Sara Petty
Virginia Tech
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The Astrophysical Journal | 2012
Daniel Stern; Roberto J. Assef; Dominic J. Benford; A. W. Blain; Roc Michael Cutri; Arjun Dey; Peter R. M. Eisenhardt; Roger L. Griffith; T. H. Jarrett; Sean Lake; Frank J. Masci; Sara Petty; S. A. Stanford; Chao-Wei Tsai; E. L. Wright; Lin Yan; Fiona A. Harrison; Kristin K. Madsen
The Wide-field Infrared Survey Explorer (WISE) is an extremely capable and efficient black hole finder. We present a simple mid-infrared color criterion, W1-W2 \geq 0.8 (i.e., [3.4]-[4.6] \geq 0.8, Vega), which identifies 61.9 \pm 5.4 AGN candidates per deg2 to a depth of W2 = 15.0. This implies a much larger census of luminous AGN than found by typical wide-area surveys, attributable to the fact that mid-infrared selection identifies both unobscured (type 1) and obscured (type 2) AGN. Optical and soft X-ray surveys alone are highly biased towards only unobscured AGN, while this simple WISE selection likely identifies even heavily obscured, Compton-thick AGN. Using deep, public data in the COSMOS field, we explore the properties of WISE-selected AGN candidates. At the mid-infrared depth considered, 160 uJy at 4.6 microns, this simple criterion identifies 78% of Spitzer mid-infrared AGN candidates according to the criteria of Stern et al. (2005) and the reliability is 95%. We explore the demographics, multiwavelength properties and redshift distribution of WISE-selected AGN candidates in the COSMOS field.
Astrophysical Journal Supplement Series | 2011
J. Davy Kirkpatrick; Michael C. Cushing; Christopher R. Gelino; Roger L. Griffith; Michael F. Skrutskie; Kenneth A. Marsh; Edward L. Wright; A. Mainzer; Peter R. M. Eisenhardt; Ian S. McLean; Maggie A. Thompson; James Monie Bauer; Dominic J. Benford; C. Bridge; Sean Lake; Sara Petty; S. A. Stanford; Chao-Wei Tsai; Vanessa P. Bailey; Charles A. Beichman; Joshua S. Bloom; John J. Bochanski; Adam J. Burgasser; P. Capak; Kelle L. Cruz; Philip M. Hinz; J. Kartaltepe; Russell P. Knox; S. Manohar; Daniel Masters
We present ground-based spectroscopic verification of 6 Y dwarfs (see also Cushing et al.), 89 T dwarfs, 8 L dwarfs, and 1 M dwarf identified by the Wide-field Infrared Survey Explorer (WISE). Eighty of these are cold brown dwarfs with spectral types ≥T6, six of which have been announced earlier by Mainzer et al. and Burgasser et al. We present color-color and color-type diagrams showing the locus of M, L, T, and Y dwarfs in WISE color space. Near-infrared and, in a few cases, optical spectra are presented for these discoveries. Near-infrared classifications as late as early Y are presented and objects with peculiar spectra are discussed. Using these new discoveries, we are also able to extend the optical T dwarf classification scheme from T8 to T9. After deriving an absolute WISE 4.6 μm (W2) magnitude versus spectral type relation, we estimate spectrophotometric distances to our discoveries. We also use available astrometric measurements to provide preliminary trigonometric parallaxes to four of our discoveries, which have types of L9 pec (red), T8, T9, and Y0; all of these lie within 10 pc of the Sun. The Y0 dwarf, WISE 1541–2250, is the closest at 2.8^(+1.3)_(–0.6) pc; if this 2.8 pc value persists after continued monitoring, WISE 1541–2250 will become the seventh closest stellar system to the Sun. Another 10 objects, with types between T6 and >Y0, have spectrophotometric distance estimates also placing them within 10 pc. The closest of these, the T6 dwarf WISE 1506+7027, is believed to fall at a distance of ~4.9 pc. WISE multi-epoch positions supplemented with positional info primarily from the Spitzer/Infrared Array Camera allow us to calculate proper motions and tangential velocities for roughly one-half of the new discoveries. This work represents the first step by WISE to complete a full-sky, volume-limited census of late-T and Y dwarfs. Using early results from this census, we present preliminary, lower limits to the space density of these objects and discuss constraints on both the functional form of the mass function and the low-mass limit of star formation.
