A. Foster
Case Western Reserve University
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Journal of Low Temperature Physics | 2018
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
The third-generation South Pole Telescope camera is designed to measure the cosmic microwave background across three frequency bands (centered at 95, 150 and 220xa0GHz) with
arXiv: Instrumentation and Methods for Astrophysics | 2018
A. Nadolski; A. M. Kofman; J. D. Vieira; Peter A. R. Ade; Z. Ahmed; A. J. Anderson; J. S. Avva; Ritoban Basu Thakur; A. N. Bender; B. A. Benson; J. E. Carlstrom; F. W. Carter; T. Cecil; C. L. Chang; Jean Francois Cliche; A. Cukierman; Tijmen de Haan; Junjia Ding; M. Dobbs; D. Dutcher; Wendy Everett; A. Foster; Jianyiang Fu; Jason Gallichio; A. Gilbert; John Groh; R. Guyser; N. W. Halverson; A. H. Harke-Hosemann; N. L. Harrington
arXiv: Instrumentation and Methods for Astrophysics | 2018
Z. Ahmed; Ritoban Basu Thakur; A. N. Bender; B. A. Benson; J. E. Carlstrom; F. W. Carter; Thomas W. Cecil; C. L. Chang; Jean-François Cliche; A. Cukierman; Tijmen de Haan; Junjia Ding; M. Dobbs; Wendeline Everett; A. Foster; A. Gilbert; John Groh; N. W. Halverson; A. H. Harke-Hosemann; N. L. Harrington; J. W. Henning; W. L. Holzapfel; N. Huang; K. D. Irwin; O. Jeong; M. Jonas; Trupti Khaire; A. M. Kofman; M. Korman; D. Kubik
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arXiv: Instrumentation and Methods for Astrophysics | 2018
F. W. Carter; Thomas W. Cecil; C. L. Chang; Hsaio-Mei Cho; Jean-François Cliche; T. M. Crawford; A. Cukierman; E. V. Denison; Tijmen de Haan; Junjia Ding; M. Dobbs; D. Dutcher; Wendeline Everett; A. Foster; John Groh; A. Gilbert; N. W. Halverson; A. H. Harke-Hosemann; N. L. Harrington; J. W. Henning; G. C. Hilton; G. P. Holder; W. L. Holzapfel; N. Huang; K. D. Irwin; O. Jeong; M. Jonas; Trupti Khaire; Lloyd Knox; A. M. Kofman
arXiv: Instrumentation and Methods for Astrophysics | 2018
J. A. Sobrin; Peter A. R. Ade; Z. Ahmed; A. J. Anderson; J. S. Avva; Ritoban Basu Thakur; Jean-François Cliche; A. Cukierman; Tijmen de Haan; Junjia Ding; M. Dobbs; D. Dutcher; Wendeline Everett; A. Foster; Jason Gallichio; A. Gilbert; John Groh; Sam Guns; N. W. Halverson; A. H. Harke-Hosemann; N. L. Harrington; J. W. Henning; W. L. Holzapfel; N. Huang; K. D. Irwin; O. Jeong; M. Jonas; Trupti Khaire; A. M. Kofman; M. Korman
∼xa016,000 transition-edge sensor (TES) bolometers. Each multichroic array element on a detector wafer has a broadband sinuous antenna that couples power to six TESs, one for each of the three observing bands and both polarizations, via lumped element filters. Ten detector wafers populate the detector array, which is coupled to the sky via a large-aperture optical system. Here we present the frequency band characterization with Fourier transform spectroscopy, measurements of optical time constants, beam properties, and optical and polarization efficiencies of the detector array. The detectors have frequency bands consistent with our simulations and have high average optical efficiency which is 86, 77 and 66% for the 95, 150 and 220xa0GHz detectors. The time constants of the detectors are mostly between 0.5 and 5 ms. The beam is round with the correct size, and the polarization efficiency is more than 90% for most of the bolometers.
Journal of Low Temperature Physics | 2018
W. Everett; 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; A. Foster; R. N. Gannon; A. Gilbert; John Groh; N. W. Halverson; A. H. Harke-Hosemann; N. L. Harrington; J. W. Henning; G. C. Hilton; W. L. Holzapfel
The desire for higher sensitivity has driven ground-based cosmic microwave background (CMB) experiments to employ ever larger focal planes, which in turn require larger reimaging optics. Practical limits to the maximum size of these optics motivates the development of quasi-optically-coupled (lenslet-coupled), multi-chroic detectors. These detectors can be sensitive across a broader bandwidth compared to waveguide-coupled detectors. However, the increase in bandwidth comes at a cost: the lenses (up to ~700 mm diameter) and lenslets (~5 mm diameter, hemispherical lenses on the focal plane) used in these systems are made from high-refractive-index materials (such as silicon or amorphous aluminum oxide) that reflect nearly a third of the incident radiation. In order to maximize the faint CMB signal that reaches the detectors, the lenses and lenslets must be coated with an anti-reflective (AR) material. The AR coating must maximize radiation transmission in scientifically interesting bands and be cryogenically stable. Such a coating was developed for the third generation camera, SPT-3G, of the South Pole Telescope (SPT) experiment, but the materials and techniques used in the development are general to AR coatings for mm-wave optics. The three-layer polytetra uoroethylene-based AR coating is broadband, inexpensive, and can be manufactured with simple tools. The coating is field tested; AR coated focal plane elements were deployed in the 2016-2017 austral summer and AR coated reimaging optics were deployed in 2017-2018.
