International Axion Observatory

Last updated
International Axion Observatory
Predecessor CERN Axion Solar Telescope
FormationJuly 2017 at DESY, Hamburg
Legal statusIn construction
PurposeSearch for axions and other physics beyond the Standard Model
Headquarters DESY, Hamburg, Germany
FieldsAstroparticle physics
Spokesperson
Igor G. Irastorza
Website iaxo.desy.de


The International Axion Observatory (IAXO) is a next-generation axion helioscope for the search of solar axions and axion-like particles. It is the follow-up of the CERN Axion Solar Telescope (CAST), which operated from 2003 to 2022. [1] IAXO will be set up by implementing the helioscope concept bringing it to a larger size and longer observation times. [2] [3] [4]

Contents

The IAXO collaboration

The Letter of Intent for International Axion Observatory was submitted to the CERN in August 2013. [5] IAXO formally founded in July 2017 and received an advanced grant from the European Research Council in October 2018. [6] The near-term goal of the collaboration is to build a precursor version of the experiment, called BabyIAXO, which will be located at DESY, Germany. [1] [7] [8] [9]

The IAXO Collaboration is formed by 21 institutes from 7 different countries.

Principle of operation

The IAXO experiment is based on the helioscope principle. Axions can be produced in stars (like the sun) via the Primakoff effect and other mechanisms. These axions would reach the telescope and would be converted into soft X-ray photons in the presence of a magnetic field. Then, these photons travel through a focusing X-ray optics, and are expected as an excess of signal in the detector when the magnet points to the Sun.

Axion heliscope's principle of operation Conceptual-arrangement-of-an-enhanced-axion-helioscope-with-x-ray-focalization-Solar.png
Axion heliscope's principle of operation

The limit to the axion-photon coupling is given by the FOM: where the first factor is related to the magnet, with the magnetic field (B), the length of the magnet (L) and the area (A). The second part depends on the efficiency () and background (b) of the detector. The third is regarding the optics, more specifically the efficiency () and the area of the focused signal on the detector readout (). And the last term is related to the time (t) of operation.

IAXO: The International Axion Observatory

Conceptual design of the International AXion Observatory IAXO design.jpg
Conceptual design of the International AXion Observatory

IAXO will be a next-generation enhanced helioscope, with a signal to noise ratio of five orders of magnitude higher compared to current-day detectors. The cross-sectional area of the magnet equipped with an X-ray focus optics is meant to increase this signal to background ratio. When the solar axions come in contact with the magnetic cross-section, they are converted into photons through the Primakoff effect. These photons would then be detected by X-ray detectors placed on the telescope. This implies that a larger magnetic cross-section will lead to a more intense signal. [3] [5] The magnet will be a purpose‐built large‐scale superconductor with a length of 20 meters and a field strength of up to 5.4 Tesla. The whole telescope will feature 8 bores (with 8 detection systems).

The helioscope will also be equipped with a mechanical system allowing it to follow the sun consistently throughout the day (about 50% of sun-tracking time), leading to enhanced exposure. [5] The IAXO subsystems comprising magnets, optics, and detectors are planned to be fully optimized for solar axion detectors.

The FOM of IAXO would be over 300 times larger than in CAST, and the sensitivity of the axion-photon coupling measurement in would be 1–1.5 order of magnitude higher than that achieved by previous detectors. [1]

BabyIAXO

Conceptual design of BabyIAXO helioscope BabyIAXO design.png
Conceptual design of BabyIAXO helioscope

BabyIAXO is a technological prototype of all the subsystems of the IAXO with 2 magnet bores (with 2 detection systems) in a magnet of 10 meters length. The prototype is a testing version and will serve as an intermediate step to explore further possible improvements to the final IAXO. BabyIAXO will be set up in Hamburg, Germany by the CERN and DESY collaboration. [10] [11] CERN will be responsible for giving in the design reports of prototype magnets and cryostat, and DESY will design and construct the movable platform along with the other infrastructure. The data taking by BabyIAXO is scheduled to start in 2028. [12] [10] [13]

In addition to being a proof of concept for IAXO, BabyIAXO will have its own physics potential and a FOM around 100 times larger than CAST.

