8A

From radiation to matter

How the early universe turned radiation into matter: the hot Big Bang, mass–energy equivalence E = mc², pair production and annihilation, the cooling sequence from quarks to nuclei to atoms, Big Bang nucleosynthesis of hydrogen and helium, recombination and the cosmic microwave background.

In 1964 Arno Penzias and Robert Wilson could not get rid of a faint hiss in their new radio antenna in New Jersey. They cleaned out pigeon droppings, checked every joint, and pointed it all over the sky. The hiss was the same everywhere. They had found light released when the universe was 380 000 years old, stretched by expansion into microwaves. It is still arriving from every direction, about 400 photons in every cubic centimetre of the room you are in.

The hot Big Bang

The Big Bang theory says the universe began about 13.8 billion years ago in an extremely hot, dense state and has been expanding and cooling ever since. It was not an explosion of matter into empty space. Space itself has been stretching everywhere at once, and there is no centre.

The early universe was dominated by radiation: high-energy photons, along with particles moving so fast they behaved like radiation. As space expanded, every photon's wavelength was stretched, so its energy fell. Temperature is a measure of the typical energy of the particles and photons, so the universe cooled. A useful rule is that the average photon energy is about $2.7kT$, where $k = 8.62 \times 10^{-5}$ eV K−1 is Boltzmann's constant.

The key idea of this page: as the universe cooled through particular temperatures, the photons no longer had enough energy to do certain things. Each of those thresholds left something behind, and together they explain where matter came from.

Mass–energy equivalence

Einstein's special relativity showed that mass and energy are two forms of the same thing. A mass $m$ is equivalent to an energy

$$E = mc^2$$

where $c = 3.00 \times 10^{8}$ m s−1. Because $c^2$ is enormous ($9.00 \times 10^{16}$), a tiny mass corresponds to a huge energy. The equation runs both ways: matter can be converted to energy (as in stars and reactors), and energy can be converted into matter, as long as the conservation laws are obeyed.

In nuclear and particle physics, energies are usually given in electron volts. One electron volt is the energy an electron gains moving through 1 V: $1\ \text{eV} = 1.602 \times 10^{-19}$ J. Masses of atoms are given in unified atomic mass units, $1\ \text{u} = 1.661 \times 10^{-27}$ kg, and the data sheet gives the shortcut

$$1\ \text{u} = 931.5\ \text{MeV}/c^2$$

so multiplying a mass in u by 931.5 gives its energy equivalent in MeV.

Worked example: the energy in an electron's mass

Calculate the rest energy of an electron ($m_e = 9.109 \times 10^{-31}$ kg) in joules and in MeV.

The question

$E = mc^2 = 9.109 \times 10^{-31} \times (3.00 \times 10^{8})^2 = 8.20 \times 10^{-14}$ J

Use E = mc²

$E = \dfrac{8.20 \times 10^{-14}}{1.602 \times 10^{-19}} = 5.12 \times 10^{5}$ eV $= 0.512$ MeV. (The accepted value, using the exact $c$, is 0.511 MeV.)

Convert to eV

Pair production and annihilation

A photon with enough energy can turn into a particle and its antiparticle. This is pair production. The most common example is a gamma-ray photon becoming an electron and a positron (an anti-electron, same mass, opposite charge):

$$\gamma \rightarrow e^- + e^+$$

Charge is conserved (0 = −1 + 1). The photon must have at least the rest energy of both particles, $2 \times 0.511 = 1.022$ MeV. In practice pair production happens near a nucleus, which recoils and lets momentum be conserved too.

The reverse is annihilation: a particle meets its antiparticle and they convert entirely into photons, usually two gamma rays of 0.511 MeV each heading in opposite directions. PET scanners in hospitals detect exactly these photon pairs from positrons emitted inside the body.

Pair production near a nucleus: a gamma-ray photon of at least 1.022 MeV becomes an electron and a positron, which curve opposite ways in a magnetic field. When the positron later meets an electron, the pair annihilates into two 0.511 MeV photons.

In the early universe, photons were energetic enough to make pairs constantly, and pairs annihilated just as often. Matter and radiation were in balance. Once the temperature fell so that typical photons had less energy than a pair's rest energy, pair production stopped, but annihilation carried on. Almost all the particles and antiparticles destroyed each other.

Almost all, but not quite. For roughly every billion antiquarks there were a billion and one quarks. That tiny excess, whose cause is still one of the big open questions in physics, is all the matter in the universe today. The billion annihilated pairs survive as the photons of the cosmic microwave background, which is why photons outnumber protons by about a billion to one.

Worked example: the temperature for making electrons

Estimate the temperature below which photons in the early universe could no longer typically make electron–positron pairs.

The question

Each pair needs 1.022 MeV $= 1.022 \times 10^{6}$ eV.

Energy needed

$2.7kT = 1.022 \times 10^{6}$ eV, so $T = \dfrac{1.022 \times 10^{6}}{2.7 \times 8.62 \times 10^{-5}} = 4.4 \times 10^{9}$ K.

Set the mean photon energy equal to it

Below about 4 billion K (a few seconds after the Big Bang), electron–positron pairs annihilate faster than they are made. The same reasoning with the proton's 938 MeV rest energy gives about $8 \times 10^{12}$ K for proton–antiproton pairs, which was reached within the first microsecond or so.

