Peter Ashton
Northwestern University
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The Astrophysical Journal | 2016
L. M. Fissel; Peter A. R. Ade; Francesco E. Angilè; Peter Ashton; Steven J. Benton; Mark J. Devlin; B. Dober; Yasuo Fukui; Nicholas Galitzki; N. N. Gandilo; J. Klein; Andrei Korotkov; Zhi-Yun Li; Peter G. Martin; Tristan G. Matthews; Lorenzo Moncelsi; Fumitaka Nakamura; C. B. Netterfield; Giles Novak; Enzo Pascale; Frédérick Poidevin; Fabio P. Santos; G. Savini; Douglas Scott; J. A. Shariff; J. D. Soler; Nicholas Thomas; Carole Tucker; Gregory S. Tucker; Derek Ward-Thompson
We present results for Vela C obtained during the 2012 flight of the Balloon-borne Large Aperture Submillimeter Telescope for Polarimetry. We mapped polarized intensity across almost the entire extent of this giant molecular cloud, in bands centered at 250, 350, and 500 μm. In this initial paper, we show our 500 μmdata smoothed to a resolution of 2 5 (approximately 0.5 pc). We show that the mean level of the fractional polarization pand most of its spatial variations can be accounted for using an empirical three-parameter power-law fit, p μ N-0.45 S-0.60, where Nis the hydrogen column density and Sis the polarization-angle dispersion on 0.5 pc scales. The decrease of pwith increasing Sis expected because changes in the magnetic field direction within the cloud volume sampled by each measurement will lead to cancellation of polarization signals. The decrease of pwith increasing Nmight be caused by the same effect, if magnetic field disorder increases for high column density sightlines. Alternatively, the intrinsic polarization efficiency of the dust grain population might be lower for material along higher density sightlines. We find no significant correlation between Nand S. Comparison of observed submillimeter polarization maps with synthetic polarization maps derived from numerical simulations provides a promising method for testing star formation theories. Realistic simulations should allow for the possibility of variable intrinsic polarization efficiency. The measured levels of correlation among p, N, and Sprovide points of comparison between observations and simulations
arXiv: Instrumentation and Methods for Astrophysics | 2014
Nicholas Galitzki; Peter A. R. Ade; Francesco E. Angilè; Peter Ashton; James A. Beall; D. Becker; Kristi J. Bradford; George Che; Hsiao-Mei Cho; Mark J. Devlin; B. Dober; L. M. Fissel; Yasuo Fukui; Jiansong Gao; Christopher E. Groppi; Seth Hillbrand; G. C. Hilton; J. Hubmayr; K. D. Irwin; J. Klein; Jeff Van Lanen; D. Li; Zhi-Yun Li; Nathan P. Lourie; Hamdi Mani; Peter G. Martin; Philip Daniel Mauskopf; Fumitaka Nakamura; Giles Novak; David P. Pappas
The Balloon-borne Large Aperture Submillimeter Telescope for Polarimetry (BLASTPol) was a suborbital experiment designed to map magnetic fields in order to study their role in star formation processes. BLASTPol made detailed polarization maps of a number of molecular clouds during its successful flights from Antarctica in 2010 and 2012. We present the next-generation BLASTPol instrument (BLAST-TNG) that will build off the success of the previous experiment and continue its role as a unique instrument and a test bed for new technologies. With a 16-fold increase in mapping speed, BLAST-TNG will make larger and deeper maps. Major improvements include a 2.5-m carbon fiber mirror that is 40% wider than the BLASTPol mirror and ~3000 polarization sensitive detectors. BLAST-TNG will observe in three bands at 250, 350, and 500 μm. The telescope will serve as a pathfinder project for microwave kinetic inductance detector (MKID) technology, as applied to feedhorn-coupled submillimeter detector arrays. The liquid helium cooled cryostat will have a 28-day hold time and will utilize a closed-cycle 3He refrigerator to cool the detector arrays to 270 mK. This will enable a detailed mapping of more targets with higher polarization resolution than any other submillimeter experiment to date. BLAST-TNG will also be the first balloon-borne telescope to offer shared risk observing time to the community. This paper outlines the motivation for the project and the instrumental design.
