The International Axion Observatory (IAXO) will be a forth generation axion helioscope. As its primary physics goal, IAXO will look for axions or axion-like particles (ALPs) originating in the Sun via the Primakoff conversion of the solar plasma photons. In terms of signalto-noise ratio, IAXO will be about 4-5 orders of magnitude more sensitive than CAST, currently the most powerful axion helioscope, reaching sensitivity to axion-photon couplings down to a few ×10 −12 GeV −1 and thus probing a large fraction of the currently unexplored axion and ALP parameter space. IAXO will also be sensitive to solar axions produced by mechanisms mediated by the axion-electron coupling g ae with sensitivity −for the first time− to values of g ae not previously excluded by astrophysics. With several other possible physics cases, IAXO has the potential to serve as a multi-purpose facility for generic axion and ALP research in the next decade. In this paper we present the conceptual design of IAXO, which follows the layout of an enhanced axion helioscope, based on a purpose-built 20m-long 8-coils toroidal superconducting magnet. All the eight 60cm-diameter magnet bores are equipped with focusing x-ray optics, able to focus the signal photons into ∼ 0.2 cm 2 spots that are imaged by ultra-low-background Micromegas x-ray detectors. The magnet is built into a structure with elevation and azimuth drives that will allow for solar tracking for ∼12 h each day.
The CERN Axion Solar Telescope has finished its search for solar axions with (3)He buffer gas, covering the search range 0.64 eV ≲ ma ≲ 1.17 eV. This closes the gap to the cosmological hot dark matter limit and actually overlaps with it. From the absence of excess x rays when the magnet was pointing to the Sun we set a typical upper limit on the axion-photon coupling of gaγ ≲ 3.3 × 10(-10) GeV(-1) at 95% C.L., with the exact value depending on the pressure setting. Future direct solar axion searches will focus on increasing the sensitivity to smaller values of gaγ, for example by the currently discussed next generation helioscope International AXion Observatory.
Axion helioscopes aim at the detection of solar axions
through their conversion into x-rays in laboratory magnetic
fields. The use of low background x-ray detectors is an essential
component contributing to the sensitivity of these searches. Here we
review the recent advances on Micromegas detectors used in the CERN
Axion Solar Telescope (CAST) and proposed for the future
International Axion Observatory (IAXO). The most recent Micromegas
setups in CAST have achieved background levels of
1.5 × 10−6 keV−1 cm−2 s−1, a factor of more than 100 lower than the
ones obtained by the first generation of CAST detectors. This
improvement is due to the development of active and passive
shielding techniques, offline discrimination techniques allowed by
highly granular readout patterns, as well as the use of radiopure
detector components. The status of the intensive R&D to reduce the
background levels will be described, including the operation of
replica detectors in test benches and the detailed Geant4 simulation
of the detector setup and the detector response, which has allowed
the progressive understanding of background origins. The best levels
currently achieved in a test setup operating in the Canfranc
Underground Laboratory (LSC) are as low as ∼ 10−7 keV−1 cm−2 s−1,
showing the good prospects of this technology for application in the
future IAXO.
The measurement of the direction of WIMP-induced nuclear recoils is a
compelling but technologically challenging strategy to provide an unambiguous
signature of the detection of Galactic dark matter. Most directional detectors
aim to reconstruct the dark-matter-induced nuclear recoil tracks, either in gas
or solid targets. The main challenge with directional detection is the need for
high spatial resolution over large volumes, which puts strong requirements on
the readout technologies. In this paper we review the various detector readout
technologies used by directional detectors. In particular, we summarize the
challenges, advantages and drawbacks of each approach, and discuss future
prospects for these technologies.Comment: 58 pages, 26 figures, accepted by Physics Report
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