Interpret
InteractiveCool the early universe
Try this
  • Start at the top of the slider ($10^{14}$ K). Photons are making proton–antiproton and electron–positron pairs. Read the mean photon energy.
  • Slide down to about $8 \times 10^{12}$ K. What happens to proton–antiproton pair production, and roughly how long after the Big Bang is this?
  • Keep cooling to $4.4 \times 10^{9}$ K. Check that the mean photon energy is now about 1 MeV, close to the 1.022 MeV a pair needs.
  • At about $10^{9}$ K helium nuclei can survive. Read off the time: it is a few minutes, not hundreds of thousands of years.
  • Cool to just below 3000 K. The photons can no longer ionise hydrogen. Read the time since the Big Bang (a few hundred thousand years) and explain why the universe becomes transparent here.

From quarks to atoms

You met a simple Big Bang timeline in Year 10. At HSC level you need to explain why each stage happens when it does, using energy and temperature.

The cooling universe. Each new kind of structure appears once the photons are no longer energetic enough to break it apart. Times and temperatures are approximate.
Time after the Big BangTemperatureWhat happens and why
Before $10^{-32}$ sabove $10^{27}$ KPossible inflation: an extremely rapid expansion that smoothed and flattened the universe. The four fundamental forces are thought to have separated from one unified force in this era.
About $10^{-12}$ sabout $10^{15}$ KThe electromagnetic and weak forces separate. Particles gain mass through the Higgs field. The universe is a quark–gluon plasma.
About $10^{-6}$ sabout $10^{12}$ KQuarks are confined into protons and neutrons (hadrons). Proton–antiproton pairs can no longer be made, and the leftover protons and neutrons remain.
1 to 10 sabout $10^{10}$ to $10^{9}$ KElectron–positron pairs annihilate; the leftover electrons remain. Neutrons stop converting easily into protons, freezing in about 1 neutron for every 6 protons, which then drops to about 1 in 7 as some neutrons decay.
About 3 to 20 minabout $10^{9}$ KBig Bang nucleosynthesis: protons and neutrons fuse into deuterium, then helium-4, with traces of lithium-7. After 20 min the universe is too cool and thin for more fusion.
About 380 000 yearsabout 3000 KRecombination: electrons join nuclei to form neutral atoms. Photons stop scattering off free electrons and travel freely: this light is the cosmic microwave background.
About 200 million yearsabout 50 K (gas)The first stars form from hydrogen and helium gas; they begin making heavier elements.

Big Bang nucleosynthesis

Within the first few minutes, neutrons and protons combined. The first step, $p + n \rightarrow {}^2\text{H} + \gamma$, could not stick until photons were too weak to break deuterium apart again (its binding energy is only 2.2 MeV). Once deuterium survived, almost every neutron ended up inside helium-4, which is very tightly bound.

A simple count shows how this predicts the composition of the universe. With about 1 neutron for every 7 protons, take 16 particles: 2 neutrons and 14 protons. The 2 neutrons join 2 protons to make one helium-4 nucleus (mass 4), leaving 12 protons as hydrogen (mass 12). Helium is $4/16 = 25\%$ of the mass. Astronomers measure about 24–25% helium by mass in the oldest gas clouds and stars, a strong confirmation of the Big Bang model.

Nothing heavier than lithium was made in useful amounts, because there are no stable nuclei with mass 5 or 8 to step through, and the universe cooled too quickly. Every heavier element was made later, in stars (page 8E).

Recombination and the cosmic microwave background

For 380 000 years the universe was a glowing plasma, opaque like the inside of the Sun, because photons scattered off free electrons. At about 3000 K, typical photons could no longer ionise hydrogen (13.6 eV), electrons and nuclei combined, and the universe became transparent. Those photons have been travelling ever since. Expansion has stretched their wavelengths by a factor of about 1100, so they now look like black-body radiation at 2.725 K, peaking in the microwave region.

The cosmic microwave background is evidence for the Big Bang because it is a near-perfect black-body spectrum, it comes equally from every direction (to 1 part in 100 000), and its temperature matches the predicted cooling. The tiny ripples in it, mapped by the COBE, WMAP and Planck satellites, are the seeds that grew into galaxies.

Measurements from the Planck satellite (2018) show that today the universe's energy is about 68% dark energy, 27% dark matter and only 5% ordinary matter made of atoms. Dark matter and dark energy are not explained by the Standard Model, and finding what they are is an active area of research.

Test yourself

  1. What is the minimum energy of a photon that can produce a proton–antiproton pair? (Proton rest energy = 938 MeV.)

  2. Which event happened about 380 000 years after the Big Bang?

  3. Why was almost no element heavier than lithium made in the first 20 minutes?

  4. The cosmic microwave background now matches a black body at 2.7 K. It was released at about 3000 K. This shows that since then the universe has

  5. The mass of 1.00 g of matter is completely converted to energy. The energy released is

Label the stages of the early universe.

10-40 s10-30 s10-20 s10-10 s100 s1010 s100108101610241032Time since the Big Bang (log scale)Temperature (K, log scale)Planck time: gravity separatesInflationElectroweak force splitsQuarks bind into protons and neutronsNucleosynthesis: H and He nuclei (3–20 min)Recombination: atoms form, CMB releasedToday: 2.725 KMatter forms as the universe cools

Put these events in the order they happened.

Mass and energy are related by $E = $ . A gamma-ray photon of at least can create an electron and a . When a particle meets its antiparticle they into photons. Big Bang nucleosynthesis produced mostly hydrogen and about 25% by mass.

5 marks

Explain how radiation was transformed into matter in the period following the Big Bang. In your answer, refer to mass–energy equivalence and to the effect of the universe's expansion.

3 marks

A positron and an electron, both essentially at rest, annihilate. Calculate the wavelength of each of the two photons produced. ($m_e = 9.109 \times 10^{-31}$ kg)