Astronomy and Astrophysics | 2017
J. D. Soler; Peter A. R. Ade; F. E. Angilè; Peter Ashton; Steven J. Benton; Mark J. Devlin; B. Dober; L. M. Fissel; Yasuo Fukui; Nicholas Galitzki; N. N. Gandilo; Patrick Hennebelle; J. Klein; Zhi-Yun Li; Andrei Korotkov; P. G. Martin; Tristan G. Matthews; Lorenzo Moncelsi; C. B. Netterfield; Giles Novak; Enzo Pascale; Frédérick Poidevin; Fabio P. Santos; G. Savini; D. Scott; J. A. Shariff; Nicholas Thomas; Carole Tucker; G. S. Tucker; Derek Ward-Thompson
We statistically evaluated the relative orientation between gas column density structures, inferred from Herschel submillimetre observations, and the magnetic field projected on the plane of sky, inferred from polarized thermal emission of Galactic dust observed by the Balloon-borne Large-Aperture Submillimetre Telescope for Polarimetry (BLASTPol) at 250, 350, and 500 μm, towards the Vela C molecular complex. First, we find very good agreement between the polarization orientations in the three wavelength-bands, suggesting that, at the considered common angular resolution of 3.0 that corresponds to a physical scale of approximately 0.61 pc, the inferred magnetic field orientation is not significantly affected by temperature or dust grain alignment effects. Second, we find that the relative orientation between gas column density structures and the magnetic field changes progressively with increasing gas column density, from mostly parallel or having no preferred orientation at low column densities to mostly perpendicular at the highest column densities. This observation is in agreement with previous studies by the Planck collaboration towards more nearby molecular clouds. Finally, we find a correspondencebetween (a) the trends in relative orientation between the column density structures and the projected magnetic field; and (b) the shape of the column density probability distribution functions (PDFs). In the sub-regions of Vela C dominated by one clear filamentary structure, or “ridges”, where the high-column density tails of the PDFs are flatter, we find a sharp transition from preferentially parallel or having no preferred relative orientation at low column densities to preferentially perpendicular at highest column densities. In the sub-regions of Vela C dominated by several filamentary structures with multiple orientations, or “nests”, where the maximum values of the column density are smaller than in the ridge-like sub-regions and the high-column density tails of the PDFs are steeper, such a transition is also present, but it is clearly less sharp than in the ridge-like sub-regions. Both of these results suggest that the magnetic field is dynamically important for the formation of density structures in this region.
The Astrophysical Journal | 2016
N. N. Gandilo; Peter A. R. Ade; Francesco E. Angilè; Peter Ashton; Steven J. Benton; Mark J. Devlin; B. Dober; L. M. Fissel; Yasuo Fukui; Nicholas Galitzki; J. Klein; Andrei Korotkov; Zhi-Yun Li; Peter G. Martin; Tristan G. Matthews; Lorenzo Moncelsi; Fumitaka Nakamura; C. B. Netterfield; Giles Novak; Enzo Pascale; Frédérick Poidevin; Fabio P. Santos; G. Savini; Douglas Scott; J. A. Shariff; J. D. Soler; Nicholas Thomas; Carole Tucker; Gregory S. Tucker; Derek Ward-Thompson
Polarization maps of the Vela C molecular cloud were obtained at 250, 350, and 500um during the 2012 flight of the balloon-borne telescope BLASTPol. These measurements are used in conjunction with 850um data from Planck to study the submillimeter spectrum of the polarization fraction for this cloud. The spectrum is relatively flat and does not exhibit a pronounced minimum at \lambda ~350um as suggested by previous measurements of other molecular clouds. The shape of the spectrum does not depend strongly on the radiative environment of the dust, as quantified by the column density or the dust temperature obtained from Herschel data. The polarization ratios observed in Vela C are consistent with a model of a porous clumpy molecular cloud being uniformly heated by the interstellar radiation field.
arXiv: Instrumentation and Methods for Astrophysics | 2018
Charles A. Hill; Sarah Marie M. Bruno; Sara M. Simon; Aamir Ali; K. Arnold; Peter Ashton; D. Barron; Sean Bryan; Y. Chinone; Gabriele Coppi; Kevin T. Crowley; A. Cukierman; Simon R. Dicker; Jo Dunkley; Giulio Fabbian; Nicholas Galitzki; Patricio A. Gallardo; J. E. Gudmundsson; J. Hubmayr; Brian Keating; Akito Kusaka; Adrian T. Lee; F. Matsuda; Philip Daniel Mauskopf; J. J. McMahon; Michael D. Niemack; Giuseppe Puglisi; Mayuri Sathyanarayana Rao; Maria Salatino; Carlos Sierra
The Simons Observatory (SO) is an upcoming experiment that will study temperature and polarization fluctuations in the cosmic microwave background (CMB) from the Atacama Desert in Chile. SO will field both a large aperture telescope (LAT) and an array of small aperture telescopes (SATs) that will observe in six bands with center frequencies spanning from 27 to 270 GHz. Key considerations during the SO design phase are vast, including the number of cameras per telescope, focal plane magnification and pixel density, in-band optical power and camera throughput, detector parameter tolerances, and scan strategy optimization. To inform the SO design in a rapid, organized, and traceable manner, we have created a Python-based sensitivity calculator with several state-of-the-art features, including detector-to-detector optical white-noise correlations, a handling of simulated and measured bandpasses, and propagation of low-level parameter uncertainties to uncertainty in on-sky noise performance. We discuss the mathematics of the sensitivity calculation, the calculators object-oriented structure and key features, how it has informed the design of SO, and how it can enhance instrument design in the broader CMB community, particularly for CMB-S4.
