Jay B. Holberg
University of Arizona
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Featured researches published by Jay B. Holberg.
The Astrophysical Journal | 2017
Howard E. Bond; Gail H. Schaefer; Ronald L. Gilliland; Jay B. Holberg; Brian D. Mason; Irving W. Lindenblad; Miranda Seitz-McLeese; W. David Arnett; Pierre Demarque; Federico Spada; Patrick A. Young; M. A. Barstow; M. R. Burleigh; Donald H. Gudehus
Sirius, the seventh-nearest stellar system, is a visual binary containing the metallic-line A1 V star Sirius A, brightest star in the sky, orbited in a 50.13-year period by Sirius B, the brightest and nearest white dwarf (WD). Using images obtained over nearly two decades with the Hubble Space Telescope (HST), along with photographic observations covering almost 20 years, and nearly 2300 historical measurements dating back to the 19th century, we determine precise orbital elements for the visual binary. Combined with the parallax and the motion of the A component, these elements yield dynamical masses of 2.063+/-0.023 Msun and 1.018+/-0.011 Msun for Sirius A and B, respectively. Our precise HST astrometry rules out third bodies orbiting either star in the system, down to masses of ~15-25 Mjup. The location of Sirius B in the H-R diagram is in excellent agreement with theoretical cooling tracks for WDs of its dynamical mass, and implies a cooling age of ~126 Myr. The position of Sirius B in the mass-radius plane is also consistent with WD theory, assuming a carbon-oxygen core. Including the pre-WD evolutionary timescale of the assumed progenitor, the total age of Sirius B is about 228+/-10 Myr. We calculated evolutionary tracks for stars with the dynamical mass of Sirius A, using two independent codes. We find it necessary to assume a slightly sub-solar metallicity, of about 0.85 Zsun, to fit its location in the luminosity-radius plane. The age of Sirius A based on these models is about 237-247 Myr, with uncertainties of +/-15 Myr, consistent with that of the WD companion. We discuss astrophysical puzzles presented by the Sirius system, including the probability that the two stars must have interacted in the past, even though there is no direct evidence for this, and the orbital eccentricity remains high.
The Astrophysical Journal | 2016
Gautham S. Narayan; Tim Axelrod; Jay B. Holberg; Thomas Matheson; Abhijit Saha; Edward W. Olszewski; Jenna Claver; Christopher W. Stubbs; Ralph C. Bohlin; Susana Elizabeth Deustua; Armin Rest
NASA [NAS5-26555]; NASA Office of Space Science [NNX13AC07G]; Ministerio de Ciencia, Tecnologia e Innovacion Productiva (Argentina) [GS-2013A-Q-8, GS-2013B-Q-22]
The Astrophysical Journal | 2016
Lotfi Ben-Jaffel; Jay B. Holberg
CNES, Universite Pierre et Marie Curie (UPMC); Centre National de la Recherche Scientifique (CNRS) in France
Universe | 2017
Matthew B. Bainbridge; M. A. Barstow; Nicole Reindl; W.U.L. Tchang-Brillet; Thomas R. Ayres; J. K. Webb; John D. Barrow; Jiting Hu; Jay B. Holberg; S. P. Preval; W.M.G. Ubachs; Vladimir Dzuba; V. V. Flambaum; Vincent Dumont; J. C. Berengut
Hot white dwarf stars are the ideal probe for a relationship between the fine-structure constant and strong gravitational fields, providing us with an opportunity for a direct observational test. We study a sample of hot white dwarf stars, combining far-UV spectroscopic observations, atomic physics, atmospheric modelling, and fundamental physics in the search for variation in the fine structure constant. This variation manifests as shifts in the observed wavelengths of absorption lines, such as quadruply ionized iron (FeV) and quadruply ionized nickel (NiV), when compared to laboratory wavelengths. Berengut et al. (Phys. Rev. Lett. 2013, 111, 010801) demonstrated the validity of such an analysis using high-resolution Space Telescope Imaging Spectrograph (STIS) spectra of G191-B2B. We have made three important improvements by: (a) using three new independent sets of laboratory wavelengths; (b) analysing a sample of objects; and (c) improving the methodology by incorporating robust techniques from previous studies towards quasars (the Many Multiplet method). A successful detection would be the first direct measurement of a gravitational field effect on a bare constant of nature. Here we describe our approach and present preliminary results from nine objects using both FeV and NiV.
