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Proceedings of SPIE | 2014

SPT-3G: a next-generation cosmic microwave background polarization experiment on the South Pole telescope

B. A. Benson; Peter A. R. Ade; Z. Ahmed; S. W. Allen; K. Arnold; J. E. Austermann; A. N. Bender; L. E. Bleem; J. E. Carlstrom; C. L. Chang; H. M. Cho; Jean-François Cliche; T. M. Crawford; A. Cukierman; T. de Haan; M. Dobbs; D. Dutcher; W. Everett; A. Gilbert; N. W. Halverson; D. Hanson; N. L. Harrington; K. Hattori; J. W. Henning; G. C. Hilton; Gilbert P. Holder; W. L. Holzapfel; K. D. Irwin; R. Keisler; L. Knox

We describe the design of a new polarization sensitive receiver, spt-3g, for the 10-meter South Pole Telescope (spt). The spt-3g receiver will deliver a factor of ~20 improvement in mapping speed over the current receiver, spt-pol. The sensitivity of the spt-3g receiver will enable the advance from statistical detection of B-mode polarization anisotropy power to high signal-to-noise measurements of the individual modes, i.e., maps. This will lead to precise (~0.06 eV) constraints on the sum of neutrino masses with the potential to directly address the neutrino mass hierarchy. It will allow a separation of the lensing and inflationary B-mode power spectra, improving constraints on the amplitude and shape of the primordial signal, either through spt-3g data alone or in combination with bicep2/keck, which is observing the same area of sky. The measurement of small-scale temperature anisotropy will provide new constraints on the epoch of reionization. Additional science from the spt-3g survey will be significantly enhanced by the synergy with the ongoing optical Dark Energy Survey (des), including: a 1% constraint on the bias of optical tracers of large-scale structure, a measurement of the differential Doppler signal from pairs of galaxy clusters that will test General Relativity on ~200Mpc scales, and improved cosmological constraints from the abundance of clusters of galaxies


Proceedings of SPIE | 2012

SPTpol: an instrument for CMB polarization measurements with the South Pole Telescope

J. E. Austermann; K. A. Aird; James A. Beall; D. Becker; A. N. Bender; B. A. Benson; L. E. Bleem; J. Britton; J. E. Carlstrom; C. L. Chang; H. C. Chiang; H. M. Cho; T. M. Crawford; A. T. Crites; A. Datesman; T. de Haan; M. Dobbs; E. M. George; N. W. Halverson; N. L. Harrington; J. W. Henning; G. C. Hilton; G. P. Holder; W. L. Holzapfel; S. Hoover; N. Huang; J. Hubmayr; K. D. Irwin; R. Keisler; J. Kennedy

SPTpol is a dual-frequency polarization-sensitive camera that was deployed on the 10-meter South Pole Telescope in January 2012. SPTpol will measure the polarization anisotropy of the cosmic microwave background (CMB) on angular scales spanning an arcminute to several degrees. The polarization sensitivity of SPTpol will enable a detection of the CMB “B-mode” polarization from the detection of the gravitational lensing of the CMB by large scale structure, and a detection or improved upper limit on a primordial signal due to inationary gravity waves. The two measurements can be used to constrain the sum of the neutrino masses and the energy scale of ination. These science goals can be achieved through the polarization sensitivity of the SPTpol camera and careful control of systematics. The SPTpol camera consists of 768 pixels, each containing two transition-edge sensor (TES) bolometers coupled to orthogonal polarizations, and a total of 1536 bolometers. The pixels are sensitive to light in one of two frequency bands centered at 90 and 150 GHz, with 180 pixels at 90 GHz and 588 pixels at 150 GHz. The SPTpol design has several features designed to control polarization systematics, including: singlemoded feedhorns with low cross-polarization, bolometer pairs well-matched to dfference atmospheric signals, an improved ground shield design based on far-sidelobe measurements of the SPT, and a small beam to reduce temperature to polarization leakage. We present an overview of the SPTpol instrument design, project status, and science projections.


