R. S. Tucker
California Institute of Technology
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Proceedings of SPIE | 2010
J. P. Filippini; Peter A. R. Ade; M. Amiri; S. J. Benton; R. Bihary; J. J. Bock; J. R. Bond; J. A. Bonetti; Sean Bryan; B. Burger; H. C. Chiang; Carlo R. Contaldi; Brendan Crill; Olivier Doré; M. Farhang; L. M. Fissel; N. N. Gandilo; S. R. Golwala; J. E. Gudmundsson; M. Halpern; Matthew Hasselfield; G. C. Hilton; Warren Holmes; Viktor V. Hristov; K. D. Irwin; W. C. Jones; C. L. Kuo; C. J. MacTavish; P. Mason; T. E. Montroy
We describe SPIDER, a balloon-borne instrument to map the polarization of the millimeter-wave sky with degree angular resolution. Spider consists of six monochromatic refracting telescopes, each illuminating a focal plane of large-format antenna-coupled bolometer arrays. A total of 2,624 superconducting transition-edge sensors are distributed among three observing bands centered at 90, 150, and 280 GHz. A cold half-wave plate at the aperture of each telescope modulates the polarization of incoming light to control systematics. SPIDERs first flight will be a 20-30-day Antarctic balloon campaign in December 2011. This flight will map ~8% of the sky to achieve unprecedented sensitivity to the polarization signature of the gravitational wave background predicted by inflationary cosmology. The SPIDER mission will also serve as a proving ground for these detector technologies in preparation for a future satellite mission.
Proceedings of SPIE | 2010
M. C. Runyan; Peter A. R. Ade; M. Amiri; S. J. Benton; R. Bihary; J. J. Bock; J. R. Bond; J. A. Bonetti; Sean Bryan; H. C. Chiang; Carlo R. Contaldi; Brendan Crill; Olivier Doré; D. T. O'Dea; M. Farhang; J. P. Filippini; L. M. Fissel; N. N. Gandilo; S. R. Golwala; J. E. Gudmundsson; Matthew Hasselfield; M. Halpern; G. C. Hilton; Warren Holmes; Viktor V. Hristov; K. D. Irwin; W. C. Jones; C. L. Kuo; C. J. MacTavish; P. Mason
Here we describe the design and performance of the SPIDER instrument. SPIDER is a balloon-borne cosmic microwave background polarization imager that will map part of the sky at 90, 145, and 280 GHz with subdegree resolution and high sensitivity. This paper discusses the general design principles of the instrument inserts, mechanical structures, optics, focal plane architecture, thermal architecture, and magnetic shielding of the TES sensors and SQUID multiplexer. We also describe the optical, noise, and magnetic shielding performance of the 145 GHz prototype instrument insert.
Proceedings of SPIE | 2010
Sean Bryan; Peter A. R. Ade; M. Amiri; S. Benton; R. Bihary; J. J. Bock; J. Richard Bond; Joseph A. Bonetti; H. Cynthia Chiang; Carlo R. Contaldi; Brendan Crill; Daniel O'Dea; Olivier Doré; M. Farhang; J. Filippini; L. M. Fissel; N. N. Gandilo; S. R. Golwala; J. E. Gudmundsson; Matthew Hasselfield; M. Halpern; Kyle Helson; G. C. Hilton; Warren Holmes; Viktor V. Hristov; K. D. Irwin; W. C. Jones; C. L. Kuo; C. J. MacTavish; Peter Mason
Spider is a balloon-borne array of six telescopes that will observe the Cosmic Microwave Background. The 2624 antenna-coupled bolometers in the instrument will make a polarization map of the CMB with approximately one-half degree resolution at 145 GHz. Polarization modulation is achieved via a cryogenic sapphire half-wave plate (HWP) skyward of the primary optic. We have measured millimeter-wave transmission spectra of the sapphire at room and cryogenic temperatures. The spectra are consistent with our physical optics model, and the data gives excellent measurements of the indices of A-cut sapphire. We have also taken preliminary spectra of the integrated HWP, optical system, and detectors in the prototype Spider receiver. We calculate the variation in response of the HWP between observing the CMB and foreground spectra, and estimate that it should not limit the Spider constraints on inflation.
