Philip N. Appleton
California Institute of Technology
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Featured researches published by Philip N. Appleton.
The Astrophysical Journal | 2011
Ramin A. Skibba; C. W. Engelbracht; Daniel A. Dale; Joannah L. Hinz; Stefano Zibetti; Alison F. Crocker; Brent Groves; L. K. Hunt; Benjamin D. Johnson; Sharon E. Meidt; E. J. Murphy; Philip N. Appleton; Lee Armus; Alberto D. Bolatto; Bernhard R. Brandl; Daniela Calzetti; Kevin V. Croxall; M. Galametz; Karl D. Gordon; Robert C. Kennicutt; Jin Koda; O. Krause; Edward Montiel; Hans-Walter Rix; Helene Roussel; Karin Sandstrom; M. Sauvage; E. Schinnerer; J. D. Smith; Fabian Walter
Using new far-infrared imaging from the Herschel Space Observatory with ancillary data from ultraviolet (UV) to submillimeter wavelengths, we estimate the total emission from dust and stars of 62 nearby galaxies in the KINGFISH survey in a way that is as empirical and model independent as possible. We collect and exploit these data in order to measure from the spectral energy distributions (SEDs) precisely how much stellar radiation is intercepted and re-radiated by dust, and how this quantity varies with galaxy properties. By including SPIRE data, we are more sensitive to emission from cold dust grains than previous analyses at shorter wavelengths, allowing for more accurate estimates of dust temperatures and masses. The dust/stellar flux ratio, which we measure by integrating the SEDs, has a range of nearly three decades (from 10^(−2.2) to 10^(0.5)). The inclusion of SPIRE data shows that estimates based on data not reaching these far-IR wavelengths are biased low by 17% on average. We find that the dust/stellar flux ratio varies with morphology and total infrared (IR) luminosity, with dwarf galaxies having faint luminosities, spirals having relatively high dust/stellar ratios and IR luminosities, and some early types having low dust/stellar ratios. We also find that dust/stellar flux ratios are related to gas-phase metallicity (log(f_(dust)/f_∗) = −0.66 ± 0.08 and −0.22 ± 0.12 for metal-poor and intermediate-metallicity galaxies, respectively), while the dust/stellar mass ratios are less so (differing by ≈0.2 dex); the more metal-rich galaxies span a much wider range of the flux ratios. In addition, the substantial scatter between dust/stellar flux and dust/stellar mass indicates that the former is a poor proxy of the latter. Comparing the dust/stellar flux ratios and dust temperatures, we also show that early types tend to have slightly warmer temperatures (by up to 5 K) than spiral galaxies, which may be due to more intense interstellar radiation fields, or possibly to different dust grain compositions. Finally, we show that early types and early-type spirals have a strong correlation between the dust/stellar flux ratio and specific star formation rate, which suggests that the relatively bright far-IR emission of some of these galaxies is due to ongoing (if limited) star formation as well as to the radiation field from older stars, which is heating the dust grains.
The Astrophysical Journal | 2003
Yu Gao; Q. Daniel Wang; Philip N. Appleton; Ray A. Lucas
We report the Chandra/ACIS-S detection of more than 20 ultraluminous X-ray sources (ULXs, L0.5−10keV > �3 × 10 39 ergss −1 ) in the Cartwheel collisional ring galaxy system, of which over a dozen are located in the outer active star-forming ring. A remarkable hyperluminous X-ray source (HLX, L0.5−10keV > �10 41 ergss −1 assuming isotropic radiation), which dominates the X-ray emission from the Cartwheel ring, is located in the same segment of the ring as most ULXs. These powerful H/ULXs appear to be coincident with giant HII region complexes, young star clusters, and radio and midinfrared hot-spots: all strong indicators of recent massive star formation. The X-ray spectra show that H/ULXs have similar properties as those of the most luminous ULXs found in the nearest starbursts and galaxy mergers such as the Antennae galaxies and M82. The close association between the X-ray sources and the starbursting ring strongly suggests that the H/ULXs are intimately associated with the production and rapid evolution of short-lived massive stars. The observations represent the most extreme X-ray luminosities discovered to date associated with star-forming regions—rivaling the X-ray luminosities usually associated with active galactic nuclei. Subject headings: galaxies: individual (VV 784, Cartwheel, ESO 350 G 040) — galaxies: interactions — galaxies: active — galaxies: starburst — X-rays: galaxies
The Astrophysical Journal | 2012
Pierre Guillard; P. Ogle; B. Emonts; Philip N. Appleton; Raffaella Morganti; C. N. Tadhunter; Tom Oosterloo; Daniel A. Evans; A. S. Evans
Observations of ionized and neutral gas outflows in radio galaxies (RGs) suggest that active galactic nucleus (AGN) radio jet feedback has a galaxy-scale impact on the host interstellar medium, but it is still unclear how the molecular gas is affected. Thus, it is crucial to determine the physical conditions of the molecular gas in powerful RGs to understandhowradiosourcesmayregulatethestarformationintheirhostgalaxies.WepresentdeepSpitzerInfrared Spectrograph (IRS) high-resolution spectroscopy of eight nearby RGs that show fast Hi outflows. Strikingly, all of these Hi-outflow RGs have bright H2 mid-IR lines that cannot be accounted for by UV or X-ray heating. This strongly suggests that the radio jet, which drives the Hi outflow, is also responsible for the shock excitation of the warm H2 gas. In addition, the warm H2 gas does not share the kinematics of the ionized/neutral gas. The mid-IR-ionized gas lines (with FWHM up to 1250 km s −1 for [Neii]12.8 μm) are systematically broader than the H2 lines, which are resolved by the IRS in ≈60% of the detected lines (with FWHM up to 900 km s −1 ). In five sources, 3C 236, 3C 293, 3C 459, 4C 12.50, and PKS 1549-79, the [Neii]12.8 μm line, and to a lesser extent the [Neiii]15.5 μm and [Nev]14.3 μm lines, clearly exhibits blueshifted wings (up to −900 km s −1 with respect to the systemic velocity) that match well the kinematics of the outflowing Hi or ionized gas. The H2 lines do not show these broad wings, except tentative detections in 4C 12.50, 3C 459, and PKS 1549-79. This shows that, contrary to the Hi gas, the H2 gas is inefficiently coupled to the AGN jet-driven outflow of ionized gas. While the dissipation of a small fraction (<10%) of the jet kinetic power can explain the turbulent heating of the molecular gas, our data show that the bulk of the warm molecular gas is not expelled from these galaxies.
