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Dive into the research topics where Daniel S. Swetz is active.

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Featured researches published by Daniel S. Swetz.


Physical Review Letters | 2011

Detection of the power spectrum of cosmic microwave background lensing by the Atacama Cosmology Telescope.

Sudeep Das; Blake D. Sherwin; Paula Aguirre; J. W. Appel; J. Richard Bond; C. Sofia Carvalho; Mark J. Devlin; Joanna Dunkley; Rolando Dünner; Thomas Essinger-Hileman; Joseph W. Fowler; Amir Hajian; M. Halpern; Matthew Hasselfield; Adam D. Hincks; Renée Hlozek; K. M. Huffenberger; John P. Hughes; K. D. Irwin; Jeff Klein; Arthur Kosowsky; Robert H. Lupton; Tobias A. Marriage; Danica Marsden; F. Menanteau; Kavilan Moodley; Michael D. Niemack; Michael R. Nolta; Lyman A. Page; Lucas Parker

We report the first detection of the gravitational lensing of the cosmic microwave background through a measurement of the four-point correlation function in the temperature maps made by the Atacama Cosmology Telescope. We verify our detection by calculating the levels of potential contaminants and performing a number of null tests. The resulting convergence power spectrum at 2° angular scales measures the amplitude of matter density fluctuations on comoving length scales of around 100 Mpc at redshifts around 0.5 to 3. The measured amplitude of the signal agrees with Lambda cold dark matter cosmology predictions. Since the amplitude of the convergence power spectrum scales as the square of the amplitude of the density fluctuations, the 4σ detection of the lensing signal measures the amplitude of density fluctuations to 12%.


The Astrophysical Journal | 2011

The Atacama Cosmology Telescope: a measurement of the cosmic microwave background power spectrum at 148 and 218 GHz from the 2008 southern survey

Sudeep Das; Tobias A. Marriage; Peter A. R. Ade; Paula Aguirre; M. Amiri; J. W. Appel; L. Felipe Barrientos; E. S. Battistelli; John R. Bond; Ben Brown; B. Burger; J. A. Chervenak; Mark J. Devlin; Simon R. Dicker; W. Bertrand Doriese; Joanna Dunkley; Rolando Dünner; Thomas Essinger-Hileman; R. P. Fisher; Joseph W. Fowler; Amir Hajian; M. Halpern; Matthew Hasselfield; C. Hernández-Monteagudo; G. C. Hilton; Matt Hilton; Adam D. Hincks; Renée Hlozek; K. M. Huffenberger; David H. Hughes

We present measurements of the cosmic microwave background (CMB) power spectrum made by the Atacama Cosmology Telescope at 148 GHz and 218 GHz, as well as the cross-frequency spectrum between the two channels. Our results clearly show the second through the seventh acoustic peaks in the CMB power spectrum. The measurements of these higher-order peaks provide an additional test of the ΛCDM cosmological model. At l>3000, we detect power in excess of the primary anisotropy spectrum of the CMB. At lower multipoles 500 < l < 3000, we find evidence for gravitational lensing of the CMB in the power spectrum at the 2.8σ level. We also detect a low level of Galactic dust in our maps, which demonstrates that we can recover known faint, diffuse signals.


Astrophysical Journal Supplement Series | 2011

Overview of the Atacama Cosmology Telescope: receiver, instrumentation, and telescope systems

Daniel S. Swetz; Peter A. R. Ade; M. Amiri; J. W. Appel; E. S. Battistelli; B. Burger; J. A. Chervenak; Mark J. Devlin; Simon R. Dicker; W. B. Doriese; Rolando Dünner; Thomas Essinger-Hileman; R. P. Fisher; J. W. Fowler; M. Halpern; Matthew Hasselfield; G. C. Hilton; Adam D. Hincks; K. D. Irwin; N. Jarosik; M. Kaul; J. Klein; Judy M. Lau; M. Limon; Tobias A. Marriage; Danica Marsden; Krista Martocci; Philip Daniel Mauskopf; Harvey Moseley; C. B. Netterfield

