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Dive into the research topics where J. E. Austermann is active.

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Featured researches published by J. E. Austermann.


Monthly Notices of the Royal Astronomical Society | 2017

A deep ALMA image of the Hubble Ultra Deep Field

James Dunlop; Ross J. McLure; A. D. Biggs; J. E. Geach; M. J. Michałowski; R. J. Ivison; W. Rujopakarn; E. van Kampen; Allison Kirkpatrick; Alexandra Pope; D. Scott; A. M. Swinbank; Thomas Targett; I. Aretxaga; J. E. Austermann; Philip Best; Victoria Bruce; Edward L. Chapin; S. Charlot; Michele Cirasuolo; K. E. K. Coppin; Richard S. Ellis; Steven L. Finkelstein; Christopher C. Hayward; David H. Hughes; E. Ibar; P. Jagannathan; Sadegh Khochfar; M. P. Koprowski; Desika Narayanan

We present the results of the first, deep Atacama Large Millimeter Array (ALMA) imaging covering the full ≃4.5 arcmin2 of the Hubble Ultra Deep Field (HUDF) imaged with Wide Field Camera 3/IR on HST. Using a 45-pointing mosaic, we have obtained a homogeneous 1.3-mm image reaching σ1.3 ≃ 35 μJy, at a resolution of ≃0.7 arcsec. From an initial list of ≃50 > 3.5σ peaks, a rigorous analysis confirms 16 sources with S1.3 > 120 μJy. All of these have secure galaxy counterparts with robust redshifts (〈z〉 = 2.15). Due to the unparalleled supporting data, the physical properties of the ALMA sources are well constrained, including their stellar masses (M*) and UV+FIR star formation rates (SFR). Our results show that stellar mass is the best predictor of SFR in the high-redshift Universe; indeed at z ≥ 2 our ALMA sample contains seven of the nine galaxies in the HUDF with M* ≥ 2 × 1010u2009M⊙, and we detect only one galaxy at z > 3.5, reflecting the rapid drop-off of high-mass galaxies with increasing redshift. The detections, coupled with stacking, allow us to probe the redshift/mass distribution of the 1.3-mm background down to S1.3 ≃ 10u2009μJy. We find strong evidence for a steep star-forming ‘main sequence’ at z ≃ 2, with SFR ∝M* and a mean specific SFR ≃ 2.2 Gyr−1. Moreover, we find that ≃85u2009peru2009cent of total star formation at z ≃ 2 is enshrouded in dust, with ≃65u2009peru2009cent of all star formation at this epoch occurring in high-mass galaxies (M* > 2 × 1010u2009M⊙), for which the average obscured:unobscured SF ratio is ≃200. Finally, we revisit the cosmic evolution of SFR density; we find this peaks at z ≃ 2.5, and that the star-forming Universe transits from primarily unobscured to primarily obscured at z ≃ 4.


Journal of Low Temperature Physics | 2016

Advanced ACTPol Cryogenic Detector Arrays and Readout

S. Henderson; Rupert Allison; J. E. Austermann; T. Baildon; Nick Battaglia; James A. Beall; D. Becker; F. De Bernardis; J. R. Bond; Edward J. Wollack

Advanced ACTPol is a polarization-sensitive upgrade for the 6xa0m aperture Atacama Cosmology Telescope, adding new frequencies and increasing sensitivity over the previous ACTPol receiver. In 2016, Advanced ACTPol will begin to map approximately half the sky in five frequency bands (28–230xa0GHz). Its maps of primary and secondary cosmic microwave background anisotropies—imaged in intensity and polarization at few arcminute-scale resolution—will enable precision cosmological constraints and also a wide array of cross-correlation science that probes the expansion history of the universe and the growth of structure via gravitational collapse. To accomplish these scientific goals, the Advanced ACTPol receiver will be a significant upgrade to the ACTPol receiver, including four new multichroic arrays of cryogenic, feedhorn-coupled AlMn transition edge sensor polarimeters (fabricated on 150 mm diameter wafers); a system of continuously rotating meta-material silicon half-wave plates; and a new multiplexing readout architecture which uses superconducting quantum interference devices and time division to achieve a 64-row multiplexing factor. Here we present the status and scientific goals of the Advanced ACTPol instrument, emphasizing the design and implementation of the Advanced ACTPol cryogenic detector arrays.