The Astrophysical Journal | 2013
D. Farrah; V. Lebouteiller; H. W. W. Spoon; J. Bernard-Salas; Chris Pearson; D. Rigopoulou; H. A. Smith; E. González-Alfonso; D. L. Clements; A. Efstathiou; D. Cormier; J. Afonso; Sara Petty; Kathryn Harris; P. D. Hurley; Colin Borys; A. Verma; A. Cooray; Valentina Salvatelli
We present Herschel observations of 6 fine-structure lines in 25 ultraluminous infrared galaxies at z < 0.27. The lines, [O III]52 μm, [N III]57 μm, [O I]63 μm, [N II]122 μm, [O I]145 μm, and [C II]158 μm, are mostly single Gaussians with widths <600 km s^(–1) and luminosities of 10^7-10^9 L_☉. There are deficits in the [O I]63/L_(IR), [N II]/L_(IR), [O I]145/L_(IR), and [C II]/L_(IR) ratios compared to lower luminosity systems. The majority of the line deficits are consistent with dustier H II regions, but part of the [C II] deficit may arise from an additional mechanism, plausibly charged dust grains. This is consistent with some of the [C II] originating from photodissociation regions or the interstellar medium (ISM). We derive relations between far-IR line luminosities and both the IR luminosity and star formation rate. We find that [N II] and both [O I] lines are good tracers of the IR luminosity and star formation rate. In contrast, [C II] is a poor tracer of the IR luminosity and star formation rate, and does not improve as a tracer of either quantity if the [C II] deficit is accounted for. The continuum luminosity densities also correlate with the IR luminosity and star formation rate. We derive ranges for the gas density and ultraviolet radiation intensity of 10^1 < n < 10^(2.5) and 10^(2.2) < G_0 < 10^(3.6), respectively. These ranges depend on optical type, the importance of star formation, and merger stage. We do not find relationships between far-IR line properties and several other parameters: active galactic nucleus (AGN) activity, merger stage, mid-IR excitation, and SMBH mass. We conclude that these far-IR lines arise from gas heated by starlight, and that they are not strongly influenced by AGN activity.
The Astrophysical Journal | 2012
D. Farrah; Tanya Urrutia; Mark Lacy; A. Efstathiou; J. Afonso; K. E. K. Coppin; Patrick B. Hall; Carol J. Lonsdale; T. H. Jarrett; C. Bridge; Colin Borys; Sara Petty
We present optical to far-infrared photometry of 31 reddened QSOs that show evidence for radiatively driven outflows originating from active galactic nuclei (AGNs) in their rest-frame UV spectra. We use these data to study the relationships between the AGN-driven outflows, and the AGN and starburst infrared luminosities. We find that FeLoBAL QSOs are invariably IR-luminous, with IR luminosities exceeding 10^(12) L_☉ in all cases. The AGN supplies 76% of the total IR emission, on average, but with a range from 20% to 100%. We find no evidence that the absolute luminosity of obscured star formation is affected by the AGN-driven outflows. Conversely, we find an anticorrelation between the strength of AGN-driven outflows, as measured from the range of outflow velocities over which absorption exceeds a minimal threshold, and the contribution from star formation to the total IR luminosity, with a much higher chance of seeing a starburst contribution in excess of 25% in systems with weak outflows than in systems with strong outflows. Moreover, we find no convincing evidence that this effect is driven by the IR luminosity of the AGN. We conclude that radiatively driven outflows from AGNs can have a dramatic, negative impact on luminous star formation in their host galaxies. We find that such outflows act to curtail star formation such that star formation contributes less than ~25% of the total IR luminosity. We also propose that the degree to which termination of star formation takes place is not deducible from the IR luminosity of the AGN.
