Physics

The International Axion Observatory is a new generation axion helioscope and its main goal is to detect axions (or other similar particles) potentially emitted by the Sun’s core in large quantities. Axions are hypothetical particles proposed in extensions of the Standard Model of Particle Physics. Their existence in not proved experimentally but there are strong theoretical reasons to suspect so. Also, there is a motivating link with the problem of the Dark Matter of the Universe.

Click here to know more about axions, and their connection with the Dark Matter and why particle physicsists search for them.

In order to do that, an axion helioscope uses a strong magnetic field to trigger the conversion of axions into detectable photons. The larger and more powerful the magnetic field, the larger the probability the conversion is. IAXO will use a huge 20m long toroidal superconducting magnet, with eight coils and eight 60cm diameter bores placed in between the coils. This magnet will be placed on a moving structure, much like that of a conventional telescope, in order to point the magnet to the Sun.

At the end of the magnet bores, specially built x-ray optics will focus the putative axion-induced photons into small regions (0.2 cm2) at a focal distance of about 5 meters. Each of the focal spots will be imaged by ultra low background x-ray Micromegas detectors.

What is the axion?
And why it is being searched for by particle physicists?
What is its relation with the Dark Matter of the Universe?

The axion is an hypothetical particle that appears in extensions of the Standard Model of Particle Physics that include the so-called Peccei-Quinn mechanism. This mechanism was postulated already 35 years ago to explain an standing problem of the Standard Model: the strong-CP problem.

A physical law has CP (charge-parity) symmetry if it is equally valid after interchanging each particle by its antiparticle (charge conjugation or C symmetry) and -at the same time- inverting the spatial coordinates (parity, “mirror” or P symmetry). It is known since some time now that the electroweak interactions do not respect CP symmetry, that is, physicists have observed phenomena that, although only slighly, violate this symmetry.

However, this does not seem to be the case with the strong interactions (those responsible for holding toghether protons and neutrons in the nuclei). The non observation of CP-violating phenomena here impose severe restrictions to input parameters (i.e. parameters not predicted) of the Standard Model, so that they need to be fine-tunned for theory and observation to agree. When this happens in a physical theory usually means that there is something we do not understand and our theory is not complete. This is the strong CP problem.

The Peccei-Quinn mechanism was proposed to solve this problem in a natural way, without required parameter fine-tunning. As a collateral effect, however, a new particle appears, the axion, which may have important observable consequences. In the first place, the axion is a neutral and very light (but not massless) particle, and it does not interact (or does it very weakly)  with conventional matter. In some way one can see the axion as a “strange photon”. In fact, theory predicts that the axion, if it exists, could transform into a photon (and viceversa) in the presence of electromagnetic fields. This property of the axion is crucial for most of the experimental strategies of axion detection.

This Feynman diagram represents the process of conversion of an axion (dashed line on the left) into a photon (wavy line on the right) in the presence of an electromagnetic field (the wavy line going downwards)

But doubtless one of the most suggestive properties of axions is that, in a natural way, they could be produced in huge numbers soon after the Big Bang. This population of axions would still be present today and could compose the Dark Matter of the Universe. The existence of Dark Matter is widely accepted in the scientific community, but its nature is still a mystery. Together with WIMPs, the axions are among the most searched candidates in the context of the nature of Dark Matter.

Detection of axions

Thanks to the property of conversion into photons in electromagnetic fields, axions could be produced and detected in the laboratory by using very intense magnets. This type of experiments are being carried out (e.g. ALPS in DESY, or OSQAR at CERN), although their sensitivity is still far from “seeing” the axions predicted by the Peccei-Quinn mechanism.

If the axion exist and it is the main component of Dark Matter, the very relic axions that would be bombarding us continuously could be detected using microwave resonant (to the axion mass) cavities, immersed in powerful magnetic fields. This scheme is followed, e.g., by the ADMX experiment in the University of Washington. ADMX could detect the axion, if its mass (which is unknown) lies in the sensitivity range of the experiment (around the few microelectronvolts) and if the Dark Matter is mainly composed by axions.

Another promising detection technique, this one independent of the axion being the Dark Matter, is that of the axion helioscope, aiming to detect axions produced at the solar interior. These could be detected, once again, using a powerful magnet, but this time equipped with low background x-ray detectors. The most powerful axion helioscope to-date is the CERN Axion Solar Telescope or CAST, datking data since about a decade at CERN. Although so far there is no sign of the axion, CAST has been the first axion helioscope with enough sensitivity to surpass previous very stringent astrophysical limits on the axion properties, and enter so far unexplored area. In particular, CAST is sensitive to Peccei-Quinn axions with masses in the 0.1-1 eV range approximately.

The International Axion Observatory is a new generation axion helioscope. Its layaout is an ambitious extension of CAST’s philosophy, using a superconducting magnet of larger dimensions and specifically designed to search for axions, and equipped with x-ray optics and low background detectors. IAXO would have sensitivity to detect axions in the much larger mass range than CAST and thus would explore an important area of parametric space which is also inaccessible by other techniques. In addition, IAXO’s magnet could also host other kind of axion experiments, so IAXO could become a sort of a generic infrastructure for axion research. If the axion exists IAXO will have a real opportunity to discover it.