Scopus | 2010

Mid-infrared spectroscopy of candidate active galactic nuclei-dominated submillimeter galaxies

K. Coppin; Ian Smail; A. M. Swinbank; Alexandra Pope; Karin Menendez-Delmestre; D. M. Alexander; James Dunlop; R. J. Ivison; Amj Mortier; E. Egami; Jared M. Gabor; E. Ibar; J. E. Austermann; A. W. Blain; Sydney Chapman; D. L. Clements; M. Rowan-Robinson; Loretta Dunne; S. Dye; D. Farrah; David H. Hughes; M. J. Page; D. Scott; Chris Simpson; M. Vaccari; Yun

Spitzer spectroscopy has revealed that ≃80% of submm galaxies (SMGs) are starburst (SB)-dominated in the mid-infrared. Here we focus on the remaining ≃20% that show signs of harboring powerful active galactic nuclei (AGNs). We have obtained Spitzer-InfraRed Spectrograph spectroscopy of a sample of eight SMGs that are candidates for harboring powerful AGNs on the basis of IRAC color selection (S_(8 μm)/S_(4.5 μm) > 2, i.e., likely power-law mid-infrared spectral energy distributions). SMGs with an AGN dominating (≳50%) their mid-infrared emission could represent the missing link sources in an evolutionary sequence involving a major merger. First of all, we detect polycyclic aromatic hydrocarbon (PAH) features in all of the SMGs, indicating redshifts from 2.5 to 3.4, demonstrating the power of the mid-infrared to determine redshifts for these optically faint dusty galaxies. Second, we see signs of both star formation (from the PAH features) and AGN activity (from continuum emission) in our sample: 62% of the sample are AGN-dominated in the mid-infrared with a median AGN content of 56%, compared with 1.65 works well at selecting mid-infrared energetically dominant AGNs in SMGs, implying a duty cycle of ~15% if all SMGs go through a subsequent mid-infrared AGN-dominated phase in the proposed evolutionary sequence.


Superconductor Science and Technology | 2015

Fabrication of large dual-polarized multichroic TES bolometer arrays for CMB measurements with the SPT-3G camera

C. M. Posada; Peter A. R. Ade; Z. Ahmed; K. Arnold; J. E. Austermann; A. N. Bender; L. E. Bleem; B. A. Benson; K. L. Byrum; J. E. Carlstrom; C. L. Chang; H. M. Cho; S. T. Ciocys; Jean-François Cliche; T. M. Crawford; A. Cukierman; David A. Czaplewski; Junjia Ding; Ralu Divan; T. de Haan; M. Dobbs; D. Dutcher; W. Everett; A. Gilbert; N. W. Halverson; N. L. Harrington; K. Hattori; J. W. Henning; G. C. Hilton; W. L. Holzapfel

This work presents the procedures used at Argonne National Laboratory to fabricate large arrays of multichroic transition-edge sensor (TES) bolometers for cosmic microwave background (CMB) measurements. These detectors will be assembled into the focal plane for the SPT-3G camera, the third generation CMB camera to be installed in the South Pole Telescope. The complete SPT-3G camera will have approximately 2690 pixels, for a total of 16 140 TES bolometric detectors. Each pixel is comprised of a broad-band sinuous antenna coupled to a Nb microstrip line. In-line filters are used to define the different bands before the millimeter-wavelength signal is fed to the respective Ti/Au TES bolometers. There are six TES bolometer detectors per pixel, which allow for measurements of three band-passes (95, 150 and 220 GHz) and two polarizations. The steps involved in the monolithic fabrication of these detector arrays are presented here in detail. Patterns are defined using a combination of stepper and contact lithography. The misalignment between layers is kept below 200 nm. The overall fabrication involves a total of 16 processes, including reactive and magnetron sputtering, reactive ion etching, inductively coupled plasma etching and chemical etching.


The Astrophysical Journal | 2018

Measurements of the Temperature and E-mode Polarization of the CMB from 500 Square Degrees of SPTpol Data

J. W. Henning; J. T. Sayre; C. L. Reichardt; Peter A. R. Ade; A. J. Anderson; J. E. Austermann; James A. Beall; A. N. Bender; B. A. Benson; L. E. Bleem; J. E. Carlstrom; C. L. Chang; H. C. Chiang; H. M. Cho; R. Citron; C. Corbett Moran; T. M. Crawford; A. T. Crites; T. de Haan; M. Dobbs; Wendeline Everett; J. Gallicchio; E. M. George; A. Gilbert; N. W. Halverson; N. L. Harrington; G. C. Hilton; Gilbert P. Holder; W. L. Holzapfel; S. Hoover

