T. K. Watson
Southwestern University
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The Astrophysical Journal | 1998
S. J. Kleinman; R. E. Nather; D. E. Winget; J. C. Clemens; P. A. Bradley; A. Kanaan; J. L. Provencal; C. F. Claver; T. K. Watson; K. Yanagida; A. Nitta; J. S. Dixson; Matt A. Wood; A. D. Grauer; B. P. Hine; G. Fontaine; James Liebert; D. J. Sullivan; D. T. Wickramasinghe; N. Achilleos; T. M. K. Marar; S. Seetha; B. N. Ashoka; E. G. Meištas; Elia M. Leibowitz; P. Moskalik; Jurek Krzesinski; J.-E. Solheim; A. Bruvold; D. O'Donoghue
The white dwarfs are promising laboratories for the study of cosmochronology and stellar evolution. Through observations of the pulsating white dwarfs, we can measure their internal structures and compositions, critical to understanding post main sequence evolution, along with their cooling rates, allowing us to calibrate their ages directly. The most important set of white dwarf variables to measure are the oldest of the pulsators, the cool DAVs, which have not previously been explored through asteroseismology due to their complexity and instability. Through a time-series photometry data set spanning ten years, we explore the pulsation spectrum of the cool DAV, G29-38 and find an underlying structure of 19 (not including multiplet components) normal-mode, probably l=1 pulsations amidst an abundance of time variability and linear combination modes. Modelling results are incomplete, but we suggest possible starting directions and discuss probable values for the stellar mass and hydrogen layer size. For the first time, we have made sense out of the complicated power spectra of a large-amplitude DA pulsator. We have shown its seemingly erratic set of observed frequencies can be understood in terms of a recurring set of normal-mode pulsations and their linear combinations. With this result, we have opened the interior secrets of the DAVs to future asteroseismological modelling, thereby joining the rest of the known white dwarf pulsators.
Monthly Notices of the Royal Astronomical Society | 2005
D. W. Kurtz; Chris Cameron; M. S. Cunha; N. Dolez; G. Vauclair; E. Pallier; A. Ulla; S. O. Kepler; A. F. M. da Costa; A. Kanaan; L. Fraga; O. Giovannini; Matt A. Wood; N. Silvestri; S. D. Kawaler; R. L. Riddle; M. D. Reed; T. K. Watson; T. S. Metcalfe; Anjum S. Mukadam; R. E. Nather; D. E. Winget; Atsuko Nitta; S. J. Kleinman; Joyce Ann Guzik; P. A. Bradley; Jaymie M. Matthews; K. Sekiguchi; D. J. Sullivan; T. Sullivan
HR 1217 is one of the best-studied rapidly oscillating Ap (roAp) stars, with a frequency spectrum of alternating even- and odd-� modes that are distorted by the presence of a strong, global magnetic field. Several recent theoretical studies have found that within the observable
web science | 2004
M. D. Reed; S. D. Kawaler; S. Zola; X. J. Jiang; S. Dreizler; S. Schuh; Jochen L. Deetjen; R. Kalytis; E. G. Meištas; R. Janulis; D. Ališauskas; Jurek Krzesinski; M. Vučković; P. Moskalik; W. Ogloza; A. Baran; G. Stachowski; D. W. Kurtz; J. M. Gonzalez Perez; Anjum S. Mukadam; T. K. Watson; C. Koen; P. A. Bradley; M. S. Cunha; Mukremin Kilic; E. W. Klumpe; R. F. Carlton; G. Handler; D. Kilkenny; R. L. Riddle
Since pulsating subdwarf B (sdBV or EC14026) stars were first discovered, observational efforts have tried to realize their potential for constraining the interior physics of extreme horizontal branch stars. Difficulties encountered along the way include uncertain mode identifications and a lack of stable pulsation mode properties. Here we report on Feige 48, an sdBV star for which follow-up observations have been obtained spanning more than four years. These observations show some stable pulsation modes. We resolve the temporal spectrum into five stable pulsation periods in the range 340–380 s with amplitudes less than 1 per cent, and two additional periods that appear in one data set each. The three largest amplitude periodicities are nearly equally spaced, and we explore the consequences of identifying them as a rotationally split l= 1 triplet by consulting a representative stellar model. The general stability of the pulsation amplitudes and phases allows us to use the pulsation phases to constrain the time-scale of evolution for this sdBV star. Additionally, we are able to place interesting limits on any stellar or planetary companion to Feige 48.
