-Bang lion years and contains dark matter, dark duced in astronomy textbooks.
    [Show full text]
  • The Reionization of Cosmic Hydrogen by the First Galaxies Abstract 1
    David Goodstein’s Cosmology Book The Reionization of Cosmic Hydrogen by the First Galaxies Abraham Loeb Department of Astronomy, Harvard University, 60 Garden St., Cambridge MA, 02138 Abstract Cosmology is by now a mature experimental science. We are privileged to live at a time when the story of genesis (how the Universe started and developed) can be critically explored by direct observations. Looking deep into the Universe through powerful telescopes, we can see images of the Universe when it was younger because of the finite time it takes light to travel to us from distant sources. Existing data sets include an image of the Universe when it was 0.4 million years old (in the form of the cosmic microwave background), as well as images of individual galaxies when the Universe was older than a billion years. But there is a serious challenge: in between these two epochs was a period when the Universe was dark, stars had not yet formed, and the cosmic microwave background no longer traced the distribution of matter. And this is precisely the most interesting period, when the primordial soup evolved into the rich zoo of objects we now see. The observers are moving ahead along several fronts. The first involves the construction of large infrared telescopes on the ground and in space, that will provide us with new photos of the first galaxies. Current plans include ground-based telescopes which are 24-42 meter in diameter, and NASA’s successor to the Hubble Space Telescope, called the James Webb Space Telescope. In addition, several observational groups around the globe are constructing radio arrays that will be capable of mapping the three-dimensional distribution of cosmic hydrogen in the infant Universe.
    [Show full text]
  • Galaxies at High Redshift Mauro Giavalisco
    eaa.iop.org DOI: 10.1888/0333750888/1669 Galaxies at High Redshift Mauro Giavalisco From Encyclopedia of Astronomy & Astrophysics P. Murdin © IOP Publishing Ltd 2006 ISBN: 0333750888 Institute of Physics Publishing Bristol and Philadelphia Downloaded on Thu Mar 02 23:08:45 GMT 2006 [131.215.103.76] Terms and Conditions Galaxies at High Redshift E NCYCLOPEDIA OF A STRONOMY AND A STROPHYSICS Galaxies at High Redshift that is progressively higher for objects that are separated in space by larger distances. If the recession velocity between Galaxies at high REDSHIFT are very distant galaxies and, two objects is small compared with the speed of light, since light propagates through space at a finite speed of its value is directly proportional to the distance between approximately 300 000 km s−1, they appear to an observer them, namely v = H d on the Earth as they were in a very remote past, when r 0 the light departed them, carrying information on their H properties at that time. Observations of objects with very where the constant of proportionality 0 is called the high redshifts play a central role in cosmology because ‘HUBBLE CONSTANT’. For larger recession velocities this they provide insight into the epochs and the mechanisms relation is replaced by a more general one calculated from the theory of general relativity. In each cases, the value of GALAXY FORMATION, if one can reach redshifts that are high H enough to correspond to the cosmic epochs when galaxies of 0 provides the recession velocity of a pair of galaxies were forming their first populations of stars and began to separated by unitary distance, and hence sets the rate of shine light throughout space.
    [Show full text]
  • The Anthropic Principle and Multiple Universe Hypotheses Oren Kreps
    The Anthropic Principle and Multiple Universe Hypotheses Oren Kreps Contents Abstract ........................................................................................................................................... 1 Introduction ..................................................................................................................................... 1 Section 1: The Fine-Tuning Argument and the Anthropic Principle .............................................. 3 The Improbability of a Life-Sustaining Universe ....................................................................... 3 Does God Explain Fine-Tuning? ................................................................................................ 4 The Anthropic Principle .............................................................................................................. 7 The Multiverse Premise ............................................................................................................ 10 Three Classes of Coincidence ................................................................................................... 13 Can The Existence of Sapient Life Justify the Multiverse? ...................................................... 16 How unlikely is fine-tuning? .................................................................................................... 17 Section 2: Multiverse Theories ..................................................................................................... 18 Many universes or all possible
    [Show full text]
  • Year 1 Cosmology Results from the Dark Energy Survey
    Year 1 Cosmology Results from the Dark Energy Survey Elisabeth Krause on behalf of the Dark Energy Survey collaboration TeVPA 2017, Columbus OH Our Simple Universe On large scales, the Universe can be modeled with remarkably few parameters age of the Universe geometry of space density of atoms density of matter amplitude of fluctuations scale dependence of fluctuations [of course, details often not quite as simple] Our Puzzling Universe Ordinary Matter “Dark Energy” accelerates the expansion 5% dominates the total energy density smoothly distributed 25% acceleration first measured by SN 1998 “Dark Matter” 70% Our Puzzling Universe Ordinary Matter “Dark Energy” accelerates the expansion 5% dominates the total energy density smoothly distributed 25% acceleration first measured by SN 1998 “Dark Matter” next frontier: understand cosmological constant Λ: w ≡P/ϱ=-1? 70% magnitude of Λ very surprising dynamic dark energy varying in time and space, w(a)? breakdown of GR? Theoretical Alternatives to Dark Energy Many new DE/modified gravity theories developed over last decades Most can be categorized based on how they break GR: The only local, second-order gravitational field equations that can be derived from a four-dimensional action that is constructed solely from the metric tensor, and admitting Bianchi identities, are GR + Λ. Lovelock’s theorem (1969) [subject to viability conditions] Theoretical Alternatives to Dark Energy Many new DE/modified gravity theories developed over last decades Most can be categorized based on how they break GR: The only local, second-order gravitational field equations that can be derived from a four-dimensional action that is constructed solely from the metric tensor, and admitting Bianchi identities, are GR + Λ.
