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Cosmic neutrino background

space Maturity 11-13 Next article →

The cosmic neutrino background, often called the CNB or relic neutrinos, is a theoretical field of radiation. This radiation consists of neutrinos that have existed since the very beginning of our universe. While the cosmic microwave background (CMB) provides a snapshot of the universe at 379,000 years old, the CNB is much older. These neutrinos decoupled, or separated from other matter, when the universe was only one second old. Because neutrinos rarely interact with normal matter, they have been traveling through space for over 13 billion years. Today, they are estimated to have a very low temperature of roughly 1.95 K.

To understand the origin of the CNB, we must look at the early universe. At the start, the universe was a very hot, dense plasma. In this state, particles constantly collided and reacted with one another. This created a state of equilibrium, where particles were balanced through constant interaction. Around one second after the Big Bang, this equilibrium was disrupted. As the universe expanded and cooled, neutrinos, electrons, and positrons were spread too far apart to continue reacting. This process is known as decoupling. Once they decoupled, the neutrinos entered a state called free streaming, where they simply moved through space without further collisions.

Scientists cannot measure the temperature of these neutrinos directly, but they can calculate it using physics. The neutrinos and photons (light particles) were once in thermal equilibrium. However, before the photons decoupled from matter, electrons and positrons annihilated. This means they combined to produce more photons, which raised the temperature of the light. By using the principle of conservation of entropy, scientists can estimate this heating. Entropy is a way to measure the energy distribution in a system. Because the photons were heated by this annihilation event, they are now hotter than the neutrinos. Based on the current CMB temperature of 2.725 K, the neutrino temperature is calculated to be about 1.95 K.

There is strong indirect evidence that the CNB exists, even if we have not seen it directly. One major piece of evidence comes from Big Bang nucleosynthesis (BBN). This is the process that created light elements in the early universe. The expansion rate of the universe during BBN was influenced by the energy density of these neutrinos. By measuring the amounts of helium and deuterium in the universe, scientists can infer the presence of neutrinos. Current measurements of these elements align well with the predictions made by the Standard Model of particle physics.

Another way we see the CNB is through its effect on the cosmic microwave background. The presence of neutrinos affects how matter clusters and how the CMB looks. Specifically, neutrinos contribute to the radiation energy density of the universe. This density affects the timing of matter-radiation equality. Neutrinos also create anisotropic stress, which can dampen certain oscillations in the CMB spectra. Data from the WMAP and Planck spacecraft have provided tight bounds on these effects. These observations help confirm that there are likely three types of neutrino species, as the Standard Model predicts.

Directly detecting these relic neutrinos is an immense challenge for modern science. Most neutrinos we detect come from high-energy sources like the Sun or nuclear reactors. The CNB neutrinos are non-relativistic, meaning they move much slower, and they have extremely low energy. Their energy is roughly $10^{10}$ times smaller than the neutrinos we can currently catch. This creates a "lose-lose" situation for detectors. The lower a neutrino's kinetic energy, the less likely it is to interact with matter. Even if an interaction occurs, the signal is incredibly faint and difficult to distinguish from background noise.

One proposed solution for direct detection is the PTOLEMY experiment located in Italy. This experiment aims to capture relic neutrinos using a target of tritium, which is a form of hydrogen. When a neutrino is captured by tritium, it triggers an induced form of beta decay. This reaction produces an electron that can be measured. The challenge is that natural beta decay also produces electrons, creating a massive amount of background noise. To succeed, the detector must have excellent energy resolution to separate the signal from the noise. A demonstrator for this technology is expected to be ready by 2027.

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