2007
DOI: 10.1038/sj.eye.6702916
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“…While 21 cm cosmology faces formidable observational challenges, recent years have seen significant advances toward resolving issues of optimal array design (Beardsley et al 2012;Parsons et al 2012b;Dillon & Parsons 2016), internal systematics (Ewall-Wice et al 2016c; Barry et al 2016;Patil et al 2016;Ewall-Wice et al 2016a), and astrophysical foreground mitigation (Datta et al 2010;Morales et al 2012;Vedantham et al 2012;Parsons et al 2012b;Trott et al 2012;Chapman et al 2012Chapman et al , 2013Thyagarajan et al 2013;Pober et al 2013a;Liu et al 2014a,b;Switzer & Liu 2014;Wolz et al 2013;Moore et al 2015;Thyagarajan et al 2015a,b;Asad et al 2015;Chapman et al 2016;Kohn et al 2016;. Increasingly competitive upper limits have been placed on the red-shifted 21 cm signal, using instruments such as the Donald C. Backer Precision Array for Probing the Epoch of Reionization (PAPER; Parsons et al 2014;Jacobs et al 2015;Ali et al 2015), the Giant Metrewave Radio Telescope (GMRT; Paciga et al 2013), the Murchison Widefield Array (MWA; Dillon et al 2014Dillon et al , 2015Ewall-Wice et al 2016c;Beardsley et al 2016), and the Low Frequency Array (LOFAR; Vedantham et al 2015;Patil et al 2017). Many of these upper limits are stringent enough to be scientifically interesting, and have typically ruled out extremely cold reionization scenarios…”
Section: Introductionmentioning
confidence: 99%
“…While 21 cm cosmology faces formidable observational challenges, recent years have seen significant advances toward resolving issues of optimal array design (Beardsley et al 2012;Parsons et al 2012b;Dillon & Parsons 2016), internal systematics (Ewall-Wice et al 2016c; Barry et al 2016;Patil et al 2016;Ewall-Wice et al 2016a), and astrophysical foreground mitigation (Datta et al 2010;Morales et al 2012;Vedantham et al 2012;Parsons et al 2012b;Trott et al 2012;Chapman et al 2012Chapman et al , 2013Thyagarajan et al 2013;Pober et al 2013a;Liu et al 2014a,b;Switzer & Liu 2014;Wolz et al 2013;Moore et al 2015;Thyagarajan et al 2015a,b;Asad et al 2015;Chapman et al 2016;Kohn et al 2016;. Increasingly competitive upper limits have been placed on the red-shifted 21 cm signal, using instruments such as the Donald C. Backer Precision Array for Probing the Epoch of Reionization (PAPER; Parsons et al 2014;Jacobs et al 2015;Ali et al 2015), the Giant Metrewave Radio Telescope (GMRT; Paciga et al 2013), the Murchison Widefield Array (MWA; Dillon et al 2014Dillon et al , 2015Ewall-Wice et al 2016c;Beardsley et al 2016), and the Low Frequency Array (LOFAR; Vedantham et al 2015;Patil et al 2017). Many of these upper limits are stringent enough to be scientifically interesting, and have typically ruled out extremely cold reionization scenarios…”
Section: Introductionmentioning
confidence: 99%
“…; EDGES, SCI-HI, LEDA, BIGHORNS; Bowman & Rogers 2010;Voytek et al 2014;Greenhill & Bernardi 2012;Sokolowski et al 2015), though space-based observatories will be required to probe the cosmic dawn at z 30 (e.g., the Dark Ages Radio Explorer, (DARE); Burns et al 2012), as the Earth's ionosphere reflects and refracts radio signals at low frequencies (Vedantham et al 2013;Datta et al 2014). Interferometers are in principle capable of measuring the global 21-cm signal, so long as they are compact (Presley et al 2015;Singh et al 2015) or can overcome challenges in lunar occultation techniques (Vedantham et al 2014).…”
Section: Introductionmentioning
confidence: 99%