    [Show full text]
  • Cosmic Microwave Background
    1 29. Cosmic Microwave Background 29. Cosmic Microwave Background Revised August 2019 by D. Scott (U. of British Columbia) and G.F. Smoot (HKUST; Paris U.; UC Berkeley; LBNL). 29.1 Introduction The energy content in electromagnetic radiation from beyond our Galaxy is dominated by the cosmic microwave background (CMB), discovered in 1965 [1]. The spectrum of the CMB is well described by a blackbody function with T = 2.7255 K. This spectral form is a main supporting pillar of the hot Big Bang model for the Universe. The lack of any observed deviations from a 7 blackbody spectrum constrains physical processes over cosmic history at redshifts z ∼< 10 (see earlier versions of this review). Currently the key CMB observable is the angular variation in temperature (or intensity) corre- lations, and to a growing extent polarization [2–4]. Since the first detection of these anisotropies by the Cosmic Background Explorer (COBE) satellite [5], there has been intense activity to map the sky at increasing levels of sensitivity and angular resolution by ground-based and balloon-borne measurements. These were joined in 2003 by the first results from NASA’s Wilkinson Microwave Anisotropy Probe (WMAP)[6], which were improved upon by analyses of data added every 2 years, culminating in the 9-year results [7]. In 2013 we had the first results [8] from the third generation CMB satellite, ESA’s Planck mission [9,10], which were enhanced by results from the 2015 Planck data release [11, 12], and then the final 2018 Planck data release [13, 14]. Additionally, CMB an- isotropies have been extended to smaller angular scales by ground-based experiments, particularly the Atacama Cosmology Telescope (ACT) [15] and the South Pole Telescope (SPT) [16].
    [Show full text]
  • Arxiv:2002.11464V1 [Physics.Gen-Ph] 13 Feb 2020 a Function of the Angles Θ and Φ in the Sky Is Shown in Fig
    Flat Space, Dark Energy, and the Cosmic Microwave Background Kevin Cahill Department of Physics and Astronomy University of New Mexico Albuquerque, New Mexico 87106 (Dated: February 27, 2020) This paper reviews some of the results of the Planck collaboration and shows how to compute the distance from the surface of last scattering, the distance from the farthest object that will ever be observed, and the maximum radius of a density fluctuation in the plasma of the CMB. It then explains how these distances together with well-known astronomical facts imply that space is flat or nearly flat and that dark energy is 69% of the energy of the universe. I. COSMIC MICROWAVE BACKGROUND RADIATION The cosmic microwave background (CMB) was predicted by Gamow in 1948 [1], estimated to be at a temperature of 5 K by Alpher and Herman in 1950 [2], and discovered by Penzias and Wilson in 1965 [3]. It has been observed in increasing detail by Roll and Wilkinson in 1966 [4], by the Cosmic Background Explorer (COBE) collaboration in 1989{1993 [5, 6], by the Wilkinson Microwave Anisotropy Probe (WMAP) collaboration in 2001{2013 [7, 8], and by the Planck collaboration in 2009{2019 [9{12]. The Planck collaboration measured CMB radiation at nine frequencies from 30 to 857 6 GHz by using a satellite at the Lagrange point L2 in the Earth's shadow some 1.5 10 km × farther from the Sun [11, 12]. Their plot of the temperature T (θ; φ) of the CMB radiation as arXiv:2002.11464v1 [physics.gen-ph] 13 Feb 2020 a function of the angles θ and φ in the sky is shown in Fig.
    [Show full text]
  • Lecture 14: the Age of the Universe
    The Age of the Universe One somewhat low-pro¯le but important test of cosmological models is that the age of the universe implied by the models agrees with the age estimated using various methods. Here we'll talk about the age we get from models, and in the next lecture will discuss several observational handles on the true age. For a change of pace, and to give us some practice in evaluating complicated equations, we will start with the equation for the lookback time provided by Hogg in astro-ph/9905116, and see whether the units, limits, etc. make sense. The lookback time from now (z = 0) back to redshift z means the time that would have elapsed on the wristwatch of an observer moving with the Hubble ow between those redshifts. Hogg's expression is: 1 z dz0 tL = 0 0 3 0 2 : (1) H0 Z0 (1 + z ) ­(1 + z ) + ­k(1 + z ) + ­¤ p Here H0 is the current value of the Hubble parameter, and ­, ­k, and ­¤ each indicate their current (z = 0) values. Does this expression behave as it should? See Figure 1 for a graphical representation. As always, we check units ¯rst. Recall that the Hubble parameter has units of inverse time, so the prefactor 1=H0 has units of time. The integral is dimensionless because the redshift is, so indeed the units are correct. Our second easy check is to note that tL must increase with increasing z. Since the integrand is always positive, this is indeed the case. Our third simple check is to note that smaller H0 should imply a larger time back to a given redshift, because H0 = a=a_ today.