The Astrophysical Journal | 2012
Jingwen Wu; Chao-Wei Tsai; Jack Sayers; Dominic J. Benford; C. Bridge; A. W. Blain; Peter R. M. Eisenhardt; Daniel Stern; Sara Petty; Roberto J. Assef; Shane Bussmann; Julia M. Comerford; Roc Michael Cutri; Neal J. Evans; Roger L. Griffith; T. H. Jarrett; Sean Lake; Carol J. Lonsdale; Jeonghee Rho; S. Adam Stanford; Benjamin J. Weiner; Edward L. Wright; Lin Yan
We have used the Caltech Submillimeter Observatory (CSO) to follow-up a sample of Wide-field Infrared Survey Explorer (WISE) selected, hyperluminous galaxies, the so-called W1W2-dropout galaxies. This is a rare (∼1000 all-sky) population of galaxies at high redshift (peaks at z = 2–3), which are faint or undetected by WISE at 3.4 and 4.6 μm, yet are clearly detected at 12 and 22 μm. The optical spectra of most of these galaxies show significant active galactic nucleus activity. We observed 14 high-redshift ( z> 1.7) W1W2-dropout galaxies with SHARC-II at 350–850 μm, with nine detections, and observed 18 with Bolocam at 1.1 mm, with five detections. Warm Spitzer follow-up of 25 targets at 3.6 and 4.5 μm, as well as optical spectra of 12 targets, are also presented in the paper. Combining WISE data with observations from warm Spitzer and CSO, we constructed their mid-IR to millimeter spectral energy distributions (SEDs). These SEDs have a consistent shape, showing significantly higher mid-IR to submillimeter ratios than other galaxy templates, suggesting a hotter dust temperature. We estimate their dust temperatures to be 60–120 K using a single-temperature model. Their infrared luminosities are well over 10 13 L� . These SEDs are not well fitted with existing galaxy templates, suggesting they are a new population with very high luminosity and hot dust. They are likely among the most luminous galaxies in the universe. We argue that they are extreme cases of luminous, hot dust-obscured galaxies (DOGs), possibly representing a short evolutionary phase during galaxy merging and evolution. A better understanding of their long-wavelength properties needs ALMA as well as Herschel data.
Monthly Notices of the Royal Astronomical Society | 2013
I. G. Roseboom; A. Lawrence; M. Elvis; Sara Petty; Yue Shen; Heng Hao
ABSTRACT We investigate the range of covering factors (determined from the ratio of IR toUV/opticalluminosity)seeninluminoustype1quasarsusingacombinationofdatafrom the WISE, UKIDSS and SDSS surveys. Accretion disk (UV/optical) and ob-scuringdust(IR)luminositiesaremeasuredviatheuseofasimplethreecomponentSEDmodel.WeusetheseestimatestoinvestigatethedistributionofcoveringfactorsanditsrelationshiptobothaccretionluminosityandIRSEDshape.Thedistributionofcoveringfactors (f C ) is observedto be log-normal,with a bias-correctedmeanof =−0.41andstandarddeviationofσ =0.2.ThefractionofIRluminos-ityemittedinthenear-IR(1–5µm)isfoundtobehigh(∼40percent),andstronglydependantoncoveringfactor.Key words: quasars:general,infrared:general 1 INTRODUCTIONThere is clear evidence that all powerful AGN are sur-rounded by a geometrically thick distribution of opticallythick material (Rowan-Robinson 1977; Lawrence & Elvis1982; Antonucci & Miller 1985; Edelson, Malkan & Rieke1987; Elvis et al. 1994; Richards et al. 2006). However de-spite nearly three decades of study the exact nature of theobscuring material has remained controversial. Recognisingthe difficulty in maintaining a smooth and geometricallythick rotating structure, Krolik & Begelman (1988) sug-gested that the material must be “clumpy” or filamentaryin nature, a view supported by both recent resolution VLTIobservations (Jaffe et al. 2004; Tristram et al. 2007) and thelack of strong 9.7µm silicate emission in the mid-IR (Rocheet al. 1991).This has motivated a large range of “clumpy” models,which assume a torus-shaped distribution of dust clouds sur-rounding the central AGN (Nenkova et al. 2002; H¨onig et al.2006; Nenkova et al. 2008, Schartmann et al. 2008; H¨oniget al. 2010; Stalevski et al. 2012). These models have beenfound to offer reasonable agreement with the observed prop-erties of large samples of AGN selected in a variety of ways(Alonso-Herrero et al. 2003; Ramos-Almeida et al. 2009; Moret al. 2009; Landt et al. 2010; Alonso-Herrero et al. 2011; Deoet al. 2011)