We present measurements of the


IEEE Transactions on Applied Superconductivity | 2017

Optimization of Transition Edge Sensor Arrays for Cosmic Microwave Background Observations With the South Pole Telescope

Junjia Ding; Peter A. R. Ade; A. J. Anderson; J. S. Avva; Z. Ahmed; K. Arnold; J. E. Austermann; A. N. Bender; B. A. Benson; L. E. Bleem; K. L. Byrum; J. E. Carlstrom; F. W. Carter; C. L. Chang; H. M. Cho; Jean-François Cliche; A. Cukierman; David A. Czaplewski; Ralu Divan; T. de Haan; M. Dobbs; D. Dutcher; W. Everett; A. Gilbert; R. N. Gannon; R. Guyser; N. W. Halverson; N. L. Harrington; K. Hattori; J. W. Henning

E


Journal of Low Temperature Physics | 2016

Design and Deployment of a Multichroic Polarimeter Array on the Atacama Cosmology Telescope

Rahul Datta; J. E. Austermann; James A. Beall; D. Becker; Kevin Coughlin; Shannon M. Duff; Patricio A. Gallardo; Emily Grace; Matthew Hasselfield; S. Henderson; G. C. Hilton; S. P. Ho; J. Hubmayr; Brian J. Koopman; Jeff Van Lanen; D. Li; J. J. McMahon; Charles Munson; F. Nati; Michael D. Niemack; Lyman A. Page; C. G. Pappas; Maria Salatino; Benjamin L. Schmitt; A. Schillaci; Sara M. Simon; Suzanne T. Staggs; J. R. Stevens; Eve M. Vavagiakis; Jonathan T. Ward

-mode polarization angular auto-power spectrum (


The Astrophysical Journal | 2017

CMB Polarization B-mode Delensing with SPTpol and Herschel

A. Manzotti; K. T. Story; W. L. K. Wu; J. E. Austermann; James A. Beall; A. N. Bender; B. A. Benson; L. E. Bleem; J. J. Bock; J. E. Carlstrom; C. L. Chang; H. C. Chiang; H. M. Cho; R. Citron; A. Conley; T. M. Crawford; A. T. Crites; T. de Haan; M. Dobbs; Scott Dodelson; W. Everett; J. Gallicchio; E. M. George; A. Gilbert; N. W. Halverson; N. L. Harrington; J. W. Henning; G. C. Hilton; Gilbert P. Holder; W. L. Holzapfel

EE


Proceedings of SPIE | 2016

The design and characterization of wideband spline-profiled feedhorns for Advanced ACTPol

Sara M. Simon; J. E. Austermann; James A. Beall; Steve K. Choi; Kevin Coughlin; Shannon M. Duff; Patricio A. Gallardo; S. Henderson; Felicity B. Hills; Shuay Pwu Patty Ho; J. Hubmayr; Alec Josaitis; Brian J. Koopman; Jeff McMahon; F. Nati; Laura Newburgh; Michael D. Niemack; Maria Salatino; Alessandro Schillaci; Benjamin L. Schmitt; Suzanne T. Staggs; Eve M. Vavagiakis; Jonathan T. Ward; Edward J. Wollack

) and temperature-


Journal of Low Temperature Physics | 2018

Optical characterization of the SPT-3G camera

Z. Pan; Peter A. R. Ade; Z. Ahmed; A. J. Anderson; J. E. Austermann; J. S. Avva; R. Basu Thakur; A. N. Bender; B. A. Benson; J. E. Carlstrom; F. W. Carter; T. Cecil; C. L. Chang; Jean-François Cliche; A. Cukierman; E. V. Denison; T. de Haan; Junjia Ding; M. Dobbs; D. Dutcher; Wendeline Everett; A. Foster; R. N. Gannon; A. Gilbert; J. C. Groh; N. W. Halverson; A. H. Harke-Hosemann; N. L. Harrington; J. W. Henning; G. C. Hilton

E

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G. C. Hilton

National Institute of Standards and Technology

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J. Hubmayr

National Institute of Standards and Technology

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James A. Beall

National Institute of Standards and Technology

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Shannon M. Duff

National Institute of Standards and Technology

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Grant W. Wilson

University of Massachusetts Boston

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K. S. Scott

National Radio Astronomy Observatory

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I. Aretxaga

National Autonomous University of Mexico

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N. W. Halverson

University of Colorado Boulder

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