The Astrophysical Journal | 2003
Anjum S. Mukadam; S. O. Kepler; D. E. Winget; R. E. Nather; Mukremin Kilic; Fergal Mullally; T. von Hippel; S. J. Kleinman; Atsuko Nitta; Joyce Ann Guzik; P. A. Bradley; Jaymie M. Matthews; K. Sekiguchi; D. J. Sullivan; T. Sullivan; R. R. Shobbrook; Peter V. Birch; X. J. Jiang; Dong-Ling Xu; S. Joshi; B. N. Ashoka; P. Ibbetson; E. M. Leibowitz; Eran O. Ofek; E. G. Meištas; R. Janulis; D. Ališauskas; R. Kalytis; G. Handler; D. Kilkenny
We report our analysis of the stability of pulsation periods in the DAV star (pulsating hydrogen atmosphere white dwarf) ZZ Ceti, also called R548. On the basis of observations that span 31 years, we conclude that the period 213.13 s observed in ZZ Ceti drifts at a rate dP/dt ≤ (5.5 ± 1.9) × 10-15 s s-1, after correcting for proper motion. Our results are consistent with previous values for this mode and an improvement over them because of the larger time base. The characteristic stability timescale implied for the pulsation period is P/ ≥ 1.2 Gyr, comparable to the theoretical cooling timescale for the star. Our current stability limit for the period 213.13 s is only slightly less than the present measurement for another DAV, G117-B15A, for the period 215.2 s, establishing this mode in ZZ Ceti as the second most stable optical clock known, comparable to atomic clocks and more stable than most pulsars. Constraining the cooling rate of ZZ Ceti aids theoretical evolutionary models and white dwarf cosmochronology. The drift rate of this clock is small enough that we can set interesting limits on reflex motion due to planetary companions.
The Astrophysical Journal | 2006
R. I. Hynes; Edward L. Robinson; K. J. Pearson; Dawn M. Gelino; W. Cui; Y. Q. Xue; Matt A. Wood; T. K. Watson; D. E. Winget; Isaac M. Silver
We present simultaneous multicolor infrared and optical photometry of the black hole X-ray transient XTE J1118+480 during its short 2005 January outburst, supported by simultaneous X-ray observations. The variability is dominated by short timescales, ~10 s, although a weak superhump also appears to be present in the optical. The optical rapid variations, at least, are well correlated with those in X-rays. Infrared JHK_s photometry, as in the previous outburst, exhibits especially large-amplitude variability. The spectral energy distribution (SED) of the variable infrared component can be fitted with a power law of slope α = -0.78 ± 0.07, where F_ν ∝ ν_α. There is no compelling evidence for evolution in the slope over five nights, during which time the source brightness decayed along almost the same track as seen in variations within the nights. We conclude that both short-term variability and longer timescale fading are dominated by a single component of constant spectral shape. We cannot fit the SED of the IR variability with a credible thermal component, either optically thick or thin. This IR SED is, however, approximately consistent with optically thin synchrotron emission from a jet. These observations therefore provide indirect evidence to support jet-dominated models for XTE J1118+480 and also provide a direct measurement of the slope of the optically thin emission, which is impossible, based on the average spectral energy distribution alone.
web science | 2002
G. Vauclair; P. Moskalik; B. Pfeiffer; M. Chevreton; N. Dolez; B. Serre; S. J. Kleinman; M. A. Barstow; A. E. Sansom; J.-E. Solheim; Juan Antonio Belmonte; Steven D. Kawaler; S. O. Kepler; A. Kanaan; O. Giovannini; D. E. Winget; T. K. Watson; R. E. Nather; J. C. Clemens; J. L. Provencal; J. S. Dixson; K. Yanagida; A. Nitta Kleinman; M. H. Montgomery; E. W. Klumpe; A. Bruvold; M. S. O'Brien; C. J. Hansen; A. D. Grauer; P. A. Bradley
The pulsating PG 1159 planetary nebula central star RXJ 2117+3412 has been observed over three successive seasons of a multisite photometric campaign. The asteroseismological analysis of the data, based on the 37 identified ` = 1 modes among the 48 independent pulsation frequencies detected in the power spectrum, leads to the derivation of the rotational splitting, the period spacing and the mode trapping cycle and amplitude, from which a number of fundamental parameters can be deduced. The average rotation period is 1.16 ± 0.05 days. The trend for the rotational splitting to decrease with increasing periods is incompatible with a solid body rotation. The total mass is 0.56 −0.04 M and the He-rich envelope mass fraction is in the range 0.013–0.078 M∗. The luminosity derived from asteroseismology is log(L/L ) = 4.05 +0.23 −0.32 and the distance 760 +230 −235 pc. At such a distance, the linear size of the planetary nebulae is 2.9 ± 0.9 pc. The role of mass loss on the excitation mechanism and its consequence on the amplitude variations is discussed.
