TheAtacama Cosmology Telescope (ACT) was a cosmological millimeter-wave telescope located onCerro Toco in theAtacama Desert in the north ofChile.[1] ACT made high-sensitivity, arcminute resolution,microwave-wavelength surveys of the sky in order to study thecosmic microwave background radiation (CMB), the relic radiation left by theBig Bang process. Located 40 km from San Pedro de Atacama, at an altitude of 5,190 metres (17,030 ft), it was one of the highest ground-based telescopes in the world.[a]
Cosmic microwave background experiments like ACT, theSouth Pole Telescope, theWMAP satellite, and thePlanck satellite have provided foundational evidence for the standardLambda-CDM model of cosmology. ACT first detected seven acoustic peaks in the power spectrum of theCMB, discovered the most extremegalaxy cluster and made the first statistical detection of the motions ofclusters of galaxies via the pairwise kinematicSunyaev–Zeldovich effect.[3]
ACT was built in 2007 and saw first light in October 2007 with its first receiver, the MillimeterBolometer Array Camera (MBAC). ACT had two major receiver upgrades which enabled polarization sensitive observations: ACTPol[4] (2013–2016) and Advanced ACT[5] (2017–2022). ACT observations ended in mid-2022. ACT is funded by the USNational Science Foundation.
Measurements ofcosmic microwave background radiation (CMB) by experiments such asCOBE,BOOMERanG,WMAP,CBI, theSouth Pole Telescope and many others, have greatly advanced our knowledge of cosmology, particularly the early evolution of the universe. At the arcminute resolutions probed by ACT, the Sunyaev–Zeldovich effect, by whichgalaxy clusters leave an imprint on the CMB, is prominent. This method of detection provides aredshift-independent measurement of the mass of the clusters, meaning that very distant, ancient clusters are as easy to detect as nearby clusters.
Atacama Cosmology Telescope observing patches and depth map
Detection of galaxy clusters and follow-up measurements invisible andX-ray light, provide a picture of the evolution of structure in the universe since theBig Bang. This is used to improve our understanding of the nature of the mysteriousdark energy which seems to be a dominant component of the universe.
High sensitivity observations of the cosmic microwave background radiation allow precision measurements of cosmological parameters, detection of galaxy clusters among other scientific goals, probing the early and late stages in the history of the evolution of the universe.
Water vapor in the atmosphere emits microwave radiation which contaminates measurements of the CMB, for this reason CMB telescopes benefit from arid, high-altitude locations. ACT is located in the dry and high (yet easily accessible) Chajnantor plateau in theAndean mountains in theAtacama Desert in northern Chile. Due to the exceptional observing conditions of the Atacama Desert and its accessibility by road and nearby ports, several other observatories are located in the region, includingCBI,ASTE,Nanten,APEX andALMA. These astronomical observatories and telescopes form theLlano de Chajnantor Observatory, a cluster of astronomical telescopes primarily in millimeter and sub-millimeter wavelengths.
The Atacama Cosmology Telescope viewed from the top of the outer ground screen. The top half of the segmented, primary mirror can be seen above the inner ground screen that moves with the telescope.The Atacama Cosmology Telescope. In this picture, the ground screen had not yet been completed, allowing the telescope to be seen.
The ACT is an off-axisGregorian telescope. This off-axis configuration is beneficial to minimize artifacts in the point spread function. The telescope reflectors consist of a six-metre (236 in) primary mirror and a two-metre (79 in) secondary mirror. Both mirrors are composed of segments, consisting of 71 (primary) and 11 (secondary) aluminum panels. These panels follow the shape of an ellipsoid of revolution and are carefully aligned to form a joint surface. Unlike most telescopes which track the rotating sky during observation, the ACT observes the sky by keeping the telescope oriented at a constant elevation and by scanning back and forth in azimuth at the relatively rapid rate of two degrees per second. The rotating portion of the telescope weighs approximately 32 tonnes (35 short tons), creating a substantial engineering challenge. A ground screen surrounding the telescope blocks contamination from microwave radiation emitted by the ground. The design, manufacture and construction of the telescope were done byDynamic Structures inVancouver,British Columbia.
ACT can accommodate three instrument cameras simultaneously. Over time these cameras were upgraded from the original MBAC design to the Advanced ACT instrument progressively adding more features like polarization sensitivity and the ability to sense multiple frequencies in one instrument module. Each camera in ACT consists of a three lens system, the Gregorian focus is reimaged into a detector focal plane, a Lyot stop reimages the primary mirror allowing stray light mitigation.