The Atacama Cosmology Telescope was designed to measure small-scale anisotropies in the Cosmic Microwave Background and detect galaxy clusters through the Sunyaev-Zel’dovich effect. The instrument is located on Cerro Toco in the Atacama Desert, at an altitude of 5190 meters. A six-meter off-axis Gregorian telescope feeds a new type of cryogenic receiver, the Millimeter Bolometer Array Camera. The receiver features three 1000-element arrays of transition-edge sensor bolometers for observations at 148GHz, 218GHz, and 277GHz. Each detector array is fed by free space mm-wave optics. Each frequency band has a field of view of approximately 22 × 26. The telescope was commissioned in 2007 and has completed its third year of operations. We discuss the major components of the telescope, camera, and related systems, and summarize the instrument performance. Subject headings: Microwave Telescopes, CMB Observations


Applied Optics | 2007

Optical design of the Atacama Cosmology Telescope and the Millimeter Bolometric Array Camera

Joseph W. Fowler; Michael D. Niemack; Simon R. Dicker; A. M. Aboobaker; Peter A. R. Ade; E. S. Battistelli; Mark Joseph Devlin; R. P. Fisher; M. Halpern; Peter Charles Hargrave; Adam D. Hincks; M. Kaul; J. Klein; Judy M. Lau; M. Limon; Tobias A. Marriage; Philip Daniel Mauskopf; Lyman A. Page; Suzanne T. Staggs; Daniel S. Swetz; Eric R. Switzer; Robert Thornton; Carole Tucker

The Atacama Cosmology Telescope is a 6 m telescope designed to map the cosmic microwave background simultaneously at 145, 215, and 280 GHz with arcminute resolution. Each frequency will have a 32 by 32 element focal plane array of transition edge sensor bolometers. The telescope and the cold reimaging optics are optimized for millimeter-wave observations with these sensitive detectors. The design of each is described.


Physical Review Letters | 2011

Evidence for dark energy from the cosmic microwave background alone using the Atacama Cosmology Telescope lensing measurements.

Blake D. Sherwin; Joanna Dunkley; Sudeep Das; J. W. Appel; J. Richard Bond; C. Sofia Carvalho; Mark J. Devlin; Rolando Dünner; Thomas Essinger-Hileman; Joseph W. Fowler; Amir Hajian; M. Halpern; Matthew Hasselfield; Adam D. Hincks; Renée Hlozek; John P. Hughes; K. D. Irwin; Jeff Klein; Arthur Kosowsky; Tobias A. Marriage; Danica Marsden; Kavilan Moodley; F. Menanteau; Michael D. Niemack; Michael R. Nolta; Lyman A. Page; Lucas Parker; Erik D. Reese; Benjamin L. Schmitt; Neelima Sehgal

For the first time, measurements of the cosmic microwave background radiation (CMB) alone favor cosmologies with w = -1 dark energy over models without dark energy at a 3.2-sigma level. We demonstrate this by combining the CMB lensing deflection power spectrum from the Atacama Cosmology Telescope with temperature and polarization power spectra from the Wilkinson Microwave Anisotropy Probe. The lensing data break the geometric degeneracy of different cosmological models with similar CMB temperature power spectra. Our CMB-only measurement of the dark energy density Ω(Λ) confirms other measurements from supernovae, galaxy clusters, and baryon acoustic oscillations, and demonstrates the power of CMB lensing as a new cosmological tool.


The Astrophysical Journal | 2011

The Atacama Cosmology Telescope: Extragalactic Sources at 148 GHz in the 2008 Survey

Tobias A. Marriage; Jean Baptiste Juin; Yen-Ting Lin; Danica Marsden; Michael R. Nolta; Bruce Partridge; Peter A. R. Ade; Paula Aguirre; M. Amiri; J. W. Appel; L. Felipe Barrientos; E. S. Battistelli; John R. Bond; Ben Brown; B. Burger; J. A. Chervenak; Sudeep Das; Mark J. Devlin; Simon R. Dicker; W. Bertrand Doriese; Joanna Dunkley; Rolando Dünner; Thomas Essinger-Hileman; R. P. Fisher; Joseph W. Fowler; Amir Hajian; M. Halpern; Matthew Hasselfield; C. Hernández-Monteagudo; G. C. Hilton

