D. Ferrusca
University of California, Berkeley
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Monthly Notices of the Royal Astronomical Society | 2010
J. E. Austermann; James Dunlop; T. A. Perera; K. S. Scott; Grant W. Wilson; I. Aretxaga; David H. Hughes; Omar Almaini; Edward L. Chapin; S. C. Chapman; Michele Cirasuolo; D. L. Clements; K. E. K. Coppin; Loretta Dunne; Simon Dye; Stephen Anthony Eales; E. Egami; D. Farrah; D. Ferrusca; Stephen Flynn; D. Haig; M. Halpern; E. Ibar; R. J. Ivison; E. van Kampen; Young-Woon Kang; Sungeun Kim; Cedric G. Lacey; James D. Lowenthal; Philip Daniel Mauskopf
We present the first results from the largest deep extragalactic mm-wavelength survey undertaken to date. These results are derived from maps covering over 0.7 deg2, made at λ= 1.1 mm, using the AzTEC continuum camera mounted on the James Clerk Maxwell Telescope. The maps were made in the two fields originally targeted at λ= 850 μm with the Submillimetre Common-User Bolometer Array (SCUBA) in the SCUBA Half-Degree Extragalactic Survey (SHADES) project, namely the Lockman Hole East (mapped to a depth of 0.9–1.3 mJy rms) and the Subaru/XMM–Newton Deep Field (mapped to a depth of 1.0–1.7 mJy rms). The wealth of existing and forthcoming deep multifrequency data in these two fields will allow the bright mm source population revealed by these new wide-area 1.1 mm images to be explored in detail in subsequent papers. Here, we present the maps themselves, a catalogue of 114 high-significance submillimetre galaxy detections, and a thorough statistical analysis leading to the most robust determination to date of the 1.1 mm source number counts. These new maps, covering an area nearly three times greater than the SCUBA SHADES maps, currently provide the largest sample of cosmological volumes of the high-redshift Universe in the mm or sub-mm. Through careful comparison, we find that both the Cosmic Evolution Survey (COSMOS) and the Great Observatories Origins Deep Survey (GOODS) North fields, also imaged with AzTEC, contain an excess of mm sources over the new 1.1 mm source-count baseline established here. In particular, our new AzTEC/SHADES results indicate that very luminous high-redshift dust enshrouded starbursts (S1.1mm > 3 mJy) are 25–50 per cent less common than would have been inferred from these smaller surveys, thus highlighting the potential roles of cosmic variance and clustering in such measurements. We compare number count predictions from recent models of the evolving mm/sub-mm source population to these sub-mm bright galaxy surveys, which provide important constraints for the ongoing refinement of semi-analytic and hydrodynamical models of galaxy formation, and find that all available models overpredict the number of bright submillimetre galaxies found in this survey.
Monthly Notices of the Royal Astronomical Society | 2010
K. S. Scott; Min S. Yun; Graham Wallace Wilson; J. E. Austermann; E. Aguilar; Itziar Aretxaga; Hajime Ezawa; D. Ferrusca; Bunyo Hatsukade; David H. Hughes; Daisuke Iono; Mauro Giavalisco; Ryohei Kawabe; Kotaro Kohno; Philip Daniel Mauskopf; Tai Oshima; T. A. Perera; J. Rand; Yoichi Tamura; Tomoka Tosaki; M. Velazquez; Christina C. Williams; M. Zeballos
We present the first results from a 1.1mm confusion-limited map of the Great Observatories Origins Deep Survey-South (GOODS-S) taken with the AzTEC camera on the Atacama Submillimeter Telescope Experiment. We imaged a 270arcmin 2 field to a 1� depth of 0.48 0.73mJy/beam, making this one of the deepest blank-field surveys at mm-wavelengths ever achieved. Although by traditional standards our GOODS-S map is extremely confused due to a sea of faint underlying sources, we demonstrate through simulations that our source identification and number counts analyses are robust, and the techniques discussed in this paper are relevant for other deeply confused surveys. We find a total of 41 dusty starburst galaxies with signal to noise ratios S/N > 3.5 within this uniformly covered region, where only two are expected to be false detections, and an additional seven robust source candidates located in the noisier (1� � 1mJy/beam) outer region of the map. We derive the 1.1mm number counts from this field using two different methods: a fluctuation or “P(d)” analysis and a semi-Bayesian technique, and find that both methods give consistent results. Our data are well-fit by a Schechter function model