Sensitivity and physics potential

Axion-Photon panorama AxionPhoton panorama.png
Axion-Photon panorama

IAXO will primarily be hunting for solar axions, along with the potential to observe the quantum chromodynamics (QCD) axion in the mass range of 1 meV to 1 eV. It is also expected to be capable of discovering axion-like particles (known as the ALPs) coupled either with photons or electrons. [1]

The QCD-axions and the ALPs are predicted to have quite similar properties, and hence IAXO, whose primary goal is to observe the solar axions and photon-coupled ALPs, will also be able to detect the QCD axions and ALPs from different unexplored astrophysical axion sources. [1] [14] It, therefore, has the potential to solve both the strong CP problem and the dark matter problem, which depends on the discovery of the axion particles. [2] [15] [12]

IAXO is believed to be the most ambitious experiment among the current-day experiment set-ups to observe the hypothetical axions. [1] It could also be later adapted to test models of hypothesized hidden photons or chameleons. [2] [3]

Sources accessible to IAXO

Any particle found by IAXO will be at the least a sub-dominant component of the dark matter. The observatory would be capable of observing from a wide range of sources given below. [1] [5]

  1. Quantum chromodynamics axions
  2. Dark matter axions
  3. Solar axions
  4. Axions from astrophysical cooling anomalies such as white dwarf cooling, neutron star cooling, globular clusters, and supergiant stars powered by helium.

BabyIAXO design

Magnet

The central magnetic systems will have a large superconducting magnet, configured in a toroidal multibore manner, in order to generate a strong magnetic field over a larger volume. It will be a 10 meters long magnet consisting of two different coils made out of 35 km Rutherford cable. This configuration is calculated to generate a 2.5 Tesla magnetic field within a 70 cm diameter. The magnetic subsystem is inspired by the ATLAS experiment. [1] [5]

X-ray optics

Since BabyIAXO will have two bores in the magnet, two X-ray optics are required to operate in parallel. Both optics are Wolter telescopes (type I).

One of the two BabyIAXO optics will be based on a mature technology developed for NASA's NuStar X-ray satellite. [5] The signal from the 0.7 m diameter bore will be focused to 0.2 area.

The second BabyIAXO optics will be one of the flight models of the XMM-Newton space mission that belongs to the ESA.

Detectors

IAXO and BabyIAXO will have multiple, diverse detectors working in parallel mounted to the different magnet bores.

The detectors for this experiment need to meet certain technical requirements. They need a high detection efficiency in the ROI (1 – 10 keV) where the Primakoff axion signal is expected. They also need very low background in ROI of under (less than 3 counts per year of data). To reach this background level, the detector relies on:

  1. The use of shielding both passive (to block environmental gammas) and active (to tag cosmic induce events).
  2. The intrinsic radiopurity of the construction materials.
  3. The advanced event discrimination strategies based on topological information, validated with simulations.

Detector technologies

Based upon the experience from CAST, the baseline detector technology will be a TPC with a Micromegas readout.

There are several other technologies under study: GridPix, Metallic Magnetic Calorimeters (MMC), Transition Edge Sensors (TES) and Silicon Drift Detectors (SDD).

See also


Related Research Articles

An axion is a hypothetical elementary particle proposed independently by Frank Wilczek and Steven Weinberg in 1978 on the basis of the Peccei–Quinn theory for resolving the strong CP problem posed by the apparent success of quantum chromodynamics (QCD) as a theory of the strong nuclear force. If axions exist and were made in the Big Bang with sufficient number density, they would form the dark matter in the universe provided the axion mass falls within a narrow range set by the ratio of the present cold dark matter mass density to the present axion number density.

<span class="mw-page-title-main">Airy disk</span> Diffraction pattern in optics

In optics, the Airy disk and Airy pattern are descriptions of the best-focused spot of light that a perfect lens with a circular aperture can make, limited by the diffraction of light. The Airy disk is of importance in physics, optics, and astronomy.

<span class="mw-page-title-main">Neutrino astronomy</span> Observing low-mass stellar particles

Neutrino astronomy is the branch of astronomy that gathers information about astronomical objects by observing and studying neutrinos emitted by them with the help of neutrino detectors in special Earth observatories. It is an emerging field in astroparticle physics providing insights into the high-energy and non-thermal processes in the universe.

<span class="mw-page-title-main">CERN Axion Solar Telescope</span> Experiment in astroparticle physics, sited at CERN in Switzerland

The CERN Axion Solar Telescope (CAST) is an experiment in astroparticle physics to search for axions originating from the Sun. The experiment, sited at CERN in Switzerland, was commissioned in 1999 and came online in 2002 with the first data-taking run starting in May 2003. The successful detection of solar axions would constitute a major discovery in particle physics, and would also open up a brand new window on the astrophysics of the solar core.