We report on extragalactic sources detected in a 455 deg2 map of the southern sky made with data at a frequency of 148 GHz from the Atacama Cosmology Telescope (ACT) 2008 observing season. We provide a catalog of 157 sources with flux densities spanning two orders of magnitude: from 15 mJy to 1500 mJy. Comparison to other catalogs shows that 98% of the ACT detections correspond to sources detected at lower radio frequencies. Three of the sources appear to be associated with the brightest cluster galaxies of low-redshift X-ray-selected galaxy clusters. Estimates of the radio to millimeter-wave spectral indices and differential counts of the sources further bolster the hypothesis that they are nearly all radio sources, and that their emission is not dominated by re-emission from warm dust. In a bright (>50 mJy) 148 GHz selected sample with complete cross-identifications from the Australia Telescope 20 GHz survey, we observe an average steepening of the spectra between 5, 20, and 148 GHz with median spectral indices of α5-20 = –0.07 ± 0.06, α20-148 = –0.39 ± 0.04, and α5-148 = –0.20 ± 0.03. When the measured spectral indices are taken into account, the 148 GHz differential source counts are consistent with previous measurements at 30 GHz in the context of a source count model dominated by radio sources. Extrapolating with an appropriately rescaled model for the radio source counts, the Poisson contribution to the spatial power spectrum from synchrotron-dominated sources with flux density less than 20 mJy is C Sync = (2.8 ± 0.3) × 10–6μK2.


Review of Scientific Instruments | 2012

A high resolution gamma-ray spectrometer based on superconducting microcalorimeters

D. A. Bennett; Robert D. Horansky; Daniel R. Schmidt; Andrew S. Hoover; Ryan Winkler; Bradley K. Alpert; James A. Beall; W. B. Doriese; J. W. Fowler; C. P. Fitzgerald; G. C. Hilton; K. D. Irwin; V. Kotsubo; J. A. B. Mates; G. C. O’Neil; Michael W. Rabin; Carl D. Reintsema; F. J. Schima; Daniel S. Swetz; Leila R. Vale; Joel N. Ullom

Improvements in superconductor device fabrication, detector hybridization techniques, and superconducting quantum interference device readout have made square-centimeter-sized arrays of gamma-ray microcalorimeters, based on transition-edge sensors (TESs), possible. At these collecting areas, gamma microcalorimeters can utilize their unprecedented energy resolution to perform spectroscopy in a number of applications that are limited by closely-spaced spectral peaks, for example, the nondestructive analysis of nuclear materials. We have built a 256 pixel spectrometer with an average full-width-at-half-maximum energy resolution of 53 eV at 97 keV, a useable dynamic range above 400 keV, and a collecting area of 5 cm(2). We have demonstrated multiplexed readout of the full 256 pixel array with 236 of the pixels (91%) giving spectroscopic data. This is the largest multiplexed array of TES microcalorimeters to date. This paper will review the spectrometer, highlighting the instrument design, detector fabrication, readout, operation of the instrument, and data processing. Further, we describe the characterization and performance of the newest 256 pixel array.


The Astrophysical Journal | 2011

The Atacama Cosmology Telescope: Calibration with the Wilkinson Microwave Anisotropy Probe using cross-correlations

Amir Hajian; Viviana Acquaviva; Peter A. R. Ade; Paula Aguirre; M. Amiri; J. W. Appel; L. Felipe Barrientos; E. S. Battistelli; John R. Bond; Ben Brown; B. Burger; J. A. Chervenak; Sudeep Das; Mark J. Devlin; Simon R. Dicker; W. Bertrand Doriese; Joanna Dunkley; Rolando Dünner; Thomas Essinger-Hileman; R. P. Fisher; Joseph W. Fowler; M. Halpern; Matthew Hasselfield; C. Hernández-Monteagudo; G. C. Hilton; Matt Hilton; Adam D. Hincks; Renée Hlozek; K. M. Huffenberger; David H. Hughes

We present a new calibration method based on cross-correlations with the Wilkinson Microwave Anisotropy Probe (WMAP) and apply it to data from the Atacama Cosmology Telescope (ACT). ACTs observing strategy and map-making procedure allows an unbiased reconstruction of the modes in the maps over a wide range of multipoles. By directly matching the ACT maps to WMAP observations in the multipole range of 400 < l < 1000, we determine the absolute calibration with an uncertainty of 2% in temperature. The precise measurement of the calibration error directly impacts the uncertainties in the cosmological parameters estimated from the ACT power spectra. We also present a combined map based on ACT and WMAP data that has a high signal-to-noise ratio over a wide range of multipoles.We present a new calibration method based on cross-correlations with WMAP and apply it to data from the Atacama Cosmology Telescope (ACT). ACTs observing strategy and map making procedure allows an unbiased reconstruction of the modes in the maps over a wide range of multipoles. By directly matching the ACT maps to WMAP observations in the multipole range of 400 < ell < 1000, we determine the absolute calibration with an uncertainty of 2% in temperature. The precise measurement of the calibration error directly impacts the uncertainties in the cosmological parameters estimated from the ACT power spectra. We also present a combined map based on ACT and WMAP data that has high signal-to-noise over a wide range of multipoles.


