R. A. Street
Las Cumbres Observatory Global Telescope Network
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The Astrophysical Journal | 2009
Misty C. Bentz; Jonelle L. Walsh; Aaron J. Barth; Nairn Reese Baliber; Vardha N. Bennert; Gabriela Canalizo; Alexei V. Filippenko; Mohan Ganeshalingam; Elinor L. Gates; Jenny E. Greene; Marton G. Hidas; Kyle D. Hiner; Nicholas Lee; Weidong Li; Matthew A. Malkan; Takeo Minezaki; Yu Sakata; Frank J. D. Serduke; Jeffrey M. Silverman; Thea N. Steele; Daniel Stern; R. A. Street; Carol E. Thornton; Tommaso Treu; Xiaofeng Wang; Jong-Hak Woo; Yuzuru Yoshii
We have recently completed a 64-night spectroscopic monitoring campaign at the Lick Observatory 3-m Shane telescope with the aim of measuring the masses of the black holes in 12 nearby (z < 0: 05) Seyfert 1 galaxies with expected masses in the range � 10 6 -10 7 Mand also the well-studied nearby active galactic nucleus (AGN) NGC 5548. Nine of the objects in the sample (including NGC 5548) showed optical variability of sufficient strength during the monitoring campaign to all ow for a time lag to be measured between the continuum fluctuations and the response to these fluctuation s in the broad Hemission. We present here the light curves for all the objects in this sample and the subseq uent Htime lags for the nine objects where these measurements were possible. The Hlag time is directly related to the size of the broad-line reg ion in AGNs, and by combining the Hlag time with the measured width of the Hemission line in the variable part of the spectrum, we determine the virial mass of the central sup ermassive black hole in these nine AGNs. The absolute calibration of the black hole masses is based on the normalization derived by Onken et al., which brings the masses determined by reverberation mapping into agreement with the local MBH -�? relationship for quiescent galaxies. We also examine the time lag response as a function of velocity across the Hline profile for six of the AGNs. The analysis of four leads to rather ambiguous results with relatively flat time lags as a function of velocity. However, SBS 1116+583A exhibits a symmetric time lag response around the line center reminiscent of simple models for circularly orbiting broad -line region (BLR) clouds, and Arp 151 shows an asymmetric profile that is most easily explained by a simple g ravitational infall model. Further investigation will be necessary to fully understand the constraints place d on physical models of the BLR by the velocity- resolved response in these objects. Subject headings:galaxies: active - galaxies: nuclei - galaxies: Seyfert
The Astrophysical Journal | 2010
Misty C. Bentz; Jonelle L. Walsh; Aaron J. Barth; Yuzuru Yoshii; Jong-Hak Woo; Xiaofeng Wang; Tommaso Treu; Carol E. Thornton; R. A. Street; Thea N. Steele; Jeffrey M. Silverman; Frank J. D. Serduke; Yu Sakata; Takeo Minezaki; Matthew A. Malkan; Weidong Li; Nicholas Lee; Kyle D. Hiner; Marton G. Hidas; Jenny E. Greene; Elinor L. Gates; Mohan Ganeshalingam; Alexei V. Filippenko; Gabriela Canalizo; Vardha N. Bennert; Nairn Reese Baliber
We have recently completed a 64-night spectroscopic monitoring campaign at the Lick Observatory 3 m Shane telescope with the aim of measuring the masses of the black holes in 12 nearby (z < 0.05) Seyfert 1 galaxies with expected masses in the range ~106-107 M ☉ and also the well-studied nearby active galactic nucleus (AGN) NGC 5548. Nine of the objects in the sample (including NGC 5548) showed optical variability of sufficient strength during the monitoring campaign to allow for a time lag to be measured between the continuum fluctuations and the response to these fluctuations in the broad Hβ emission, which we have previously reported. We present here the light curves for the Hα, Hγ, He II λ4686, and He I λ5876 emission lines and the time lags for the emission-line responses relative to changes in the continuum flux. Combining each emission-line time lag with the measured width of the line in the variable part of the spectrum, we determine a virial mass of the central supermassive black hole from several independent emission lines. We find that the masses are generally consistent within the uncertainties. The time-lag response as a function of velocity across the Balmer line profiles is examined for six of the AGNs. We find similar responses across all three Balmer lines for Arp 151, which shows a strongly asymmetric profile, and for SBS 1116+583A and NGC 6814, which show a symmetric response about zero velocity. For the other three AGNs, the data quality is somewhat lower and the velocity-resolved time-lag response is less clear. Finally, we compare several trends seen in the data set against the predictions from photoionization calculations as presented by Korista & Goad. We confirm several of their predictions, including an increase in responsivity and a decrease in the mean time lag as the excitation and ionization level for the species increases. Specifically, we find the time lags of the optical recombination lines to have weighted mean ratios of τ(Hα):τ(Hβ):τ(Hγ):τ(He I):τ(He II) = 1.54:1.00:0.61:0.36:0.25. Further confirmation of photoionization predictions for broad-line gas behavior will require additional monitoring programs for these AGNs while they are in different luminosity states.
