S. T. McWilliams
West Virginia University
Network
Latest external collaboration on country level. Dive into details by clicking on the dots.
Publication
Featured researches published by S. T. McWilliams.
The Astrophysical Journal | 2016
Zaven Arzoumanian; A. Brazier; S. Burke-Spolaor; S. J. Chamberlin; S. Chatterjee; B. Christy; J. M. Cordes; Neil J. Cornish; K. Crowter; Paul Demorest; X. Deng; T. Dolch; Justin Ellis; R. D. Ferdman; E. Fonseca; N. Garver-Daniels; M. E. Gonzalez; F. A. Jenet; Glenn Jones; M. L. Jones; V. M. Kaspi; M. Koop; M. T. Lam; T. J. W. Lazio; Lina Levin; Andrea N. Lommen; D. R. Lorimer; J. Luo; R. S. Lynch; D. R. Madison
We compute upper limits on the nanohertz-frequency isotropic stochastic gravitational wave background (GWB) using the 9 year data set from the North American Nanohertz Observatory for Gravitational Waves (NANOGrav) collaboration. Well-tested Bayesian techniques are used to set upper limits on the dimensionless strain amplitude (at a frequency of 1 yr^(−1) for a GWB from supermassive black hole binaries of A_(gw) < 1.5 x 10^(-15). We also parameterize the GWB spectrum with a broken power-law model by placing priors on the strain amplitude derived from simulations of Sesana and McWilliams et al. Using Bayesian model selection we find that the data favor a broken power law to a pure power law with odds ratios of 2.2 and 22 to one for the Sesana and McWilliams prior models, respectively. Using the broken power-law analysis we construct posterior distributions on environmental factors that drive the binary to the GW-driven regime including the stellar mass density for stellar-scattering, mass accretion rate for circumbinary disk interaction, and orbital eccentricity for eccentric binaries, marking the first time that the shape of the GWB spectrum has been used to make astrophysical inferences. Returning to a power-law model, we place stringent limits on the energy density of relic GWs, Ω_(gw)(f)h^2 < 4.2 x 10^(-10). Our limit on the cosmic string GWB, Ω_(gw)(f)h^2 < 2.2 x 10^(-10), translates to a conservative limit on the cosmic string tension with Gµ < 3.3 x 10^(-8), a factor of four better than the joint Planck and high-l cosmic microwave background data from other experiments.
Monthly Notices of the Royal Astronomical Society | 2016
L. Lentati; R. M. Shannon; W. A. Coles; J. P. W. Verbiest; R. van Haasteren; Justin Ellis; R. N. Caballero; R. N. Manchester; Zaven Arzoumanian; S. Babak; C. G. Bassa; N. D. R. Bhat; P. Brem; M. Burgay; S. Burke-Spolaor; D. J. Champion; S. Chatterjee; I. Cognard; J. M. Cordes; S. Dai; Paul Demorest; G. Desvignes; T. Dolch; R. D. Ferdman; E. Fonseca; Jonathan R. Gair; M. E. Gonzalez; E. Graikou; L. Guillemot; J. W. T. Hessels
We analyse the stochastic properties of the 49 pulsars that comprise the first International Pulsar Timing Array (IPTA) data release. We use Bayesian methodology, performing model selection to determine the optimal description of the stochastic signals present in each pulsar. In addition to spin-noise and dispersion-measure (DM) variations, these models can include timing noise unique to a single observing system, or frequency band. We show the improved radio-frequency coverage and presence of overlapping data from different observing systems in the IPTA data set enables us to separate both system and band-dependent effects with much greater efficacy than in the individual PTA data sets. For example, we show that PSR J1643−1224 has, in addition to DM variations, significant band-dependent noise that is coherent between PTAs which we interpret as coming from time-variable scattering or refraction in the ionised interstellar medium. Failing to model these different contributions appropriately can dramatically alter the astrophysical interpretation of the stochastic signals observed in the residuals. In some cases, the spectral exponent of the spin noise signal can vary from 1.6 to 4 depending upon the model, which has direct implications for the long-term sensitivity of the pulsar to a stochastic gravitational-wave (GW) background. By using a more appropriate model, however, we can greatly improve a pulsars sensitivity to GWs. For example, including system and band-dependent signals in the PSR J0437−4715 data set improves the upper limit on a fiducial GW background by ∼ 60% compared to a model that includes DM variations and spin-noise only.