Journal of Low Temperature Physics | 2018
J. S. Avva; Peter A. R. Ade; Z. Ahmed; A. J. Anderson; J. E. Austermann; R. Basu Thakur; D. Barron; 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; T. Elleflot; W. Everett; A. Foster; R. N. Gannon; A. Gilbert; John Groh; N. W. Halverson; A. H. Harke-Hosemann; N. L. Harrington; M. Hasegawa
The third-generation instrument for the 10-meter South Pole Telescope, SPT-3G, was first installed in January 2017. In addition to completely new cryostats, secondary telescope optics, and readout electronics, the number of detectors in the focal plane has increased by an order of magnitude from previous instruments to ~16,000. The SPT-3G focal plane consists of ten detector modules, each with an array of 269 trichroic, polarization-sensitive pixels on a six-inch silicon wafer. Within each pixel is a broadband, dual-polarization sinuous antenna; the signal from each orthogonal linear polarization is divided into three frequency bands centered at 95, 150, and 220 GHz by in-line lumped element filters and transmitted via superconducting microstrip to Ti/Au transition-edge sensor (TES) bolometers. Properties of the TES film, microstrip filters, and bolometer island must be tightly controlled to achieve optimal performance. For the second year of SPT-3G operation, we have replaced all ten wafers in the focal plane with new detector arrays tuned to increase mapping speed and improve overall performance. Here we discuss the TES superconducting transition temperature and normal resistance, detector saturation power, bandpasses, optical efficiency, and full array yield for the 2018 focal plane.
Journal of Low Temperature Physics | 2018
A. J. Anderson; Peter A. R. Ade; Z. Ahmed; J. E. Austermann; J. S. Avva; P. S. Barry; R. Basu Thakur; A. N. Bender; B. A. Benson; L. E. Bleem; K. L. Byrum; J. E. Carlstrom; F. W. Carter; T. Cecil; C. L. Chang; H. M. Cho; Jean-François Cliche; T. M. Crawford; A. Cukierman; E. V. Denison; T. de Haan; Junjia Ding; M. Dobbs; D. Dutcher; W. Everett; A. Foster; R. N. Gannon; A. Gilbert; John Groh; N. W. Halverson
The South Pole Telescope (SPT) is a millimeter-wavelength telescope designed for high-precision measurements of the cosmic microwave background (CMB). The SPT measures both the temperature and polarization of the CMB with a large aperture, resulting in high resolution maps sensitive to signals across a wide range of angular scales on the sky. With these data, the SPT has the potential to make a broad range of cosmological measurements. These include constraining the effect of massive neutrinos on large-scale structure formation as well as cleaning galactic and cosmological foregrounds from CMB polarization data in future searches for inflationary gravitational waves. The SPT began observing in January 2017 with a new receiver (SPT-3G) containing ~16,000 polarization-sensitive transition-edge sensor bolometers. Several key technology developments have enabled this large-format focal plane, including advances in detectors, readout electronics, and large millimeter-wavelength optics. We discuss the implementation of these technologies in the SPT-3G receiver as well as the challenges they presented. In late 2017 the implementations of all three of these technologies were modified to optimize total performance. Here, we present the current instrument status of the SPT-3G receiver.
Journal of Low Temperature Physics | 2018
F. W. Carter; 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; T. Cecil; C. L. Chang; Jean-François Cliche; A. Cukierman; E. V. Denison; T. de Haan; Junjia Ding; Ralu Divan; M. Dobbs; D. Dutcher; W. 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
The SPT-3G receiver was commissioned in early 2017 on the 10-meter South Pole Telescope (SPT) to map anisotropies in the cosmic microwave background (CMB). New optics, detector, and readout technologies have yielded a multichroic, high-resolution, low-noise camera with impressive throughput and sensitivity, offering the potential to improve our understanding of inflationary physics, astroparticle physics, and growth of structure. We highlight several key features and design principles of the new receiver, and summarize its performance to date.
Journal of Low Temperature Physics | 2018
C. M. Posada; 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; Ralu Divan; M. Dobbs; D. Dutcher; W. Everett; A. Foster; R. N. Gannon; A. Gilbert; J. C. Groh; N. W. Halverson; A. H. Harke-Hosemann; N. L. Harrington; J. W. Henning
During the austral summer of 2016–2017, the third-generation camera, SPT-3G, was installed on the South Pole Telescope, increasing the detector count in the focal plane by an order of magnitude relative to the previous generation. Designed to map the polarization of the cosmic microwave background, SPT-3G contains ten 6