Monthly Notices of the Royal Astronomical Society | 2014
Suzy Jones; A. W. Blain; Daniel Stern; Roberto J. Assef; C. Bridge; Peter R. M. Eisenhardt; Sara Petty; Jingwen Wu; Chao-Wei Tsai; Roc Michael Cutri; Edward L. Wright; Lin Yan
We present SCUBA-2 (Submillimetre Common-User Bolometer Array) 850 μm submillimetre (submm) observations of the fields of 10 dusty, luminous galaxies at z ∼ 1.7–4.6, detected at 12 and/or 22 μm by the Wide-field Infrared Survey Explorer (WISE) all-sky survey, but faint or undetected at 3.4 and 4.6 μm; dubbed hot, dust-obscured galaxies (Hot DOGs). The six detected targets all have total infrared luminosities greater than 10^(13) L_⊙, with one greater than 10^(14) L_⊙. Their spectral energy distributions (SEDs) are very blue from mid-infrared to submm wavelengths and not well fitted by standard active galactic nuclei (AGN) SED templates, without adding extra dust extinction to fit the WISE 3.4 and 4.6 μm data. The SCUBA-2 850 μm observations confirm that the Hot DOGs have less cold and/or more warm dust emission than standard AGN templates, and limit an underlying extended spiral or ULIRG-type galaxy to contribute less than about 2 or 55 per cent of the typical total Hot DOG IR luminosity, respectively. The two most distant and luminous targets have similar observed submm to mid-infrared ratios to the rest, and thus appear to have even hotter SEDs. The number of serendipitous submm galaxies detected in the 1.5-arcmin-radius SCUBA-2 850 μm maps indicates there is a significant overdensity of serendipitous sources around Hot DOGs. These submm observations confirm that the WISE-selected ultraluminous galaxies have very blue mid-infrared to submm SEDs, suggesting that they contain very powerful AGN, and are apparently located in unusual arcmin-scale overdensities of very luminous dusty galaxies.
Monthly Notices of the Royal Astronomical Society | 2016
Kathryn Harris; D. Farrah; Bernhard Schulz; E. Hatziminaoglou; M. Viero; Nick Anderson; M. Béthermin; S. C. Chapman; D. L. Clements; A. Cooray; A. Efstathiou; Anne Feltre; P. D. Hurley; E. Ibar; Mark Lacy; S. J. Oliver; Mat Page; I. Perez-Fournon; Sara Petty; Lura K. Pitchford; D. Rigopoulou; Douglas Scott; M. Symeonidis; J. D. Vieira; Lingyu Wang
We investigate the relation between star formation rates (M_s) and AGN properties in optically selected type 1 quasars at 2 < z < 3 using data from Herschel and the SDSS. We find that M_s remains approximately constant with redshift, at 300 ± 100 M⊙ yr^(−1). Conversely, M_s increases with AGN luminosity, up to a maximum of ∼ 600 M⊙ yr^(−1), and with C IV FWHM. In context with previous results, this is consistent with a relation between M_s and black hole accretion rate (M_(bh)) existing in only parts of the z−M_s–M_(bh) plane, dependent on the free gas fraction, the trigger for activity, and the processes that may quench star formation. The relations between M_s and both AGN luminosity and C IV FWHM are consistent with star formation rates in quasars scaling with black hole mass, though we cannot rule out a separate relation with black hole accretion rate. Star formation rates are observed to decline with increasing C IV equivalent width. This decline can be partially explained via the Baldwin effect, but may have an additional contribution from one or more of three factors; M_i is not a linear tracer of L_(2500), the Baldwin effect changes form at high AGN luminosities, and high C IV EW values signpost a change in the relation between M_s and M_(bh). Finally, there is no strong relation between M_s and Eddington ratio, or the asymmetry of the C IV line. The former suggests that star formation rates do not scale with how efficiently the black hole is accreting, while the latter is consistent with C IV asymmetries arising from orientation effects.