The Astrophysical Journal | 2015
Peter A. R. Ade; R. W. Aikin; M. Amiri; Denis Barkats; S. J. Benton; C. A. Bischoff; J. J. Bock; J. A. Bonetti; J. A. Brevik; I. Buder; E. Bullock; Goutam Chattopadhyay; G. R. Davis; P. K. Day; C. D. Dowell; L. Duband; J. Filippini; S. Fliescher; S. R. Golwala; M. Halpern; M. Hasselfield; S. R. Hildebrandt; G. C. Hilton; V. V. Hristov; H. Hui; K. D. Irwin; W. C. Jones; K. S. Karkare; J. P. Kaufman; Brian Keating
We have developed antenna-coupled transition-edge sensor bolometers for a wide range of cosmic microwave background (CMB) polarimetry experiments, including Bicep2, Keck Array, and the balloon borne Spider. These detectors have reached maturity and this paper reports on their design principles, overall performance, and key challenges associated with design and production. Our detector arrays repeatedly produce spectral bands with 20%–30% bandwidth at 95, 150, or 230 GHz. The integrated antenna arrays synthesize symmetric co-aligned beams with controlled side-lobe levels. Cross-polarized response on boresight is typically
Proceedings of SPIE | 2014
A. S. Rahlin; Peter A. R. Ade; M. Amiri; S. J. Benton; J. J. Bock; J. R. Bond; Sean Bryan; Hsin C. Chiang; Carlo R. Contaldi; B. P. Crill; O. Doré; M. Farhang; J. Filippini; L. M. Fissel; A. A. Fraisse; A. E. Gambrel; N. N. Gandilo; S. R. Golwala; J. E. Gudmundsson; M. Halpern; Matthew Hasselfield; G. C. Hilton; Warren Holmes; V. V. Hristov; K. D. Irwin; W. C. Jones; Z. Kermish; C. L. Kuo; C. J. MacTavish; P. Mason
\sim 0.5\%
The Astrophysical Journal | 2011
D. T. O'Dea; Peter A. R. Ade; M. Amiri; S. J. Benton; J. J. Bock; J. R. Bond; J. A. Bonetti; Sean Bryan; B. Burger; H. C. Chiang; C. N. Clark; Carlo R. Contaldi; Brendan Crill; G. Davis; Olivier Doré; M. Farhang; J. Filippini; L. M. Fissel; A. A. Fraisse; N. N. Gandilo; S. R. Golwala; J. E. Gudmundsson; Matthew Hasselfield; G. C. Hilton; Warren Holmes; Viktor V. Hristov; K. D. Irwin; W. C. Jones; C. L. Kuo; C. J. MacTavish
, consistent with cross-talk in our multiplexed readout system. End-to-end optical efficiencies in our cameras are routinely 35% or higher, with per detector sensitivities of NET ~ 300
Proceedings of SPIE | 2012
R. O'Brient; Peter A. R. Ade; Z. Ahmed; R. W. Aikin; M. Amiri; S. J. Benton; C. A. Bischoff; J. J. Bock; J. A. Bonetti; J. A. Brevik; B. Burger; G. R. Davis; Peter K. Day; C. D. Dowell; L. Duband; J. Filippini; S. Fliescher; S. R. Golwala; J. A. Grayson; M. Halpern; Matthew Hasselfield; G. C. Hilton; V. V. Hristov; H. Hui; K. D. Irwin; S. A. Kernasovskiy; J. M. Kovac; Chao-Lin Kuo; E. M. Leitch; M. Lueker
\mu {{\rm{K}}}_{\mathrm{CMB}}\sqrt{{\rm{s}}}
Review of Scientific Instruments | 2016
Sean Bryan; Peter A. R. Ade; M. Amiri; Steven J. Benton; R. Bihary; J. J. Bock; J. Richard Bond; H. Cynthia Chiang; Carlo R. Contaldi; Brendan Crill; Olivier Doré; Benjamin Elder; J. Filippini; A. A. Fraisse; A. E. Gambrel; N. N. Gandilo; J. E. Gudmundsson; Matthew Hasselfield; M. Halpern; G. C. Hilton; Warren Holmes; Viktor V. Hristov; K. D. Irwin; W. C. Jones; Z. Kermish; C. Lawrie; C. J. MacTavish; Peter Mason; K. G. Megerian; Lorenzo Moncelsi
. Thanks to the scalability of this design, we have deployed 2560 detectors as 1280 matched pairs in Keck Array with a combined instantaneous sensitivity of
The Astrophysical Journal | 2017
J. M. Nagy; Peter A. R. Ade; M. Amiri; Steven J. Benton; A. S. Bergman; R. Bihary; J. J. Bock; J. R. Bond; Sean Bryan; H. C. Chiang; Carlo R. Contaldi; O. Doré; Adri J. Duivenvoorden; H. K. Eriksen; M. Farhang; J. Filippini; L. M. Fissel; A. A. Fraisse; Katherine Freese; Mathew Galloway; A. E. Gambrel; N. N. Gandilo; K. Ganga; J. E. Gudmundsson; M. Halpern; John Hartley; Matthew Hasselfield; G. C. Hilton; W. A. Holmes; V. V. Hristov
\sim 9\;\mu {{\rm{K}}}_{\mathrm{CMB}}\sqrt{{\rm{s}}}
Proceedings of SPIE | 2014
N. N. Gandilo; Peter A. R. Ade; M. Amiri; F. E. Angilè; S. J. Benton; J. J. Bock; J. R. Bond; Sean Bryan; H. C. Chiang; Carlo R. Contaldi; B. P. Crill; Mark J. Devlin; B. Dober; O. Doré; M. Farhang; J. P. Filippini; L. M. Fissel; A. A. Fraisse; Yasuo Fukui; Nicholas Galitzki; A. E. Gambrel; S. R. Golwala; J. E. Gudmundsson; M. Halpern; Matthew Hasselfield; G. C. Hilton; Warren Holmes; V. V. Hristov; K. D. Irwin; W. C. Jones
, as measured directly from CMB maps in the 2013 season. Similar arrays have recently flown in the Spider instrument, and development of this technology is ongoing.