Cosmic Microwave Background Radiation

Chapter index in this window —   — Chapter index in separate window

Video lecture for this page

This material (including images) is copyrighted!. See my copyright notice for fair use practices. Select the photographs to display the original source in another window. Links to external sites will be displayed in another window.

George Gamov (lived 1904--1968) predicted in 1948 that there should be a faint glow left over from when the universe was much hotter and denser. Since the universe is observed to be expanding, it means that the galaxies were originally right on top of each other. Also, the energy of the universe was concentrated in a smaller volume. The entire universe would have glowed first in the gamma ray band, then the X-ray band, then to less energetic bands as the universe expanded. By now, about 13.8 billion years after the start of the expansion, the cold universe should glow in the radio band. The expansion rate has slowed down over time because of the force of gravity. This means that the early expansion was faster than it is now. At the start of the expansion, the expansion rate was extremely rapid.

The early large expansion rate and very hot temperatures made Fred Hoyle (lived 1915 - 2001) call this theory of the birth of the universe, the Big Bang. At the time he coined the term, Hoyle was advocating another theory that used the perfect cosmological principle called the Steady State theory. So at the time, Hoyle's "Big Bang" term was made in joking disdain. However, the Big Bang proponents liked the term and used it from then on.

Observation

Arno Penzias and Robert Wilson observed in 1965 a radio background source that was spread all over the universe---the cosmic microwave background radiation. The radiation has the same intensity and spectral character as a thermal continuous source at 3 K (more precisely, 2.728 ± 0.004 K) as measured by the COBE satellite in every direction observed. To a high degree of precision the sky is uniformly bright in radio. The uniformity of the background radiation is evidence for the cosmological principle. The error bars in the figure below are too small to be seen.

the nearly perfect thermal spectrum of the CMBR

Interpretation

This background radiation is interpreted to be the relic of the early universe. If this is correct, then the early universe was very uniform. Since the further out in space you look means the further back in time you look, the microwave radiation is coming from the universe as it was a few hundred thousand years after the Big Bang when the universe was much hotter. The glow from the early hot universe has been redshifted by 1000 times! Hoyle's Steady State theory could not adequately explain the presence of the background radiation and so was abandoned by most astronomers.

Let's take a closer look at what was happening in the universe when it produced the background radiation. The early universe (both the matter and the radiation) was much more compact. The radiation density was so great that it dominated the expansion rate and the conditions of the universe for the first 10,000 years. Remember Einstein's equation relating energy and mass? The energy E=mc2 so the radiation energy had a definite gravitational effect!

The early universe was hot and opaque (photons could not move very far before being absorbed). The freely-moving electrons, protons, and neutrons scattered the photons all about making the dense gas opaque. Dense hot gases will produce a continuous spectrum that depends only on the temperature (a thermal spectrum). The universe cooled off as it expanded. Eventually, the early universe cooled to where the electrons and protons could combine to form neutral hydrogen atoms and not be blown apart by energetic photons. The process of the electrons becoming bound to the protons to make atoms is called recombination. Okay, "recombination" is not really correct since this was the first time that the electrons combined with the protons, but the term also describes processes that occur today. Extrapolating the expansion rate and the temperature of the universe backward in time, one finds that at the temperature of 3000 K, the universe was about 380,000 years old.

how the universe became transparent

At the time of recombination, the number of unit particles was cut at least in half (one electron + one proton become a single atom; the neutrons also were incorporated into the atoms). That meant the photons could travel further without hitting some kind of unit particle. Also, the expansion of the universe spread the matter out. In addition, the coolness of the universe (only 3000 K at the time of recombination) meant that longer wavelengths of light were present. Instead of the gamma rays and X-rays of earlier times, the predominant form of radiation was the longer wavelength visible light and infrared. Longer wavelengths of light are able to more easily to pass through gas. For all of these reasons the photons could then travel long distances without running into some particle. The universe became transparent when the universe was glowing at the temperature of the surface of a cool star. The photons from this time are now reaching our radio telescopes. They are by far the oldest radiation that can be detected.

The universe could not have been perfectly uniform, though. The universe must have been slightly lumpy to form galaxies and people later on from the internal gravity of the lumps. Gravity is symmetrical so it needed some initial density variations to provide some direction to where surrounding matter could be attracted. The COBE satellite found slight variations in the brightness of the background radiation of about 1 part in 100,000. The slight variations exist because some parts of the universe were slightly denser than other parts. The slightly denser regions had more gravity and attracted more material to them while the expansion occurred. Over time, the denser regions got even denser and eventually formed galaxies about 1 billion years after the Big Bang. The slightly less dense places got even emptier as gravity increased the contrast between the denser places and less dense places. See the figure at the end of the superclusters section for a simulation of this process.