Monthly Notices of the Royal Astronomical Society | 2002
D. W. Kurtz; S. D. Kawaler; R. L. Riddle; M. D. Reed; M. S. Cunha; Matt A. Wood; N. Silvestri; T. K. Watson; N. Dolez; P. Moskalik; S. Zola; E. Pallier; Joyce Ann Guzik; T. S. Metcalfe; Anjum S. Mukadam; R. E. Nather; D. E. Winget; D. J. Sullivan; T. Sullivan; K. Sekiguchi; X. J. Jiang; R. R. Shobbrook; B. N. Ashoka; S. Seetha; S. Joshi; D. O'Donoghue; G. Handler; M. Mueller; J. M. Gonzalez Perez; J.-E. Solheim
ABSTRACT HR1217 is a prototypical rapidly oscillating Ap star that has presented a test tothe theory of nonradial stellar pulsation. Prior observations showed a clear patternof five modes with alternating frequency spacings of 33.3µHz and 34.6µHz, with asixth mode at a problematic spacing of 50.0µHz (which equals 1.5×33.3µHz) to thehigh-frequency side. Asymptotic pulsation theory allowed for a frequency spacing of34µHz, but hipparcos observations rule out such a spacing. Theoretical calculationsof magnetoacoustic modes in Ap stars by Cunha (2001) predicted that there shouldbe a previously undetected mode 34µHz higher than the main group, with a smallerspacing between it and the highest one. In this Letter, we present preliminary resultsfrom a multi-site photometric campaign on the rapidly oscillating Ap star HR1217using the “Whole Earth Telescope”. While a complete analysis of the data will appearin a later paper, one outstanding result from this run is the discovery of a newlydetected frequency in the pulsation spectrum of this star, at the frequency predictedby Cunha (2001).Keywords: Stars: oscillations – stars: variables – stars: individual (HR1217) – stars:magnetic.
The Astrophysical Journal | 2009
Judith L. Provencal; M. H. Montgomery; A. Kanaan; Harry L. Shipman; D. Childers; A. Baran; S. O. Kepler; M. D. Reed; A.-Y. Zhou; J. R. Eggen; T. K. Watson; D. E. Winget; Susan E. Thompson; Basmah Riaz; Atsuko Nitta; S. J. Kleinman; R. Crowe; J. Slivkoff; P. Sherard; N. Purves; P. M. Binder; R. Knight; S.-L. Kim; W. P. Chen; M. Yang; H. C. Lin; C. C. Lin; C. W. Chen; X. J. Jiang; A. V. Sergeev
We report on the analysis of 436.1 hr of nearly continuous high-speed photometry on the pulsating DB white dwarf GD358 acquired with the Whole Earth Telescope (WET) during the 2006 international observing run, designated XCOV25. The Fourier transform (FT) of the light curve contains power between 1000 and 4000 μHz, with the dominant peak at 1234 μHz. We find 27 independent frequencies distributed in 10 modes, as well as numerous combination frequencies. Our discussion focuses on a new asteroseismological analysis of GD358, incorporating the 2006 data set and drawing on 24 years of archival observations. Our results reveal that, while the general frequency locations of the identified modes are consistent throughout the years, the multiplet structure is complex and cannot be interpreted simply as l = 1 modes in the limit of slow rotation. The high-k multiplets exhibit significant variability in structure, amplitude and frequency. Any identification of the m components for the high-k multiplets is highly suspect. The k = 9 and 8 modes typically do show triplet structure more consistent with theoretical expectations. The frequencies and amplitudes exhibit some variability, but much less than the high-k modes. Analysis of the k = 9 and 8 multiplet splittings from 1990 to 2008 reveal a long-term change in multiplet splittings coinciding with the 1996 sforzando event, where GD358 dramatically altered its pulsation characteristics on a timescale of hours. We explore potential implications, including the possible connections between convection and/or magnetic fields and pulsations. We suggest future investigations, including theoretical investigations of the relationship between magnetic fields, pulsation, growth rates, and convection.