    [Show full text]
  • The Hubble Constant
    Astro-2: History of the Universe Lecture 3; April 11 2013 Previously.. On Astro-2 • The universe is much larger than the Milky Way (Gpc vs kpc) • There are billion of galaxies, the Milky Way is average Joe galaxy • Most galaxies can be classified based on their appearance as – Elliptical – Lenticular – Spiral – Irregular • Spirals rotate and have young stars, gas and dust • Ellipticals do not rotate and have old stars, no gas nor dust Previously.. On Astro-2 • It is difficult but very important to figure out the size and distance of things in the universe • One way astronomers do that is by using “standard candles”. • Examples of standard candles are cepheids variable stars and supernovae Two important questions • Are there black holes in galaxies? • What is a black hole? Two important questions • How do we know it? • Exactly in the same way we know the mass of the sun, or the mass of galaxies for that matter! Two important questions • If the universe is homogeneous and isotropic how do stars know that there is a center of a galaxy to orbit around? • It is a matter of scale: • On scale much larger than a Mpc the universe is homogeneous • On scales much smaller than a Mpc the universe is NOT homogenous, there are galaxies, for example. Assignments. Due Friday 4/19 4PM 1. To TA: Universe 24.42 - 24.43 - 24.45 2. On your own: 24.17 thru 24.30 Today.. On Astro-2 1. How far are galaxies? 2. Measuring velocities and “redshifts”. 3. Hubble’s law.
    [Show full text]
  • 22. Big-Bang Cosmology
    1 22. Big-Bang Cosmology 22. Big-Bang Cosmology Revised August 2019 by K.A. Olive (Minnesota U.) and J.A. Peacock (Edinburgh U.). 22.1 Introduction to Standard Big-Bang Model The observed expansion of the Universe [1–3] is a natural (almost inevitable) result of any homogeneous and isotropic cosmological model based on general relativity. However, by itself, the Hubble expansion does not provide sufficient evidence for what we generally refer to as the Big-Bang model of cosmology. While general relativity is in principle capable of describing the cosmology of any given distribution of matter, it is extremely fortunate that our Universe appears to be homogeneous and isotropic on large scales. Together, homogeneity and isotropy allow us to extend the Copernican Principle to the Cosmological Principle, stating that all spatial positions in the Universe are essentially equivalent. The formulation of the Big-Bang model began in the 1940s with the work of George Gamow and his collaborators, Ralph Alpher and Robert Herman. In order to account for the possibility that the abundances of the elements had a cosmological origin, they proposed that the early Universe was once very hot and dense (enough so as to allow for the nucleosynthetic processing of hydrogen), and has subsequently expanded and cooled to its present state [4,5]. In 1948, Alpher and Herman predicted that a direct consequence of this model is the presence of a relic background radiation with a temperature of order a few K [6,7]. Of course this radiation was observed 16 years later as the Cosmic Microwave Background (CMB) [8].
    [Show full text]
  • The Problem of the Age of the Universe and the Earliest Galaxies
    The Problem of the Age of the Universe and the Earliest Galaxies Roger Ellman Abstract A number of years ago the estimates of astronomers and astrophysicists were that the earliest galaxies took about 2½ - 3 billion years to form, that is, that they did not appear until 2.5-3.0 billion years after the Big Bang. Those estimates were based on analysis of the processes involved in star formation and in the aggregation and “clumping” of matter in the early universe. Since then improved equipment and techniques [e.g. Keck and Hubble telescopes and gravitational lensing] have resulted in reports of observation of early galaxies having stars that formed as early as 300 million years after the Big Bang. Such new data has led to the abandonment of the several billion years estimates of the time required for star and galaxy formation; however, an alternative response to the data would be to re-examine the Hubble theory from which the age of the universe and the distance to high redshift objects is determined. Roger Ellman, The-Origin Foundation, Inc. 320 Gemma Circle, Santa Rosa, CA 95404, USA [email protected] http://www.The-Origin.org 1 The Problem of the Age of the Universe and the Earliest Galaxies Roger Ellman Background of the Problem A number of years ago the estimates of astronomers and astrophysicists were that the earliest galaxies took about 2½ - 3 billion years to form, that is, that they did not appear until 2.5-3.0 billion years after the Big Bang. Those estimates were based on analysis of the processes involved in star formation and in the aggregation and “clumping” of matter in the early universe.
    [Show full text]