G. Simard
McGill University
Network
Latest external collaboration on country level. Dive into details by clicking on the dots.
Publication
Featured researches published by G. Simard.
Proceedings of SPIE | 2014
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
Monthly Notices of the Royal Astronomical Society | 2016
D. Kirk; Y. Omori; A. Benoit-Lévy; R. Cawthon; C. L. Chang; P. Larsen; Adam Amara; David Bacon; T. M. Crawford; Scott Dodelson; P. Fosalba; T. Giannantonio; Gilbert P. Holder; Bhuvnesh Jain; Tomasz Kacprzak; Ofer Lahav; N. MacCrann; Andrina Nicola; Alexandre Refregier; E. Sheldon; K. Story; M. A. Troxel; J. D. Vieira; V. Vikram; J. Zuntz; Timothy M. C. Abbott; F. B. Abdalla; M. R. Becker; B. A. Benson; G. M. Bernstein
We measure the cross-correlation between weak lensing of galaxy images and of the cosmic microwave background (CMB). The effects of gravitational lensing on different sources will be correlated if the lensing is caused by the same mass fluctuations. We use galaxy shape measurements from 139 deg(2) of the Dark Energy Survey (DES) Science Verification data and overlapping CMB lensing from the South Pole Telescope (SPT) and Planck. The DES source galaxies have a median redshift of z(med) similar to 0.7, while the CMB lensing kernel is broad and peaks at z similar to 2. The resulting cross-correlation is maximally sensitive to mass fluctuations at z similar to 0.44. Assuming the Planck 2015 best-fitting cosmology, the amplitude of the DESxSPT cross-power is found to be A(SPT) = 0.88 +/- 0.30 and that from DESxPlanck to be A(Planck) = 0.86 +/- 0.39, where A = 1 corresponds to the theoretical prediction. These are consistent with the expected signal and correspond to significances of 2.9 sigma and 2.2 sigma, respectively. We demonstrate that our results are robust to a number of important systematic effects including the shear measurement method, estimator choice, photo-z uncertainty and CMB lensing systematics. We calculate a value of A = 1.08 +/- 0.36 for DESxSPT when we correct the observations with a simple intrinsic alignment model. With three measurements of this cross-correlation now existing in the literature, there is not yet reliable evidence for any deviation from the expected LCDM level of cross-correlation. We provide forecasts for the expected signal-to-noise ratio of the combination of the five-year DES survey and SPT-3G.
The Astrophysical Journal | 2018
G. Simard; Y. Omori; K. Aylor; E. Baxter; B. A. Benson; L. E. Bleem; J. E. Carlstrom; C. L. Chang; H. M. Cho; R. Chown; T. M. Crawford; A. T. Crites; T. de Haan; M. Dobbs; W. Everett; E. M. George; N. W. Halverson; N. L. Harrington; J. W. Henning; G. P. Holder; Z. Hou; W. L. Holzapfel; J. D. Hrubes; L. Knox; A. T. Lee; E. M. Leitch; D. Luong-Van; A. Manzotti; J. J. McMahon; S. S. Meyer
We report constraints on cosmological parameters from the angular power spectrum of a cosmic microwave background (CMB) gravitational lensing potential map created using temperature data from 2500 deg2 of South Pole Telescope (SPT) data supplemented with data from Planck in the same sky region, with the statistical power in the combined map primarily from the SPT data. We fit the lensing power spectrum to a model including cold dark matter and a cosmological constant (ΛCDM), and to models with single-parameter extensions to ΛCDM. We find constraints that are comparable to and consistent with those found using the full-sky Planck CMB lensing data, e.g., σ_8 Ω^(0.25)_m = 0.598 ± 0.024 from the lensing data alone with weak priors placed on other parameters. Combining with primary CMB data, we explore single-parameter extensions to ΛCDM. We find Ω_k = -0.012^(+0.021)_(-0.023) or M_ν < 0.70 eV at 95% confidence, in good agreement with results including the lensing potential as measured by Planck. We include two parameters that scale the effect of lensing on the CMB: A_L, which scales the lensing power spectrum in both the lens reconstruction power and in the smearing of the acoustic peaks, and A^(oo), which scales only the amplitude of the lensing reconstruction power spectrum. We find A^(oo) x A_L = 1.01 ± 0.08 for the lensing map made from combined SPT and Planck data, indicating that the amount of lensing is in excellent agreement with expectations from the observed CMB angular power spectrum when not including the information from smearing of the acoustic peaks.
IEEE Transactions on Applied Superconductivity | 2015
C. L. Chang; Peter A. R. Ade; Z. Ahmed; S. W. Allen; K. Arnold; J. E. Austermann; A. N. Bender; L. E. Bleem; B. A. Benson; J. E. Carlstrom; H. M. Cho; S. T. Ciocys; Jean-François Cliche; T. M. Crawford; A. Cukierman; Junjia Ding; 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; J. Hubmayr
Low loss superconducting microstrip is an essential component in realizing 100 kilo-pixel multichroic cosmic microwave background detector arrays. We have been developing a low loss microstrip by understanding and controlling the loss mechanisms. We present the fabrication of the superconducting microstrip, the loss measurements at a few GHz frequencies using half-wavelength resonators, and the loss measurements at 220 GHz frequencies with the superconducting microstrip coupled to slot antennas at one end and to TES detectors at the other end. The measured loss tangent of the microstrip made of sputtered Nb and SiOx is 1-2e-3.
The Astrophysical Journal | 2017
Y. Omori; R. Chown; G. Simard; K. T. Story; K. Aylor; E. Baxter; B. A. Benson; L. E. Bleem; J. E. Carlstrom; C. L. Chang; H. M. Cho; T. M. Crawford; A. T. Crites; T. de Haan; M. Dobbs; W. Everett; E. M. George; N. W. Halverson; N. L. Harrington; G. P. Holder; Z. Hou; W. L. Holzapfel; J. D. Hrubes; L. Knox; A. T. Lee; E. M. Leitch; D. Luong-Van; A. Manzotti; D. P. Marrone; J. J. McMahon
The Astrophysical Journal | 2018
R. Chown; N. L. Harrington; A. A. Stark; G. Simard; R. Williamson; Dobbs; T. M. Crawford; A. T. Lee; S. Padin; E. M. George; L. Knox; D. P. Marrone; W. Everett; J. W. Henning; C. L. Reichardt; L. Mocanu; B. A. Benson; K. Aylor; Zachary K. Staniszewski; J. T. Sayre; J. J. Mohr; K. T. Story; S. S. Meyer; Z. Hou; K. Vanderlinde; K. K. Schaffer; J. E. Carlstrom; C. Pryke; W. L. Holzapfel; N. W. Halverson