Proceedings of SPIE | 2016
Nicholas Galitzki; Peter A. R. Ade; Francesco E. Angilè; Peter Ashton; J. E. Austermann; Tashalee Billings; George Che; H. M. Cho; Kristina Davis; Mark J. Devlin; Simon R. Dicker; B. Dober; L. M. Fissel; Yasuo Fukui; Jiansong Gao; Samuel Gordon; Christopher Groppi; Seth Hillbrand; G. C. Hilton; J. Hubmayr; K. D. Irwin; J. Klein; D. Li; Zhi Yun Li; Nathan P. Lourie; Ian Lowe; Hamdi Mani; Peter G. Martin; Philip Daniel Mauskopf; C. M. McKenney
Polarized thermal emission from interstellar dust grains can be used to map magnetic fields in star forming molecular clouds and the diffuse interstellar medium (ISM). The Balloon-borne Large Aperture Submillimeter Telescope for Polarimetry (BLASTPol) flew from Antarctica in 2010 and 2012 and produced degree-scale polarization maps of several nearby molecular clouds with arcminute resolution. The success of BLASTPol has motivated a next-generation instrument, BLAST-TNG, which will use more than 3000 linear polarization- sensitive microwave kinetic inductance detectors (MKIDs) combined with a 2.5 m diameter carbon fiber primary mirror to make diffraction-limited observations at 250, 350, and 500 µm. With 16 times the mapping speed of BLASTPol, sub-arcminute resolution, and a longer flight time, BLAST-TNG will be able to examine nearby molecular clouds and the diffuse galactic dust polarization spectrum in unprecedented detail. The 250 μm detec- tor array has been integrated into the new cryogenic receiver, and is undergoing testing to establish the optical and polarization characteristics of the instrument. BLAST-TNG will demonstrate the effectiveness of kilo-pixel MKID arrays for applications in submillimeter astronomy. BLAST-TNG is scheduled to fly from Antarctica in December 2017 for 28 days and will be the first balloon-borne telescope to offer a quarter of the flight for “shared risk” observing by the community.
arXiv: Instrumentation and Methods for Astrophysics | 2018
John L. Orlowski-Scherer; Ningfeng Zhu; Xhilei Zhu; K. Arnold; Sara M. Simon; Nicholas Galitzki; Simon Dikcer; M. Limon; Mark J. Devlin; Michael D. Niemack; Giuseppe Puglisi; Gabriele Coppi; Eve M. Vavagiakis; Max Silva-Feaver; Brian Keating; Aamir Ali; L. Piccirillo; Adrian T. Lee; Patricio A. Gallardo; Maria Salatino; Peter Ashton; Jeff McMahon; Marius Lungu; Andrew J. May; Robert Thornton
The Simons Observatory (SO) will make precision temperature and polarization measurements of the cosmic microwave background (CMB) using a series of telescopes which will cover angular scales between one arcminute and tens of degrees, contain over 60,000 detectors, and sample frequencies between 27 and 270 GHz. SO will consist of a six-meter-aperture telescope coupled to over 30,000 detectors along with an array of half-meter aperture refractive cameras, which together couple to an additional 30,000+ detectors. SO will measure fundamental cosmological parameters of our universe, find high redshift clusters via the Sunyaev-Zeldovich effect, constrain properties of neutrinos, and seek signatures of dark matter through gravitational lensing. In this paper we will present results of the simulations of the SO large aperture telescope receiver (LATR). We will show details of simulations performed to ensure the structural integrity and thermal performance of our receiver, as well as will present the results of finite element analyses (FEA) of designs for the structural support system. Additionally, a full thermal model for the LATR will be described. The model will be used to ensure we meet our design requirements. Finally, we will present the results of FEA used to identify the primary vibrational modes, and planned methods for suppressing these modes. Design solutions to each of these problems that have been informed by simulation will be presented.