THE THIRTEENTH INTERNATIONAL WORKSHOP ON LOW TEMPERATURE DETECTORS—LTD13 | 2009

Feedhorn‐Coupled TES Polarimeters for Next‐Generation CMB Instruments

K. W. Yoon; J. W. Appel; J. E. Austermann; James A. Beall; D. Becker; B. A. Benson; L. E. Bleem; J. Britton; C. L. Chang; J. E. Carlstrom; H. M. Cho; A. T. Crites; Thomas Essinger-Hileman; W. Everett; N. W. Halverson; J. W. Henning; G. C. Hilton; K. D. Irwin; Jeff McMahon; J. Mehl; S. S. Meyer; Samuel J. Moseley; Michael D. Niemack; Lucas Parker; S. M. Simon; Suzanne T. Staggs; Kongpop U-Yen; C. Visnjic; Edward J. Wollack; Y. Zhao

The next generation of cosmic microwave background (CMB) polarization experiments targeting the signatures of inflation will require unprecedented sensitivities in addition to careful control of systematics. With existing detector technologies approaching the photon noise limit, improvements in system sensitivities must come from ever‐larger focal plane arrays of millimeter‐wave detectors. We report on the design and performance of microfabricated planar orthomode transducer (OMT) coupled TES polarimeters and silicon micromachined platelet feedhorns optimized for scaling to large monolithic arrays. Future versions of these detectors are targeted for deployment in a number of upcoming CMB experiments, including ABS, SPTpol, and ACTpol.


Proceedings of SPIE | 2012

Performance and on-sky optical characterization of the SPTpol instrument

E. M. George; Peter A. R. Ade; K. A. Aird; J. E. Austermann; James A. Beall; D. Becker; A. N. Bender; B. A. Benson; L. E. Bleem; J. Britton; J. E. Carlstrom; C. L. Chang; H. C. Chiang; H. M. Cho; T. M. Crawford; A. T. Crites; A. Datesman; T. de Haan; M. Dobbs; W. Everett; A. Ewall-Wice; N. W. Halverson; N. L. Harrington; J. W. Henning; G. C. Hilton; W. L. Holzapfel; S. Hoover; N. Huang; J. Hubmayr; K. D. Irwin

In January 2012, the 10m South Pole Telescope (SPT) was equipped with a polarization-sensitive camera, SPTpol, in order to measure the polarization anisotropy of the cosmic microwave background (CMB). Measurements of the polarization of the CMB at small angular scales (~several arcminutes) can detect the gravitational lensing of the CMB by large scale structure and constrain the sum of the neutrino masses. At large angular scales (~few degrees) CMB measurements can constrain the energy scale of Inflation. SPTpol is a two-color mm-wave camera that consists of 180 polarimeters at 90 GHz and 588 polarimeters at 150 GHz, with each polarimeter consisting of a dual transition edge sensor (TES) bolometers. The full complement of 150 GHz detectors consists of 7 arrays of 84 ortho-mode transducers (OMTs) that are stripline coupled to two TES detectors per OMT, developed by the TRUCE collaboration and fabricated at NIST. Each 90 GHz pixel consists of two antenna-coupled absorbers coupled to two TES detectors, developed with Argonne National Labs. The 1536 total detectors are read out with digital frequency-domain multiplexing (DfMUX). The SPTpol deployment represents the first on-sky tests of both of these detector technologies, and is one of the first deployed instruments using DfMUX readout technology. We present the details of the design, commissioning, deployment, on-sky optical characterization and detector performance of the complete SPTpol focal plane.


THE THIRTEENTH INTERNATIONAL WORKSHOP ON LOW TEMPERATURE DETECTORS—LTD13 | 2009

Planar Orthomode Transducers for Feedhorn‐coupled TES Polarimeters

Jeff McMahon; J. W. Appel; J. E. Austermann; James A. Beall; D. Becker; B. A. Benson; L. E. Bleem; J. Britton; C. L. Chang; J. E. Carlstrom; H. M. Cho; A. T. Crites; Thomas Essinger-Hileman; W. Everett; N. W. Halverson; J. W. Henning; G. C. Hilton; K. D. Irwin; J. Mehl; S. S. Meyer; S. Mossley; Michael D. Niemack; Lucas Parker; S. M. Simon; Suzanne T. Staggs; C. Visnjic; Edward J. Wollack; K. U.‐Yen; K. W. Yoon; Y. Zhao

We present simulations and discuss measurements of a planar orthomode transducer (OMT) being developed for use with bolometric detectors in observations of the polarization of the cosmic microwave background (CMB). This OMT couples radiation from a circular waveguide onto microstrip where it is filtered and then detected. A corrugated feed horn defines the optical beam. Simulations suggest this OMT achieves a coupling efficiency of greater than 96% with cross‐polarization below 1% over 30% bandwidth.