Monthly Notices of the Royal Astronomical Society | 2016
K. Harrington; Min S. Yun; Ryan Cybulski; Grant W. Wilson; I. Aretxaga; Miguel Chavez; V. De la Luz; Neal R. Erickson; D. Ferrusca; A. Gallup; David H. Hughes; A. Montaña; Gopal Narayanan; D. Sánchez-Argüelles; F. P. Schloerb; Kamal Souccar; Elena Terlevich; Roberto Terlevich; M. Zeballos; J. A. Zavala
We present 8.5 arcsec resolution 1.1mm continuum imaging and CO spectroscopic redshift measurements of eight extremely bright submillimetre galaxies identified from the Planck and Herschel surveys, taken with the Large Millimeter Telescopes AzTEC and Redshift Search Receiver instruments. We compiled a candidate list of high redshift galaxies by cross-correlating the Planck Surveyor missions highest frequency channel (857 GHz, FWHM = 4.5 arcmin) with the archival Herschel Spectral and Photometric Imaging Receiver (SPIRE) imaging data, and requiring the presence of a unique, single Herschel counterpart within the 150 arcsec search radius of the Planck source positions with 350 micron flux density larger than 100 mJy, excluding known blazars and foreground galaxies. All eight candidate objects observed are detected in 1.1mm continuum by AzTEC bolometer camera, and at least one CO line is detected in all cases with a spectroscopic redshift between 1.3 < z(CO) < 3.3. Their infrared spectral energy distributions mapped using the Herschel and AzTEC photometry are consistent with cold dust emission with characteristic temperature between
THE THIRTEENTH INTERNATIONAL WORKSHOP ON LOW TEMPERATURE DETECTORS—LTD13 | 2009
B. Westbrook; Peter A. R. Ade; A. N. Bender; H. M. Cho; John Clarke; M. Dobbs; D. Ferrusca; N. W. Halverson; W. L. Holzapfel; B. R. Johnson; J. Kennedy; Z. Kermish; T. M. Lanting; A. T. Lee; M. Lueker; J. Mehl; X. Meng; T. Plagge; C. L. Reichardt; P. L. Richards; D. Schwan; E. Shirokoff; H. Spieler
T_d
arXiv: Instrumentation and Methods for Astrophysics | 2018
Sean Bryan; J. E. Austermann; Philip Daniel Mauskopf; Giles Novak; Sara M. Simon; Grant W. Wilson; Jeff McMahon; D. Ferrusca; A. Montaña; D. Sánchez-Argüelles
= 43 K and 84 K. With apparent infrared luminosity of up to L(IR) =
Monthly Notices of the Royal Astronomical Society | 2018
M. Zeballos; I. Aretxaga; David H. Hughes; A. Humphrey; Grant W. Wilson; J. E. Austermann; James Dunlop; H. Ezawa; D. Ferrusca; Bunyo Hatsukade; R. J. Ivison; Ryohei Kawabe; Sungeun Kim; Tadayuki Kodama; Kotaro Kohno; A. Montaña; K. Nakanishi; Manolis Plionis; D. Sánchez-Argüelles; J. A. Stevens; Yoichi Tamura; M. Velazquez; M. S. Yun
3\times10^{14} \mu^{-1} L_\odot
Millimeter, Submillimeter, and Far-Infrared Detectors and Instrumentation for Astronomy IX | 2018
T. L. R. Brien; S. Doyle; E. Castillo-Dominguez; D. Ferrusca; David H. Hughes; Enzo Pascale; S. Rowe; Carole Tucker; Peter A. R. Ade; Amber Hornsby; P. S. Barry; Thomas Gascard; Victor Gomez; Peter Charles Hargrave; Josie Parrianen; Abel Perez; Salvador Ventura González
, they are some of the most luminous galaxies ever found (with yet unknown gravitational magnification factor
Ground-based and Airborne Telescopes VII | 2018
David H. Hughes; F. Peter Schloerb; Min Su Yun; Miguel León Chávez; Grant W. Wilson; Gopal Narayanan; Neal R. Erickson; David R. Smith; Kamal Souccar; David M. Gale; José Luis Hernández Rebollar; D. Ferrusca; M. Velázquez; D. Sánchez-Argüelles; Edgar Castillo; I. Aretxaga; Alexandra Pope; Shep Doeleman; A. Montaña; Arturo I. Gómez-Ruiz
\mu
Proceedings of SPIE | 2016
M. Zeballos; D. Ferrusca; David H. Hughes
). The analysis of their spectral energy distributions (SEDs) suggests that star formation is powering the bulk of their extremely large IR luminosities. Derived molecular gas masses of
Proceedings of SPIE | 2006
M. Velázquez; D. Ferrusca; David H. Hughes
M_{H2}=(0.6-7.8)\times 10^{11} M_\odot