Monthly Notices of the Royal Astronomical Society | 2017
S. P. Preval; M. A. Barstow; N. R. Badnell; Ivan Hubeny; Jay B. Holberg
To calculate realistic models of objects with Ni in their atmospheres, accurate atomic data for the relevant ionization stages needs to be included in model atmosphere calculations. In the context of white dwarf stars, we investigate the effect of changing the Ni {\sc iv}-{\sc vi} bound-bound and bound-free atomic data has on model atmosphere calculations. Models including PICS calculated with {\sc autostructure} show significant flux attenuation of up to
Monthly Notices of the Royal Astronomical Society | 2018
Simon R.G. Joyce; M. A. Barstow; S. L. Casewell; M. R. Burleigh; Jay B. Holberg; Howard E. Bond
\sim 80
Archive | 2017
Matthew B. Bainbridge; M. A. Barstow; N Reindl; John David Barrow; J. K. Webb; J Hu; S. P. Preval; Jay B. Holberg; G Nave; L Tchang-Brillet; Thomas R. Ayres
\% shortward of 180\AA\, in the EUV region compared to a model using hydrogenic PICS. Comparatively, models including a larger set of Ni transitions left the EUV, UV, and optical continua unaffected. We use models calculated with permutations of this atomic data to test for potential changes to measured metal abundances of the hot DA white dwarf G191-B2B. Models including {\sc autostructure} PICS were found to change the abundances of N and O by as much as
Monthly Notices of the Royal Astronomical Society | 2016
Jay B. Holberg; T. D. Oswalt; Edward M. Sion; George P. McCook
\sim 22
Archive | 2010
Kevin R. Covey; Abhijit Saha; Timothy C. Beers; John J. Bochanski; Pat Boeshaar; Adam J. Burgasser; Phillip A. Cargile; Yanping Chu; Charles F. Claver; Kenneth H. Cook; Saurav Dhital; Suzanne L. Hawley; Leslie Hebb; Todd J. Henry; Eric J. Hilton; Jay B. Holberg; Zeljko Ivezic; Mario Juric; Stella Kafka; Jasonjot Singh Kalirai; Sebastien Lepine; Lucas M. Macri; P. McGehee; David G. Monet; Knut Olsen; John V. Pepper; Andrej Prsa; Ata Sarajedini; Nicole M. Silvestri; Keivan G. Stassun
\% compared to models using hydrogenic PICS, but heavier species were relatively unaffected. Models including {\sc autostructure} PICS caused the abundances of N/O {\sc iv} and {\sc v} to diverge. This is because the increased opacity in the {\sc autostructure} PICS model causes these charge states to form higher in the atmosphere, moreso for N/O {\sc v}. Models using an extended line list caused significant changes to the Ni {\sc iv}-{\sc v} abundances. While both PICS and an extended line list cause changes in both synthetic spectra and measured abundances, the biggest changes are caused by using {\sc autostructure} PICS for Ni.
arXiv: Earth and Planetary Astrophysics | 2016
Lotfi Ben-Jaffel; Jay B. Holberg
SRGJ acknowledges support from the Science and Technology Facilities Council (STFC, UK). MAB acknowledges support from the Gaia post-launch support programme of the UK Space Agency. This work has made use of data from the European Space Agency (ESA) mission Gaia, processed by the Gaia Data Processing and Analysis Consortium (DPAC). Funding for the DPAC has been provided by national institutions, in particular the institutions participating in the Gaia Multilateral Agreement. JBH was partially supported by NSF grant AST-1413537.