Proceedings of SPIE | 2012

Feedhorn-coupled TES polarimeter camera modules at 150 GHz for CMB polarization measurements with SPTpol

J. W. Henning; Peter A. R. Ade; K. A. Aird; J. E. Austermann; James A. Beall; D. Becker; B. A. Benson; L. E. Bleem; J. Britton; J. E. Carlstrom; C. L. Chang; H. M. Cho; T. M. Crawford; A. T. Crites; A. Datesman; T. de Haan; M. Dobbs; W. Everett; A. Ewall-Wice; E. M. George; N. W. Halverson; N. L. Harrington; G. C. Hilton; W. L. Holzapfel; J. Hubmayr; K. D. Irwin; M. Karfunkle; R. Keisler; J. Kennedy; A. T. Lee

The SPTpol camera is a dichroic polarimetric receiver at 90 and 150 GHz. Deployed in January 2012 on the South Pole Telescope (SPT), SPTpol is looking for faint polarization signals in the Cosmic Microwave Background (CMB). The camera consists of 180 individual Transition Edge Sensor (TES) polarimeters at 90 GHz and seven 84-polarimeter camera modules (a total of 588 polarimeters) at 150 GHz. We present the design, dark characterization, and in-lab optical properties of the 150 GHz camera modules. The modules consist of photolithographed arrays of TES polarimeters coupled to silicon platelet arrays of corrugated feedhorns, both of which are fabricated at NIST-Boulder. In addition to mounting hardware and RF shielding, each module also contains a set of passive readout electronics for digital frequency-domain multiplexing. A single module, therefore, is fully functional as a miniature focal plane and can be tested independently. Across the modules tested before deployment, the detectors average a critical temperature of 478 mK, normal resistance RN of 1.2Ω , unloaded saturation power of 22.5 pW, (detector-only) optical efficiency of ~ 90%, and have electrothermal time constants < 1 ms in transition.


Proceedings of SPIE | 2012

Design and characterization of 90 GHz feedhorn-coupled TES polarimeter pixels in the SPTpol camera

J. T. Sayre; Peter A. R. Ade; K. A. Aird; J. E. Austermann; James A. Beall; D. Becker; B. A. Benson; L. E. Bleem; J. Britton; J. E. Carlstrom; C. L. Chang; H. M. Cho; T. M. Crawford; A. T. Crites; A. Datesman; T. de Haan; M. Dobbs; W. Everett; A. Ewall-Wice; E. M. George; N. W. Halverson; N. L. Harrington; J. W. Henning; G. C. Hilton; W. L. Holzapfel; J. Hubmayr; K. D. Irwin; M. Karfunkle; R. Keisler; J. Kennedy

The SPTpol camera is a two-color, polarization-sensitive bolometer receiver, and was installed on the 10 meter South Pole Telescope in January 2012. SPTpol is designed to study the faint polarization signals in the Cosmic Microwave Background, with two primary scientific goals. One is to constrain the tensor-to-scalar ratio of perturbations in the primordial plasma, and thus constrain the space of permissible in inflationary models. The other is to measure the weak lensing effect of large-scale structure on CMB polarization, which can be used to constrain the sum of neutrino masses as well as other growth-related parameters. The SPTpol focal plane consists of seven 84-element monolithic arrays of 150 GHz pixels (588 total) and 180 individual 90 GHz single- pixel modules. In this paper we present the design and characterization of the 90 GHz modules.