The Astrophysical Journal | 1998
M. S. O'Brien; G. Vauclair; S. D. Kawaler; T. K. Watson; D. E. Winget; R. E. Nather; M. H. Montgomery; A. Nitta; S. J. Kleinman; D. J. Sullivan; X. J. Jiang; T. M. K. Marar; S. Seetha; B. N. Ashoka; J. Bhattacharya; Elia M. Leibowitz; S. Hemar; P. Ibbetson; Brian Warner; L. van Zyl; P. Moskalik; S. Zola; G. Pajdosz; Jurek Krzesinski; N. Dolez; M. Chevreton; J.-E. Solheim; T. Thomassen; S. O. Kepler; O. Giovannini
Observation of g-mode pulsations in the variable pre-white dwarf (GW Virginis) stars provides a unique means to probe their interiors and to study the late stages of stellar evolution. Multisite campaigns have in several cases proved highly successful in decoding pre-white dwarf light curves. Three previous attempts to untangle the pulsation spectrum of the coolest GW Virginis star, PG 0122+200, confirmed the existence of multiple g-modes but left the fundamental period spacing and therefore the stars mass and luminosity in doubt. We present an analysis based on new observations of PG 0122+200 obtained during a Whole Earth Telescope (WET) campaign conducted in the fall of 1996. Although our coverage was, because of bad weather, far poorer than in previous WET campaigns, we confirm the previous result that PG 0122+200 rotates once in 1.6 ± 0.1 days. The most likely period spacing supported by the data implies a mass of 0.69±0.03 M☉. Based on the best seismology we can currently do, the cooling of PG 0122+200 is dominated by neutrino losses. This is not true for all pre-white dwarf stars and makes PG 0122+200 the prime candidate for learning useful physics. Constraints placed on the cooling rate of PG 0122+200 by future measurement of dΠ/dt could provide a unique test of the standard theory of lepton interactions in the (experimentally unexplored) region of phase-space appropriate to pre-white dwarf interiors.
The Astrophysical Journal | 2012
J. L. Provencal; M. H. Montgomery; A. Kanaan; Susan E. Thompson; J. Dalessio; Harry L. Shipman; D. Childers; J. C. Clemens; R. Rosen; P. Henrique; Agnes Bischoff-Kim; W. Strickland; D. Chandler; B. Walter; T. K. Watson; B. Castanheira; S. Wang; G. Handler; Matt A. Wood; Stephane Vennes; P. Nemeth; S. O. Kepler; M. D. Reed; Atsuko Nitta; S. J. Kleinman; Timothy M. Brown; S.-L. Kim; D. J. Sullivan; W. P. Chen; M. Yang
We report on an analysis of 308.3?hr of high-speed photometry targeting the pulsating DA white dwarf EC14012-1446. The data were acquired with the Whole Earth Telescope during the 2008 international observing run XCOV26. The Fourier transform of the light curve contains 19 independent frequencies and numerous combination frequencies. The dominant peaks are 1633.907, 1887.404, and 2504.897 ?Hz. Our analysis of the combination amplitudes reveals that the parent frequencies are consistent with modes of spherical degree l = 1. The combination amplitudes also provide m identifications for the largest amplitude parent frequencies. Our seismology analysis, which includes 2004-2007 archival data, confirms these identifications, provides constraints on additional frequencies, and finds an average period spacing of 41?s. Building on this foundation, we present nonlinear fits to high signal-to-noise light curves from the SOAR 4.1?m, McDonald 2.1?m, and KPNO 2?m telescopes. The fits indicate a time-averaged convective response timescale of ?0 = 99.4 ? 17?s, a temperature exponent N = 85 ? 6.2, and an inclination angle of ? i = 329 ? 32. We present our current empirical map of the convective response timescale across the DA instability strip.