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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

SPTpol: An instrument for CMB polarization

Jeff McMahon; K. A. Aird; B. A. Benson; L. E. Bleem; J. Britton; J. E. Carlstrom; C. L. Chang; Hsiao-Mei Cho; T. Dehaan; T. M. Crawford; A. T. Crites; A. Datesman; M. Dobbs; W. Everett; N. W. Halverson; G. P. Holder; W. L. Holzapfel; D. Hmbes; K. D. Irwin; M. Joy; R. Keisler; T. M. Lanting; Adrian T. Lee; E. M. Leitch; A. Loehr; M. Lueker; J. Mehl; S. S. Meyer; J. J. Mohr; T. E. Montroy

SPTpol will consist of an 850 element polarization sensitive bolometric camera deployed to the South Pole Telescope in late 2011. This camera is optimized for measurement of the polarization of the cosmic microwave background with arcminute resolution. These measurements will be used to constrain neutrino masses and to constrain the amplitude of gravitational waves from inflation. The camera includes two detector architectures that observe in two different frequency bands. At 150 GHz, SPTpol will use 650 feedhorn-coupled TES polarimeters fabricated at NIST. At 90 GHz, it will use 200 absorber-coupled polarimeters developed at Argonne National Lab. The NIST pixels will be coupled to the telescope using a monolithic array of corrugated feeds and the Argonne devices will be coupled with individually machined contoured feeds. The entire focal plane will be readout using a digital frequency-domain multiplexer system. We provide an overview of the project, describe the detectors and discuss the design of this system.


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.


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.


IEEE Transactions on Applied Superconductivity | 2011

Thermal Properties of Silicon Nitride Beams Below One Kelvin

G. Wang; V. Yefremenko; Valentyn Novosad; A. Datesman; J. Pearson; Ralu Divan; C. L. Chang; L. E. Bleem; A. T. Crites; J. Mehl; T. Natoli; J. J. McMahon; J. Sayre; J. E. Ruhl; S. S. Meyer; J. E. Carlstrom

We have investigated thermal properties of 1 μm thick silicon nitride beams of different lateral dimensions. We measured the thermal conductance by simultaneously employing a TES both as a heater and as a sensor. Based upon these measurements, we calculate the thermal conductivity of the beams. We utilize a boundary limited phonon transport model and assume a temperature independent phonon mean free path. We find that the thermal conductivity is determined by the fraction of diffusive reflection at surface. The following results are obtained from 0.30 K to 0.55 K: the volume heat capacity is 0.082T+0.502T3 J/m3-K . The width dependent phonon mean free path is 6.58 μm, 9.80 μm and 11.55 μm for 10 μm, 20 μm and 30 μm beams respectively at a 29% surface diffusive reflection.


IEEE Transactions on Applied Superconductivity | 2011

Progress on ANL/KICP Bolometers for SPTpol

A. T. Crites; B. A. Benson; L. E. Bleem; J. E. Carlstrom; C. L. Chang; A. Datesman; Ralu Divan; E. M. George; W. L. Holzapfel; A. T. Lee; M. Lueker; J. J. McMahon; J. Mehl; S. S. Meyer; T. E. Montroy; T. Natoli; Valentyn Novosad; J. Pearson; J. E. Ruhl; J. Sayre; E. Shirokoff; K. Story; G. Wang; V. Yefremenko; E. Young

We present progress on Argonne/KICP TES bolometers fabricated at Argonne National Labs. These detectors will be used to measure the polarization of the Cosmic Microwave Background radiation with SPTpol. The sensors are bolometers consisting of a Mo/Au transition edge sensors (TES) suspended on silicon nitride with a gold bar absorber to couple radiation to the device. We present optical measurements and thermal characterizations of prototype devices.


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

Design and Fabrication of Argonne/KICP Detectors for CMB Polarization

V. Yefremenko; A. Datesman; G. Wang; J. Pearson; V. Novosad; Ralu Divan; L. E. Bleem; C. L. Chang; A. T. Crites; W. Everett; Jeff McMahon; J. Mehl; S. S. Meyer; J. E. Ruhl; J. Sayre; J. E. Carlstrom

We present the design, microfabrication and assembly of dual‐polarization absorber‐coupled Transition Edge Sensor (TES) bolometer detectors for cosmic microwave background B‐mode polarization studies. The device consists of two separate dies incorporating suspended silicon nitride membranes within silicon frames, carefully aligned perpendicularly and fixtured face‐to‐face. Polarization sensitivity around 95 GHz is provided by a single dipole‐like absorber element; we briefly analyze this absorber‐in‐waveguide configuration in closed form using the EMF method. Proximity effect Mo/Au bilayers provide control of the TES critical temperature between 400 mK and 600 mK, with a normal resistance Rn∼1Ω. DC magnetron sputtering, wet etching, and liftoff were employed for TES fabrication. Optimization of the superconducting Mo thin film utilized independent RF bias applied to the substrate during deposition in a confocal geometry. This technique allows outstanding thin film uniformity and stress to be achieved simu...


Proceedings of SPIE | 2012

South Pole Telescope software systems: control, monitoring, and data acquisition

K. Story; E. M. Leitch; 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; E. M. George; N. W. Halverson; N. L. Harrington; J. W. Henning; G. C. Hilton; W. L. Holzapfel; S. Hoover; N. Huang

We present the software system used to control and operate the South Pole Telescope. The South Pole Telescope is a 10-meter millimeter-wavelength telescope designed to measure anisotropies in the cosmic microwave background (CMB) at arcminute angular resolution. In the austral summer of 2011/12, the SPT was equipped with a new polarization-sensitive camera, which consists of 1536 transition-edge sensor bolometers. The bolometers are read out using 36 independent digital frequency multiplexing (DfMux) readout boards, each with its own embedded processors. These autonomous boards control and read out data from the focal plane with on-board software and firmware. An overall control software system running on a separate control computer controls the DfMux boards, the cryostat and all other aspects of telescope operation. This control software collects and monitors data in real-time, and stores the data to disk for transfer to the United States for analysis.


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

Optical design of Argonne/KICP detectors for CMB polarization.

Jeff McMahon; L. E. Bleem; A. T. Crites; J. E. Carlstrom; C. L. Chang; A. Datesman; Ralu Divan; W. Everett; J. Mehl; S. S. Meyer; V. Novosad; J. Pearson; J. E. Ruhl; J. Sayre; G. Wang; V. Yefremenko

We present simulations and measurements of a new optical coupling scheme for bolometric detectors for cosmic microwave background (CMB) polarization under development by Argonne National Labs and the University of Chicago. We show simulations of the performance and a tolerance analysis of this device along with measurements that validate its performance. Optical measurements of a prototype point to a 90% coupling efficiency with a cross‐polarization below ‐20 dB.

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A. T. Crites

California Institute of Technology

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V. Yefremenko

Argonne National Laboratory

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J. Pearson

Argonne National Laboratory

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Ralu Divan

Argonne National Laboratory

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