The Astrophysical Journal | 2018
Zaven Arzoumanian; P. T. Baker; A. Brazier; S. Burke-Spolaor; S. J. Chamberlin; S. Chatterjee; B. Christy; J. M. Cordes; Neil J. Cornish; F. Crawford; H. Thankful Cromartie; K. Crowter; Megan E. DeCesar; Paul Demorest; T. Dolch; Justin Ellis; R. D. Ferdman; E. C. Ferrara; W. M. Folkner; E. Fonseca; N. Garver-Daniels; Peter A. Gentile; Roland Haas; J. S. Hazboun; E. A. Huerta; K. Islo; Glenn Jones; M. L. Jones; David L. Kaplan; V. M. Kaspi
We search for an isotropic stochastic gravitational-wave background (GWB) in the newly released 11 year data set from the North American Nanohertz Observatory for Gravitational Waves (NANOGrav). While we find no evidence for a GWB, we place constraints on a population of inspiraling supermassive black hole (SMBH) binaries, a network of decaying cosmic strings, and a primordial GWB. For the first time, we find that the GWB constraints are sensitive to the solar system ephemeris (SSE) model used and that SSE errors can mimic a GWB signal. We developed an approach that bridges systematic SSE differences, producing the first pulsar-timing array (PTA) constraints that are robust against SSE errors. We thus place a 95% upper limit on the GW-strain amplitude of A_(GWB) < 1.45 × 10^(−15) at a frequency of f = 1 yr^(−1) for a fiducial f^(−2/3) power-law spectrum and with interpulsar correlations modeled. This is a factor of ~2 improvement over the NANOGrav nine-year limit calculated using the same procedure. Previous PTA upper limits on the GWB (as well as their astrophysical and cosmological interpretations) will need revision in light of SSE systematic errors. We use our constraints to characterize the combined influence on the GWB of the stellar mass density in galactic cores, the eccentricity of SMBH binaries, and SMBH–galactic-bulge scaling relationships. We constrain the cosmic-string tension using recent simulations, yielding an SSE-marginalized 95% upper limit of Gμ < 5.3 × 10^(−11)—a factor of ~2 better than the published NANOGrav nine-year constraints. Our SSE-marginalized 95% upper limit on the energy density of a primordial GWB (for a radiation-dominated post-inflation universe) is Ω_(GWB)(f) h^2 < 3.4 × 10^(−10).
Physical Review D | 2016
V. Tiwari; Sergey Klimenko; N. Christensen; E. A. Huerta; S. R P Mohapatra; A. Gopakumar; M. Haney; P. Ajith; S. T. McWilliams; G. Vedovato; M. Drago; F. Salemi; G. A. Prodi; C. Lazzaro; S. Tiwari; G. Mitselmakher; F. Da Silva
Most compact binary systems are expected to circularize before the frequency of emitted gravitational waves (GWs) enters the sensitivity band of the ground based interferometric detectors. However, several mechanisms have been proposed for the formation of binary systems, which retain eccentricity throughout their lifetimes. Since no matched-filtering algorithm has been developed to extract continuous GW signals from compact binaries on orbits with low to moderate values of eccentricity, and available algorithms to detect binaries on quasicircular orbits are suboptimal to recover these events, in this paper we propose a search method for detection of gravitational waves produced from the coalescences of eccentric binary black holes (eBBH). We study the search sensitivity and the false alarm rates on a segment of data from the second joint science run of LIGO and Virgo detectors, and discuss the implications of the eccentric binary search for the advanced GW detectors.