Below is a sequence of false-color microwave all-sky maps from the Differential Microwave Radiometer (DMR) instrument on the COBE satellite. The galactic equator runs horizontally through the center of each map. The range of temperatures for each map is given in the caption.

raw background data from COBE

The colors for the temperatures range from blue for 0 K to red for 4 K (yes, the color scheme is backward---blue should be hot and red should be cool). Notice that the background appears completely uniform at a temperature of 2.728 K.
doppler effect shows our motion against the background

The colors for the temperatures range from blue for 2.724 K to red for 2.732 K. The double-lobe pattern shows the doppler effect from the motion of the Sun with respect to the background radiation. The background appears about 1/1000 times hotter (redder in this false-color map) in the direction the Sun is moving toward and about 1/1000 times cooler (bluer here) in the direction the Sun is moving away from.
the Milky Way emission on top of the background fluctuations

The colors for the temperatures range from blue for 2.7279 K to red for 2.7281 K. The effect of the Sun's motion has been subtracted out leaving fluctuations that are thirty times smaller than the previous map. The faint microwave contribution of the Milky Way is clearly seen along the center. The Cygnus constellation is at left center, the Sagittarius constellation is at the center, and the Orion constellation is at right center.

Below is a picture of the fluctuations in the background radiation when the Milky Way's contribution is subtracted out. It shows a comparison of the coarse resolution of COBE with the finer resolution of the Wilkinson Microwave Anisotropy Probe (WMAP). WMAP had over 30 times greater resolution than the COBE satellite. With that greater resolution WMAP enabled us to learn the composition, geometry, and history of the universe, amount of matter in the universe, as well as, it provided much tighter constraints on the models. Selecting the map below will take you to the WMAP homepage in another window.

the fluctuations in the CMBR---galaxy seeds (COBE vs. WMAP)

The follow-up to WMAP is the Planck mission with over 2.5 times greater resolution than WMAP. The first data release in early 2013 confirmed the standard cosmology model derived from the COBE and WMAP missions but it did show some surprises at the really large scales (6 to 90 degrees across) with slightly weaker than expected fluctuations at those scales and also an asymmetry in the temperature fluctuations across the two halves of the sky, where one hemisphere has a wider variation in the fluctuations than the other hemisphere. In the past, advances in technology led to breakthroughs in our understanding of the nature of the universe and the high-precision measurements of Planck may be indicating a need to modify the standard cosmology model.

comparison of COBE to WMAP to Planck

The time period between when the universe became transparent about 380,000 years after the Big Bang and formation of the first stars in the galaxies and the large black holes in the quasars began flooding the universe with powerful ultraviolet is called the "Dark Ages" or "Dark Era" in cosmological models. The ultraviolet light re-ionized the gas, freeing a lot of electrons. The transition period from the Dark Ages to the modern universe is called the "Epoch of Reionization". The light from the cosmic background would scatter off these newly freed electrons and become "polarized" so that the light waves tend to oscillate in a particular direction. How the light is polarized can tell you when the electrons were being freed again, i.e., when the stars first began to shine.

how polarization works

WMAP has detected the polarization of the microwave background and derived a time of about 400 million years after the Big Bang for the first stars but the higher resolution data of Planck puts the time at about 560 million years after the Big Bang. The Epoch of Reionization is thought to take place between about 560 million years to about 1 billion years after the Big Bang. The visible light from these first stars will now have been redshifted into the infrared.

Farthest galaxy in the universe timeline

The Hubble Space Telescope has detected near-infrared light from galaxies shining about 750 million years after the Big Bang in the "Hubble Ultra Deep Field" (and even further back---400 million years after the Big Bang with the new WFPC3 camera) and the Spitzer Space Telescope may have spotted infrared light from early galaxies of about that time in other areas of the sky (see also link). One galaxy whose light was magnified by gravitational lensing by a foreground galaxy cluster appears to have formed a mere 200 million years after the Big Bang. A 2019 study using Spitzer found that the earliest galaxies near the end of the Epoch of Reionization produced much more ionizing radiation than do modern galaxies for some unknown reason. However, it will take the much larger light-gathering power and resolution of the infrared James Webb Space Telescope to study these objects in detail and figure out why.

microwave background to formation of galaxies

previousGo back to previous section -- next Go to next section

Go to Astronomy Notes home

last updated: June 28, 2022

Is this page a copy of Strobel's Astronomy Notes?

Author of original content: Nick Strobel