The Astrophysical Journal | 2013
A. W. Blain; Roberto J. Assef; Daniel Stern; Chao-Wei Tsai; Peter R. M. Eisenhardt; C. Bridge; Dominic J. Benford; Thomas Harold Jarrett; Roc Michael Cutri; Sara Petty; Jingwen Wu; Edward L. Wright
We present WISE All-Sky mid-infrared (IR) survey detections of 55% (17/31) of the known QSOs at z > 6 from a range of surveys: the SDSS, the CFHT-LS, FIRST, Spitzer, and UKIDSS. The WISE catalog thus provides a substantial increase in the quantity of IR data available for these sources: 17 are detected in the WISE W1 (3.4 μm) band, 16 in W2 (4.6 μm), 3 in W3 (12 μm), and 0 in W4 (22 μm). This is particularly important with Spitzer in its warm-mission phase and no faint follow-up capability at wavelengths longward of 5 μm until the launch of James Webb Space Telescope (JWST). WISE thus provides a useful tool for understanding QSOs found in forthcoming large-area optical/IR sky surveys using PanSTARRS, SkyMapper, VISTA, DES, and LSST. The rest-UV properties of the WISE-detected and the WISE-non-detected samples differ: the detections have brighter i/z-band magnitudes and redder rest-UV colors. This suggests that a more aggressive hunt for very high redshift QSOs by combining WISE W1 and W2 data with red, observed optical colors could be effective at least for a subset of dusty candidate QSOs. Stacking the WISE images of the WISE-non-detected QSOs indicates that they are, on average, significantly fainter than the WISE-detected examples, and are thus not narrowly missing detection in the WISE catalog. The WISE catalog detection of three of our sample in the W3 band indicates that their mid-IR flux can be detected individually, although there is no stacked W3 detection of sources detected in W1 but not W3. Stacking analyses of WISE data for large active galactic nucleus samples will be a useful tool, and high-redshift QSOs of all types will be easy targets for JWST.
The Astronomical Journal | 2012
Sean Lake; Edward L. Wright; Sara Petty; Roberto J. Assef; T. H. Jarrett; S. A. Stanford; Daniel Stern; Chao-Wei Tsai
We report on the results of an optical spectroscopic survey at high Galactic latitude (|b| ≥ 30°) of a sample of WISE-selected targets, grouped by WISE W1 (λ_eff = 3.4 μm) flux, which we use to characterize the sources WISE detected. We observed 762 targets in 10 disjoint fields centered on ultraluminous infrared galaxy candidates using DEIMOS on Keck II. We find 0.30 ± 0.02 galaxies arcmin–2 with a median redshift of z = 0.33 ± 0.01 for the sample with W1 ≥ 120 μJy. The foreground stellar densities in our survey range from 0.23 ± 0.07 arcmin–2 to 1.1 ± 0.1 arcmin–2 for the same sample. We obtained spectra that produced science grade redshifts for ≥90% of our targets for sources with W1 flux ≥120 μJy that also had an i-band flux gsim 18 μJy. We used this for targeting very preliminary data reductions available to the team in 2010 August. Our results therefore present a conservative estimate of what is possible to achieve using WISEs Preliminary Data Release for the study of field galaxies.