The Astronomical Journal | 2007
Beverly J. Smith; Curtis Struck; Mark Hancock; Philip N. Appleton; V. Charmandaris; William T. Reach
We present Spitzer mid-infrared images from a survey of three dozen pre-merger strongly interacting galaxy pairs selected from the Arp Atlas. The global mid-infrared colors of these galaxies and their tidal tails and bridges are similar to those of normal spiral galaxies, thus this optically selected sample of interacting galaxies does not have strongly enhanced normalized star formation rates in their disks or tidal features. Despite distortion and disturbance these systems continue to form stars at a normal rate on average. The morphology of these galaxies is generally smoother in the shorter wavelength IRAC bands than at 8
Proceedings of SPIE | 2004
James R. Houck; Thomas L. Roellig; Jeff Van Cleve; William J. Forrest; Terry L. Herter; C. R. Lawrence; Keith Matthews; Harold J. Reitsema; B. T. Soifer; Dan M. Watson; D. Weedman; Marty Huisjen; John R. Troeltzsch; D. J. Barry; J. Bernard-Salas; Craig Blacken; Bernhard R. Brandl; V. Charmandaris; D. Devost; G. E. Gull; Peter Hall; Charles P. Henderson; S. James U. Higdon; Bruce Pirger; Justin Schoenwald; Greg C. Sloan; Keven Isao Uchida; Philip N. Appleton; Lee Armus; M. J. Burgdorf
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The Astrophysical Journal | 2014
Katherine Alatalo; Mark D. Lacy; Lauranne Lanz; T. Bitsakis; Philip N. Appleton; Kristina Nyland; Sabrina L. Cales; Philip Chang; Timothy A. Davis; P. T. de Zeeuw; Carol J. Lonsdale; Sergio Martin; David S. Meier; P. Ogle
m, where dozens of clumps of star formation are detected.
The Astronomical Journal | 2007
Mark Hancock; Beverly J. Smith; Curtis Struck; Mark L. Giroux; Philip N. Appleton; V. Charmandaris; William T. Reach
The Infrared Spectrograph (IRS) is one of three science instruments on the Spitzer Space Telescope. The IRS comprises four separate spectrograph modules covering the wavelength range from 5.3 to 38 μm with spectral resolutions, R~90 and 650, and it was optimized to take full advantage of the very low background in the space environment. The IRS is performing at or better than the pre-launch predictions. An autonomous target acquisition capability enables the IRS to locate the mid-infrared centroid of a source, providing the information so that the spacecraft can accurately offset that centroid to a selected slit. This feature is particularly useful when taking spectra of sources with poorly known coordinates. An automated data reduction pipeline has been developed at the Spitzer Science Center.
The Astrophysical Journal | 2014
Katherine Alatalo; Sabrina L. Cales; Philip N. Appleton; Lisa J. Kewley; Mark D. Lacy; Ute Lisenfeld; Kristina Nyland; Jeffrey A. Rich
NGC1266 is a nearby lenticular galaxy that harbors a massive outflow of molecular gas powered by the mechanical energy of an active galactic nucleus (AGN). It has been speculated that such outflows hinder star formation (SF) in their host galaxies, providing a form of feedback to the process of galaxy formation. Previous studies, however, indicated that only jets from extremely rare, high power quasars or radio galaxies could impart significant feedback on their hosts. Here we present detailed observations of the gas and dust continuum of NGC1266 at millimeter wavelengths. Our observations show that molecular gas is being driven out of the nuclear region at
The Astrophysical Journal | 1998
M. A. Bransford; Philip N. Appleton; Charlene Anne Heisler; R. P. Norris; A. P. Marston
\dot{M}_{\rm out} \approx 110 M_\odot
The Astrophysical Journal | 2015
Lauranne Lanz; P. Ogle; Daniel A. Evans; Philip N. Appleton; Pierre Guillard; B. Emonts
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