Synchrotron Radiation News | 2014

Transition-Edge Sensor Microcalorimeters for X-ray Beamline Science

Joel N. Ullom; W. B. Doriese; Daniel A. Fischer; J. W. Fowler; G. C. Hilton; Cherno Jaye; Carl D. Reintsema; Daniel S. Swetz; Daniel R. Schmidt

An important and fast-growing technology in the realm of cryogenic detectors has recently been applied to beamline science: the superconducting Transition-Edge Sensor (TES). A TES consists of a thin metal film that is held in the superconducting-to-normal transition by a voltage bias. When a single X-ray photon is absorbed, the temperature and resistance of the film increase, which causes a negative-going current pulse with amplitude proportional to the deposited energy. The thin-film thermometer is typically coupled to a photon absorber composed of a high atomic number element such as bismuth or gold, so efficiencies near unity are possible for X-rays up to 10 keV. TESs are an example of a broader class of sensors called microcalorimeters that measure energetic events through a change in temperature. The energy resolution of a well-designed microcalorimeter is set by thermodynamic power fluctuations between the sensor and the local heat bath as well as by additional noise terms such as the Johnson noise in the sensing element. The energy resolution ΔE of a microcalorimeter is proportional to (kbT2C)1/2 where T is the sensor temperature and C is its specific heat. The temperature dependence of ΔE makes it advantageous to operate TESs at the lowest temperatures that can be conveniently reached, typically 0.1 K. For X-ray measurements between 1–10 keV, the dependence of ΔE on C limits the C of individual sensors to about 10−12 J/K, corresponding to device areas near 0.1 mm2 [1].


Journal of Synchrotron Radiation | 2015

High-resolution X-ray emission spectroscopy with transition-edge sensors: present performance and future potential

Jens Uhlig; W. B. Doriese; J. W. Fowler; Daniel S. Swetz; Cherno Jaye; Daniel A. Fischer; Carl D. Reintsema; D. A. Bennett; L.R. Vale; Ujjwal Mandal; Galen C. O'Neil; L. Miaja-Avila; Y. I. Joe; A. El Nahhas; Wilfred Fullagar; F. Parnefjord Gustafsson; Villy Sundström; Dharmalingam Kurunthu; G. C. Hilton; Daniel R. Schmidt; Joel N. Ullom

X-ray emission spectroscopy (XES) is a powerful element-selective tool to analyze the oxidation states of atoms in complex compounds, determine their electronic configuration, and identify unknown compounds in challenging environments. Until now the low efficiency of wavelength-dispersive X-ray spectrometer technology has limited the use of XES, especially in combination with weaker laboratory X-ray sources. More efficient energy-dispersive detectors have either insufficient energy resolution because of the statistical limits described by Fano or too low counting rates to be of practical use. This paper updates an approach to high-resolution X-ray emission spectroscopy that uses a microcalorimeter detector array of superconducting transition-edge sensors (TESs). TES arrays are discussed and compared with conventional methods, and shown under which circumstances they are superior. It is also shown that a TES array can be integrated into a table-top time-resolved X-ray source and a soft X-ray synchrotron beamline to perform emission spectroscopy with good chemical sensitivity over a very wide range of energies.

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Joel N. Ullom

National Institute of Standards and Technology

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G. C. Hilton

National Institute of Standards and Technology

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Daniel R. Schmidt

National Institute of Standards and Technology

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J. W. Fowler

National Institute of Standards and Technology

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W. B. Doriese

National Institute of Standards and Technology

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D. A. Bennett

National Institute of Standards and Technology

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Carl D. Reintsema

National Institute of Standards and Technology

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Mark J. Devlin

University of Pennsylvania

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Adam D. Hincks

University of British Columbia

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