<span class="mw-page-title-main">LHCb experiment</span> Experiment at the Large Hadron Collider

The LHCb experiment is a particle physics detector experiment collecting data at the Large Hadron Collider at CERN. LHCb is a specialized b-physics experiment, designed primarily to measure the parameters of CP violation in the interactions of b-hadrons. Such studies can help to explain the matter-antimatter asymmetry of the Universe. The detector is also able to perform measurements of production cross sections, exotic hadron spectroscopy, charm physics and electroweak physics in the forward region. The LHCb collaborators, who built, operate and analyse data from the experiment, are composed of approximately 1650 people from 98 scientific institutes, representing 22 countries. Vincenzo Vagnoni succeeded on July 1, 2023 as spokesperson for the collaboration from Chris Parkes. The experiment is located at point 8 on the LHC tunnel close to Ferney-Voltaire, France just over the border from Geneva. The (small) MoEDAL experiment shares the same cavern.

The ring-imaging Cherenkov, or RICH, detector is a device for identifying the type of an electrically charged subatomic particle of known momentum, that traverses a transparent refractive medium, by measurement of the presence and characteristics of the Cherenkov radiation emitted during that traversal. RICH detectors were first developed in the 1980s and are used in high energy elementary particle-, nuclear- and astro-physics experiments.

<span class="mw-page-title-main">Air shower (physics)</span> Cascade of atmospheric subatomic particles

Air showers are extensive cascades of subatomic particles and ionized nuclei, produced in the atmosphere when a primary cosmic ray enters the atmosphere. When a particle of the cosmic radiation, which could be a proton, a nucleus, an electron, a photon, or (rarely) a positron, interacts with the nucleus of a molecule in the atmosphere, it produces a vast number of secondary particles, which make up the shower. In the first interactions of the cascade especially hadrons are produced and decay rapidly in the air, producing other particles and electromagnetic radiation, which are part of the shower components. Depending on the energy of the cosmic ray, the detectable size of the shower can reach several kilometers in diameter.

In theoretical physics, Pauli–Villars regularization (P–V) is a procedure that isolates divergent terms from finite parts in loop calculations in field theory in order to renormalize the theory. Wolfgang Pauli and Felix Villars published the method in 1949, based on earlier work by Richard Feynman, Ernst Stueckelberg and Dominique Rivier.

<span class="mw-page-title-main">Helioscope</span>

A helioscope is an instrument used in observing the Sun and sunspots. The helioscope was first used by Benedetto Castelli (1578-1643) and refined by Galileo Galilei (1564–1642). The method involves projecting an image of the sun onto a white sheet of paper suspended in a darkened room with the use of a telescope.

<span class="mw-page-title-main">Elitzur–Vaidman bomb tester</span> Quantum mechanics thought experiment

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<span class="mw-page-title-main">X-ray telescope</span> Telescope designed to observe remote objects by detecting X-rays

An X-ray telescope (XRT) is a telescope that is designed to observe remote objects in the X-ray spectrum. X-rays are absorbed by the Earth's atmosphere, so instruments to detect X-rays must be taken to high altitude by balloons, sounding rockets, and satellites.

<span class="mw-page-title-main">Solar telescope</span> Telescope used to observe the Sun

A solar telescope or a solar observatory is a special-purpose telescope used to observe the Sun. Solar telescopes usually detect light with wavelengths in, or not far outside, the visible spectrum. Obsolete names for Sun telescopes include heliograph and photoheliograph.

<span class="mw-page-title-main">LHCf experiment</span>

The LHCf is a special-purpose Large Hadron Collider experiment for astroparticle physics, and one of nine detectors in the LHC accelerator at CERN. LHCf is designed to study the particles generated in the forward region of collisions, those almost directly in line with the colliding proton beams.

PVLAS aims to carry out a test of quantum electrodynamics and possibly detect dark matter at the Department of Physics and National Institute of Nuclear Physics in Ferrara, Italy. It searches for vacuum polarization causing nonlinear optical behavior in magnetic fields. Experiments began in 2001 at the INFN Laboratory in Legnaro and continue today with new equipment.

<span class="mw-page-title-main">COMPASS experiment</span>

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<span class="mw-page-title-main">Primakoff effect</span> Phenomenon in particle physics

In particle physics, the Primakoff effect, named after Henry Primakoff, is the resonant production of neutral pseudoscalar mesons by high-energy photons interacting with an atomic nucleus. It can be viewed as the reverse process of the decay of the meson into two photons and has been used for the measurement of the decay width of neutral mesons.

<span class="mw-page-title-main">Cosmic-ray observatory</span> Installation built to detect high-energy-particles coming from space

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<span class="mw-page-title-main">NA62 experiment</span>

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<span class="mw-page-title-main">Courant–Snyder parameters</span> Set of quantities in accelerator physics

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