arXiv: Instrumentation and Methods for Astrophysics | 2018
Ningfeng Zhu; John L. Orlowski-Scherer; Zhilei Xu; Aamir Ali; K. Arnold; Peter Ashton; Gabriele Coppi; Mark J. Devlin; Simon R. Dicker; Nicholas Galitzki; Patricio A. Gallardo; Shuay-Pwu P. Ho; J. Hubmayr; Brian Keating; Adrian T. Lee; M. Limon; Philip Daniel Mauskopf; Andrew J. May; Jeff McMahon; Michael D. Niemack; L. Piccirillo; Giuseppe Puglisi; Maria Salatino; Mayuri S. Rao; Max Silva-Feaver; Sara M. Simon; Suzanne T. Staggs; Joel N. Ullom; Eve M. Vavagiakis; B. Westbrook
The Simons Observatory (SO) will make precision temperature and polarization measurements of the cosmic microwave background (CMB) using a series of telescopes which will cover angular scales between one arcminute and tens of degrees and sample frequencies between 27 and 270 GHz. Here we present the current design of the large aperture telescope receiver (LATR), a 2.4m diameter cryostat that will be mounted on the SO 6m telescope and will be the largest CMB receiver to date. The cryostat size was chosen to take advantage of the large focal plane area having high Strehl ratios, which is inherent to the Cross-Dragone telescope design. The LATR will be able to accommodate thirteen optics tubes, each having a 36 cm diameter aperture and illuminating several thousand transition-edge sensor (TES) bolometers. This set of equipment will provide an opportunity to make measurements with unparalleled sensitivity. However, the size and complexity of the LATR also pose numerous technical challenges. In the following paper, we present the design of the LATR and include how we address these challenges. The solutions we develop in the process of designing the LATR will be informative for the general CMB community, and for future CMB experiments like CMB-S4.
arXiv: Instrumentation and Methods for Astrophysics | 2018
Simon R. Dicker; Charles A. Hill; J. Hubmayr; Brian Keating; Adrian T. Lee; M. Limon; F. Matsuda; Jeff McMahon; Edward J. Wollack; Zhilei Xu; Ningfeng Zhu; Patricio A. Gallardo; Jon E. Gudmudsson; Phillip Mauskopf; Aamir Ali; Peter Ashton; Gabriele Coppi; Mark J. Devlin; Nicholas Galitzki; Shuay-Pwu P. Ho; Michael D. Niemack; John L. Orlowski-Scherer; L. Piccirillo; Maria Salatino; Sara M. Simon; Suzanne T. Staggs; Robert Thornton; Joel N. Ullom; Eve M. Vavagiakis
The Simons Observatory will consist of a single large (6 m diameter) telescope and a number of smaller (∼0.5 m diameter) refracting telescopes designed to measure the polarization of the Cosmic Microwave Background to unprecedented accuracy. The large aperture telescope is the same design as the CCAT-prime telescope, a modified Crossed Dragone design with a field-of-view of over 7.8 degrees diameter at 90 GHz. This paper presents an overview of the cold reimaging optics for this telescope and what drove our choice of 350–400 mm diameter silicon lenses in a 2.4 m cryostat over other possibilities. We will also consider the future expandability of this design to CMB Stage-4 and beyond.
arXiv: Instrumentation and Methods for Astrophysics | 2018
Nathan P. Lourie; Nicholas Galitzki; F. E. Angilè; Peter Ashton; Mark J. Devlin; Simon R. Dicker; B. Dober; L. M. Fissel; Samuel Gordon; J. Klein; Ian Lowe; Philip Daniel Mauskopf; F. Nati; Giles Novak; J. D. Soler; Paul Williams; Brian E. Catanzaro; Joy Didier; Javier Romualdez
The Next Generation Balloon-borne Large Aperture Submillimeter Telescope (BLAST-TNG) is a submillimeter mapping experiment planned for a 28 day long-duration balloon (LDB) flight from McMurdo Station, Antarctica during the 2018-2019 season. BLAST-TNG will detect submillimeter polarized interstellar dust emission, tracing magnetic fields in galactic molecular clouds. BLAST-TNG will be the first polarimeter with the sensitivity and resolution to probe the ∼0.1 parsec-scale features that are critical to understanding the origin of structures in the interstellar medium. With three detector arrays operating at 250, 350, and 500 μm (1200, 857, and 600 GHz), BLAST-TNG will obtain diffraction-limited resolution at each waveband of 30, 41, and 59 arcseconds respectively. To achieve the submillimeter resolution necessary for its science goals, the BLAST-TNG telescope features a 2.5 m aperture carbon fiber composite primary mirror, one of the largest mirrors flown on a balloon platform. Successful performance of such a large telescope on a balloon-borne platform requires stiff, lightweight optical components and mounting structures. Through a combination of optical metrology and finite element modeling of thermal and mechanical stresses on both the telescope optics and mounting structures, we expect diffractionlimited resolution at all our wavebands. We expect pointing errors due to deformation of the telescope mount to be negligible. We have developed a detailed thermal model of the sun shielding, gondola, and optical components to optimize our observing strategy and increase the stability of the telescope over the flight. We present preflight characterization of the telescope and its platform.