The Astrophysical Journal | 2016
Stephen Taylor; E. A. Huerta; Jonathan R. Gair; S. T. McWilliams
The couplings between supermassive black-hole binaries and their environments within galactic nuclei have been well studied as part of the search for solutions to the final parsec problem. The scattering of stars by the binary or the interaction with a circumbinary disk may efficiently drive the system to sub-parsec separations, allowing the binary to enter a regime where the emission of gravitational waves can drive it to merger within a Hubble time. However, these interactions can also affect the orbital parameters of the binary. In particular, they may drive an increase in binary eccentricity which survives until the systems gravitational-wave signal enters the pulsar-timing array band. Therefore, if we can measure the eccentricity from observed signals, we can potentially deduce some of the properties of the binary environment. To this end, we build on previous techniques to present a general Bayesian pipeline with which we can detect and estimate the parameters of an eccentric supermassive black-hole binary system with pulsar-timing arrays. Additionally, we generalize the pulsar-timing array
Monthly Notices of the Royal Astronomical Society | 2018
R. N. Caballero; Y. J. Guo; K. J. Lee; P. Lazarus; D. J. Champion; G. Desvignes; M. Kramer; K. Plant; Zaven Arzoumanian; M. Bailes; C. G. Bassa; N. D. R. Bhat; A. Brazier; M. Burgay; S. Burke-Spolaor; S. J. Chamberlin; S. Chatterjee; I. Cognard; J. M. Cordes; S. Dai; Paul Demorest; T. Dolch; R. D. Ferdman; E. Fonseca; Jonathan R. Gair; N. Garver-Daniels; Peter A. Gentile; M. E. Gonzalez; E. Graikou; L. Guillemot
\mathcal{F}_e
Monthly Notices of the Royal Astronomical Society | 2016
J. P. W. Verbiest; L. Lentati; George Hobbs; R. van Haasteren; Paul Demorest; G. H. Janssen; J. B. Wang; G. Desvignes; R. N. Caballero; M. J. Keith; D. J. Champion; Zaven Arzoumanian; S. Babak; C. G. Bassa; N. D. R. Bhat; A. Brazier; P. Brem; M. Burgay; S. Burke-Spolaor; S. J. Chamberlin; S. Chatterjee; B. Christy; I. Cognard; J. M. Cordes; S. Dai; T. Dolch; Justin Ellis; R. D. Ferdman; E. Fonseca; Jonathan R. Gair
-statistic to eccentric systems, and show that both this statistic and the Bayesian pipeline are robust when studying circular or arbitrarily eccentric systems. We explore how eccentricity influences the detection prospects of single gravitational-wave sources, as well as the detection penalty incurred by employing a circular waveform template to search for eccentric signals, and conclude by identifying important avenues for future study.
The Astrophysical Journal | 2015
Zaven Arzoumanian; A. Brazier; S. Burke-Spolaor; S. J. Chamberlin; Shami Chatterjee; B. Christy; J. M. Cordes; Neil J. Cornish; Paul Demorest; X. Deng; T. Dolch; Justin Ellis; R. D. Ferdman; E. Fonseca; N. Garver-Daniels; F. A. Jenet; Glenn Jones; V. M. Kaspi; M. Koop; M. T. Lam; T. J. W. Lazio; Lina Levin; Andrea N. Lommen; D. R. Lorimer; J. Luo; R. S. Lynch; D. R. Madison; M. A. McLaughlin; S. T. McWilliams; David J. Nice
Pulsar-timing analyses are sensitive to errors in the Solar-system ephemerides (SSEs) that timing models utilize to estimate the location of the Solar-system barycentre, the quasi-inertial reference frame to which all recorded pulse times-of-arrival are referred. Any error in the SSE will affect all pulsars, therefore pulsar timing arrays (PTAs) are a suitable tool to search for such errors and impose independent constraints on relevant physical parameters. We employ the first data release of the International Pulsar Timing Array to constrain the masses of the planet–moons systems and to search for possible unmodelled objects (UMOs) in the Solar system. We employ 10 SSEs from two independent research groups, derive and compare mass constraints of planetary systems, and derive the first PTA mass constraints on asteroid-belt objects. Constraints on planetary-system masses have been improved by factors of up to 20 from the previous relevant study using the same assumptions, with the mass of the Jovian system measured at 9.5479189(3) × 10^(−4) M⊙. The mass of the dwarf planet Ceres is measured at 4.7(4) × 10^(−10) M⊙. We also present the first sensitivity curves using real data that place generic limits on the masses of UMOs, which can also be used as upper limits on the mass of putative exotic objects. For example, upper limits on dark-matter clumps are comparable to published limits using independent methods. While the constraints on planetary masses derived with all employed SSEs are consistent, we note and discuss differences in the associated timing residuals and UMO sensitivity curves.