Monthly Notices of the Royal Astronomical Society | 2008
D. R. Anderson; Michaël Gillon; C. Hellier; P. F. L. Maxted; F. Pepe; D. Queloz; D. M. Wilson; A. Collier Cameron; B. Smalley; T. A. Lister; S. J. Bentley; D. J. Christian; B. Enoch; L. Hebb; K. Horne; J. Irwin; Y. C. Joshi; S. R. Kane; M. Marmier; M. Mayor; N. Parley; Don Pollacco; F. Pont; R. Ryans; D. Segransan; I. Skillen; R. A. Street; S. Udry; Richard G. West; P. J. Wheatley
We report the discovery of WASP-5b, a Jupiter-mass planet orbiting a 12th-mag G-type star in the Southern hemisphere. The 1.6-d orbital period places WASP-5b in the class of very hot Jupiters and leads to a predicted equilibrium temperature of 1750 K. WASP-5b is the densest of any known Jovian-mass planet, being a factor of 7 denser than TrES-4, which is subject to similar stellar insolation, and a factor of 3 denser than WASP-4b, which has a similar orbital period. We present transit photometry and radial velocity measurements of WASP-5 (= USNO-B1 0487-0799749), from which we derive the mass, radius and density of the planet: M_P= 1.58^(+0.13)_(−0.08) M_J, R_P= 1.090^(+0.094)_(−0.058) R_J and ρ_P= 1.22^(+0.19)_(−0.24) ρ_J. The orbital period is P= 1.6284296^(+0.0000048)_(−0.0000037) d and the mid-transit epoch is T_C (HJD) = 245 4375.62466^(+0.00026)_(−0.00025).
The Astrophysical Journal | 2008
Misty C. Bentz; Jonelle L. Walsh; Aaron J. Barth; Nairn Reese Baliber; Nicola Bennert; Gabriela Canalizo; Alexei V. Filippenko; Mohan Ganeshalingam; Elinor L. Gates; Jenny E. Greene; Marton G. Hidas; Kyle D. Hiner; Nicholas Lee; Weidong Li; Matthew A. Malkan; Takeo Minezaki; Frank J. D. Serduke; Joshua H. Shiode; Jeffrey M. Silverman; Thea N. Steele; Daniel Stern; R. A. Street; Carol E. Thornton; Tommaso Treu; Xiaofeng Wang; Jong-Hak Woo; Yuzuru Yoshii
We have recently completed a 64 night spectroscopic monitoring campaign at the Lick Observatory 3 m Shane telescope with the aim of measuring the masses of the black holes in 13 nearby (z < 0.05) Seyfert 1 galaxies with expected masses in the range ~106-107 M☉. We present here the first results from this project—the mass of the central black hole in Arp 151. Strong variability throughout the campaign led to an exceptionally clean Hβ lag measurement in this object of 4.25−0.66+0.68 days in the observed frame. Coupled with the width of the Hβ emission line in the variable spectrum, we determine a black hole mass of (7.1 ± 1.2) × 106 M☉, assuming the Onken et al. normalization for reverberation-based virial masses. We also find velocity-resolved lag information within the Hβ emission line which clearly shows infalling gas in the Hβ-emitting region. Further detailed analysis may lead to a full model of the geometry and kinematics of broad line region gas around the central black hole in Arp 151.
Astrophysical Journal Supplement Series | 2009
Jonelle L. Walsh; Takeo Minezaki; Misty C. Bentz; Aaron J. Barth; Nairn Reese Baliber; Weidong Li; Daniel Stern; Vardha N. Bennert; Timothy M. Brown; Gabriela Canalizo; Alexei V. Filippenko; Elinor L. Gates; Jenny E. Greene; Matthew A. Malkan; Yu Sakata; R. A. Street; Tommaso Treu; Jong-Hak Woo; Yuzuru Yoshii
The Lick AGN Monitoring Project targeted 13 nearby Seyfert 1 galaxies with the intent of measuring the masses of their central black holes using reverberation mapping. The sample includes 12 galaxies selected to have black holes with masses roughly in the range 106-107 M ☉, as well as the well-studied active galactic nucleus (AGN) NGC 5548. In conjunction with a spectroscopic monitoring campaign, we obtained broadband B and V images on most nights from 2008 February through 2008 May. The imaging observations were carried out by four telescopes: the 0.76 m Katzman Automatic Imaging Telescope, the 2 m Multicolor Active Galactic Nuclei Monitoring telescope, the Palomar 60 inch (1.5 m) telescope, and the 0.80 m Tenagra II telescope. Having well-sampled light curves over the course of a few months is useful for obtaining the broad-line reverberation lag and black hole mass, and also allows us to examine the characteristics of the continuum variability. In this paper, we discuss the observational methods and the photometric measurements, and present the AGN continuum light curves. We measure various variability characteristics of each of the light curves. We do not detect any evidence for a time lag between the B- and V-band variations, and we do not find significant color variations for the AGNs in our sample.