THE THIRTEENTH INTERNATIONAL WORKSHOP ON LOW TEMPERATURE DETECTORS—LTD13 | 2009

Optical properties of Feedhorn‐coupled TES polarimeters for CMB polarimetry

L. E. Bleem; J. W. Appel; J. E. Austermann; James A. Beall; D. Becker; B. A. Benson; J. Britton; J. E. Carlstrom; C. L. Chang; H. M. Cho; A. T. Crites; Thomas Essinger-Hileman; W. Everett; N. W. Halverson; J. W. Henning; G. C. Hilton; K. D. Irwin; Jeff McMahon; J. Mehl; S. S. Meyer; Michael D. Niemack; Lucas Parker; S. M. Simon; Suzanne T. Staggs; C. Visnjic; K. W. Yoon; Y. Zhao

We present data characterizing the optical properties of feedhorn‐coupled TES polarimeters useful for future CMB measurements. In this detector architecture, TES bolometers are coupled to radiation through superconducting microstrip to a planar ortho‐mode transducer inserted into waveguide. Filters in the microstrip define the pass bands for the detectors. We will present measurements of the co‐polar optical efficiency, the cross‐polar isolation and the detector bandpass and compare these results to expectations from simulations.


IEEE Transactions on Applied Superconductivity | 2013

Improvements in Silicon Oxide Dielectric Loss for Superconducting Microwave Detector Circuits

D. Li; Jiansong Gao; J. E. Austermann; James A. Beall; D. Becker; H. M. Cho; Anna E. Fox; N. W. Halverson; J. W. Henning; G. C. Hilton; J. Hubmayr; K. D. Irwin; J. Van Lanen; J. P. Nibarger; Michael D. Niemack

Dielectric loss in low-temperature superconducting integrated circuits can cause lower overall efficiency, particularly in the 90 to 220 GHz regime. We present a method to tune the dielectric loss for silicon oxide deposited by plasma-enhanced chemical-vapor deposition at ambient temperatures. Deposition in an environment with a higher silane-to-oxygen ratio produces silicon oxide films with a lower loss-tangent and a slightly higher optical index of refraction, while contributing no appreciable change in film stress. We measured the dielectric loss by fabricating a series of Nb-SiOx-Nb microstrip resonators in the frequency range of 6 to 9 GHz and comparing their temperature dependence to a model of parasitic two-level-system fluctuators. The dielectric loss-tangent of silicon oxide was improved from 6 ×10-3 for stoichiometric silicon dioxide to 2 ×10-3 for a more silicon-rich silicon oxide. We present details of the fabrication process and measurements of microstrip resonators.


IEEE Transactions on Applied Superconductivity | 2011

Stability of Al-Mn Transition Edge Sensors for Frequency Domain Multiplexing

J. Hubmayr; J. E. Austermann; James A. Beall; D. Becker; D. A. Bennett; B. A. Benson; L. E. Bleem; C. L. Chang; J. E. Carlstrom; H. M. Cho; A. T. Crites; M. Dobbs; W. Everett; E. M. George; W. L. Holzapfel; N. W. Halverson; J. W. Henning; G. C. Hilton; K. D. Irwin; D. Li; Peter J. Lowell; M. Lueker; J. J. McMahon; J. Mehl; S. S. Meyer; J. P. Nibarger; Michael D. Niemack; Daniel R. Schmidt; E. Shirokoff; S. M. Simon

We are developing arrays of 150 GHz transition edge sensor (TES) polarimeters for the South Pole Telescope polarimeter (SPTpol). Prototype devices use an aluminum manganese (Al-Mn) alloy TES with a normal resistance Rn suited to frequency domain multiplexing (fMUX) used in SPTpol. Using the fMUX readout, the devices exhibit noise performance consistent with expectations when R >; 0.8Rn. Below 0.8Rn, the detectors have high loopgain and become unstable, which is predicted by use of a compound TES model. We address this issue in a recent fabrication with increased TES heat capacity and normal metal structures on the TES to tune the temperature sensitivity.

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G. C. Hilton

National Institute of Standards and Technology

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J. E. Austermann

University of Colorado Boulder

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N. W. Halverson

University of Colorado Boulder

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A. T. Crites

California Institute of Technology

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D. Becker

National Institute of Standards and Technology

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James A. Beall

National Institute of Standards and Technology

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