The three lenses in ACT are made of cryogenically cooled anti-reflection coated silicon, a desirable material for instruments in the millimeter due to its high index of refraction (n=3). Anti-reflection coatings in ACTPol and AdvACT are made of sub-wavelength structured metamaterial silicon, an innovation in ground based CMB telescopes at the time. The optical components and the detector module are kept at a vacuum with a plastic window. A stack of filters reject infra-red radiation which is detrimental for mm-wavelength observations.
Radiation is thermally coupled to transition-edge sensor bolometers, which are read out using an array of SQUIDs.
Observations are made at resolutions of about anarcminute (1/60th of a degree) in three frequencies: 145 GHz, 215 GHz and 280 GHz. Each frequency is measured by a 3 cm × 3 cm (1.2 in × 1.2 in), 1024 element array, for a total of 3072 detectors. The detectors are superconductingtransition-edge sensors, a technology whose high sensitivity allows measurements of the temperature of the CMB to within a few millionths of a degree.[16] A system ofcryogenicheliumrefrigerators keep the detectors a third of a degree aboveabsolute zero.
ACT has had three generations of cameras. Each camera is the result of the development of specialized detector technology which has been optimized through the years. These cameras take advantage of superconducting transition edgesensor arrays to achieve high sensitivity.
The first array of cameras to populate the ACT focal plane (MBAC) consisted of three cameras where each one was sensitive to its own band and had no polarization sensitivity. The second generation of cameras (ACTPol) added polarization sensitivity and the first camera to be sensitive to two bands (dichroic). The third generation of cameras (AdvACT) incorporated the advances achieved in ACTPol, which allowed all cameras to be sensitive to two bands.
^The Receiver Lab Telescope (RLT), an 80 cm (31 in) instrument, is higher at 5,525 m (18,125 ft), but is not permanent as it is fixed to the roof of a movable shipping container.[2] The 2009University of Tokyo Atacama Observatory is significantly higher than both.
^Marrone; et al. (2005). "Observations in the 1.3 and 1.5 THz Atmospheric Windows with the Receiver Lab Telescope".Sixteenth International Symposium on Space Terahertz Technology: 64.arXiv:astro-ph/0505273.Bibcode:2005stt..conf...64M.
^Henderson, S. W.; Allison, R.; Austermann, J.; Baildon, T.; Battaglia, N.; Beall, J. A.; Becker, D.; De Bernardis, F.; Bond, J. R.; Calabrese, E.; Choi, S. K. (1 August 2016). "Advanced ACTPol Cryogenic Detector Arrays and Readout".Journal of Low Temperature Physics.184 (3):772–779.arXiv:1510.02809.Bibcode:2016JLTP..184..772H.doi:10.1007/s10909-016-1575-z.ISSN1573-7357.S2CID53411729.
^Choi, Steve K.; Hasselfield, Matthew; Ho, Shuay-Pwu Patty; Koopman, Brian; Lungu, Marius; Abitbol, Maximilian H.; Addison, Graeme E.; Ade, Peter A. R.; Aiola, Simone; Alonso, David; Amiri, Mandana; Amodeo, Stefania; Angile, Elio; Austermann, Jason E.; Baildon, Taylor (30 December 2020). "The Atacama Cosmology Telescope: a measurement of the Cosmic Microwave Background power spectra at 98 and 150 GHz".Journal of Cosmology and Astroparticle Physics.2020 (12): 045.arXiv:2007.07289.doi:10.1088/1475-7516/2020/12/045.ISSN1475-7516.S2CID220525420.
^Madhavacheril, Mathew;Sehgal, Neelima; Allison, Rupert; Battaglia, Nick; Bond, J. Richard; Calabrese, Erminia; Caligiuri, Jerod; Coughlin, Kevin; Crichton, Devin; Datta, Rahul; Devlin, Mark J.; Dunkley, Joanna; Dünner, Rolando; Fogarty, Kevin; Grace, Emily; Hajian, Amir; Hasselfield, Matthew; Hill, J. Colin; Hilton, Matt; Hincks, Adam D.; Hlozek, Renée; Hughes, John P.; Kosowsky, Arthur; Louis, Thibaut; Lungu, Marius; McMahon, Jeff; Moodley, Kavilan; Munson, Charles; Naess, Sigurd; Nati, Federico; Newburgh, Laura; Niemack, Michael D.; Page, Lyman A.; Partridge, Bruce; Schmitt, Benjamin; Sherwin, Blake D.; Sievers, Jon; Spergel, David N.; Staggs, Suzanne T.; Thornton, Robert; Van Engelen, Alexander; Ward, Jonathan T.; Wollack, Edward J. (13 April 2015). "Evidence of Lensing of the Cosmic Microwave Background by Dark Matter Halos".Physical Review Letters.114 (15).arXiv:1411.7999.doi:10.1103/PhysRevLett.114.151302.