Monthly Notices of the Royal Astronomical Society | 2010
M. G. Hidas; Y. Tsapras; D. Mislis; A. N. Ramaprakash; S. C. C. Barros; R. A. Street; J. H. M. M. Schmitt; Iain A. Steele; Don Pollacco; A. Ayiomamitis; J. Antoniadis; A. Nitsos; J. H. Seiradakis; S. Urakawa
We have used four telescopes at different longitudes to obtain near-continuous light-curve coverage of the star HD 80606 as it was transited by its ∼4-M Jup planet. The observations were performed during the predicted transit windows around 2008 October 25 and 2009 February 14. Our data set is unique in that it simultaneously constrains the duration of the transit and the planets period. Our Markov Chain Monte Carlo analysis of the light curves, combined with constraints from radial-velocity data, yields system parameters consistent with previously reported values. We find a planet-to-star radius ratio marginally smaller than previously reported, corresponding to a planet radius of R p = 0.921 ± 0.0367P Jup .
Monthly Notices of the Royal Astronomical Society | 2007
R. A. Street; D. J. Christian; W. I. Clarkson; A. Collier Cameron; B. Enoch; S. R. Kane; Tim Lister; Richard G. West; D. M. Wilson; A. Evans; A. Fitzsimmons; C. A. Haswell; C. Hellier; Simon T. Hodgkin; K. Horne; J. Irwin; F. P. Keenan; A. J. Norton; J. P. Osborne; Don Pollacco; R. Ryans; I. Skillen; P. J. Wheatley; J. R. Barnes
The definitive version is available at www.blackwell-synergy.com Copyright Blackwell Publishing DOI : 10.1111/j.1365-2966.2007.11987.x
Monthly Notices of the Royal Astronomical Society | 2008
P. L. Dufton; R. Ryans; H. M. A. Thompson; R. A. Street
High-resolution Hubble Space Telescope ultraviolet spectra for five B-type stars in the Magellanic Bridge and in the Large (LMC) and Small (SMC) Magellanic Clouds have been analysed to estimate their iron abundances. Those for the Clouds are lower than estimates obtained from late-type stars or the optical lines in B-type stars by approximately 0.5 dex. This may be due to systematic errors possibly arising from non-local thermodynamic equilibrium (non-LTE) effects or from errors in the atomic data, as similar low Fe abundances have previously been reported from the analysis of the ultraviolet spectra of Galactic early-type stars. The iron abundance estimates for all three Bridge targets appear to be significantly lower than those found for the SMC and LMC by approximately −0.5 and −0.8 dex, respectively, and these differential results should not be affected by any systematic errors present in the absolute abundance estimates. These differential iron abundance estimates are consistent with the underabundances for C, N, O, Mg and Si of approximately −1.1 dex relative to our Galaxy previously found in our Bridge targets. The implications of these very low metal abundances for the Magellanic Bridge are discussed in terms of metal deficient material being stripped from the SMC.
Monthly Notices of the Royal Astronomical Society | 2007
W. I. Clarkson; B. Enoch; C. A. Haswell; A. J. Norton; D. J. Christian; A. Collier Cameron; S. R. Kane; K. Horne; Tim Lister; R. A. Street; Richard G. West; D. M. Wilson; N. Evans; A. Fitzsimmons; C. Hellier; Simon T. Hodgkin; J. Irwin; F. P. Keenan; J. P. Osborne; N. Parley; Don Pollacco; R. Ryans; I. Skillen; P. J. Wheatley
The Wide Angle Search for Planets (WASP) photometrically surveys a large number of nearby stars to uncover candidate extrasolar planet systems by virtue of small-amplitude light curve dips on a less than or similar to 5-d time-scale typical of the Hot-Jupiters. Observations with the SuperWASP-North instrument between 2004 April and September produced a rich photometric data set of some 1.3 x 10(9) data points from 6.7 million stars. Our custom-built data acquisition and processing system produces similar to 0.02 mag photometric precision at V = 13. n nWe present the transit candidates in the 03(h)-06(h) RA range. Out of 141 895 light curves with sufficient sampling to provide adequate coverage, 2688 show statistically significant transit-like periodicities. Out of these, 44 pass a visual inspection of the light curve, of which 24 are removed through a set of cuts on the statistical significance of artefacts. All but four of the remaining 20 objects are removed when prior information at higher spatial resolution from existing catalogues is taken into account. Of the four candidates remaining, one is considered a good candidate for follow-up observations with three further second-priority targets. We provide detailed information on these candidates, as well as a selection of the false-positives and astrophysical false-alarms that were eliminated, and discuss briefly the impact of sampling on our results.