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A Census of Large-scale (≥10 PC), Velocity-coherent, Dense Filaments in the Northern Galactic Plane: Automated Identification Using Minimum Spanning Tree

Ke Wang (王科) et al. 2016 ApJS 226 9

Large-scale gaseous filaments with lengths up to the order of 100 pc are on the upper end of the filamentary hierarchy of the Galactic interstellar medium (ISM). Their association with respect to the Galactic structure and their role in Galactic star formation are of great interest from both an observational and theoretical point of view. Previous “by-eye” searches, combined together, have started to uncover the Galactic distribution of large filaments, yet inherent bias and small sample size limit conclusive statistical results from being drawn. Here, we present (1) a new, automated method for identifying large-scale velocity-coherent dense filaments, and (2) the first statistics and the Galactic distribution of these filaments. We use a customized minimum spanning tree algorithm to identify filaments by connecting voxels in the position–position–velocity space, using the Bolocam Galactic Plane Survey spectroscopic catalog. In the range of $7\buildrel{\circ}\over{.} 5\leqslant l\leqslant 194^\circ $, we have identified 54 large-scale filaments and derived mass ( $\sim {10}^{3}\mbox{--}{10}^{5}$ ${M}_{\odot }$), length (10–276 pc), linear mass density (54–8625 ${M}_{\odot }$ pc −1), aspect ratio, linearity, velocity gradient, temperature, fragmentation, Galactic location, and orientation angle. The filaments concentrate along major spiral arms. They are widely distributed across the Galactic disk, with 50% located within ±20 pc from the Galactic mid-plane and 27% run in the center of spiral arms. An order of 1% of the molecular ISM is confined in large filaments. Massive star formation is more favorable in large filaments compared to elsewhere. This is the first comprehensive catalog of large filaments that can be useful for a quantitative comparison with spiral structures and numerical simulations.

The Metal Abundances across Cosmic Time (MACT) Survey. I. Optical Spectroscopy in the Subaru Deep Field

Chun Ly et al. 2016 ApJS 226 5

Deep rest-frame optical spectroscopy is critical for characterizing and understanding the physical conditions and properties of the ionized gas in galaxies. Here, we present a new spectroscopic survey called “Metal Abundances across Cosmic Time” or ${ \mathcal M }{ \mathcal A }{ \mathcal C }{ \mathcal T }$, which will obtain rest-frame optical spectra for ∼3000 emission-line galaxies. This paper describes the optical spectroscopy that has been conducted with MMT/Hectospec and Keck/DEIMOS for ≈1900 z = 0.1–1 emission-line galaxies selected from our narrowband and intermediate-band imaging in the Subaru Deep Field. In addition, we present a sample of 164 galaxies for which we have measured the weak [O iii] λ4363 line (66 with at least 3 σ detections and 98 with significant upper limits). This nebular emission line determines the gas-phase metallicity by measuring the electron temperature of the ionized gas. This paper presents the optical spectra, emission-line measurements, interstellar properties (e.g., metallicity, gas density), and stellar properties (e.g., star formation rates, stellar mass). Paper II of the ${ \mathcal M }{ \mathcal A }{ \mathcal C }{ \mathcal T }$ survey (Ly et al.) presents the first results on the stellar mass–gas metallicity relation at z ≲ 1 using the sample with [O iii] λ4363 measurements.

The Spitzer Infrared Spectrograph Survey of Protoplanetary Disks in Orion A. I. Disk Properties

K. H. Kim et al. 2016 ApJS 226 8

We present our investigation of 319 Class II objects in Orion A observed by Spitzer/IRS. We also present the follow-up observations of 120 of these Class II objects in Orion A from the Infrared Telescope Facility/SpeX. We measure continuum spectral indices, equivalent widths, and integrated fluxes that pertain to disk structure and dust composition from IRS spectra of Class II objects in Orion A. We estimate mass accretion rates using hydrogen recombination lines in the SpeX spectra of our targets. Utilizing these properties, we compare the distributions of the disk and dust properties of Orion A disks with those of Taurus disks with respect to position within Orion A (Orion Nebular Cluster [ONC] and L1641) and with the subgroups by the inferred radial structures, such as transitional disks (TDs) versus radially continuous full disks (FDs). Our main findings are as follows. (1) Inner disks evolve faster than the outer disks. (2) The mass accretion rates of TDs and those of radially continuous FDs are statistically significantly displaced from each other. The median mass accretion rate of radially continuous disks in the ONC and L1641 is not very different from that in Taurus. (3) Less grain processing has occurred in the disks in the ONC compared to those in Taurus, based on analysis of the shape index of the 10 μm silicate feature ( F 11.3/ F 9.8). (4) The 20–31 μm continuum spectral index tracks the projected distance from the most luminous Trapezium star, θ 1 Ori C. A possible explanation is UV ablation of the outer parts of disks.

197 Candidates and 104 Validated Planets in K2's First Five Fields

Ian J. M. Crossfield et al. 2016 ApJS 226 7

We present 197 planet candidates discovered using data from the first year of the NASA K2 mission (Campaigns 0–4), along with the results of an intensive program of photometric analyses, stellar spectroscopy, high-resolution imaging, and statistical validation. We distill these candidates into sets of 104 validated planets (57 in multi-planet systems), $30$ false positives, and 63 remaining candidates. Our validated systems span a range of properties, with median values of R P  =  $2.3\,{R}_{\oplus }$, P =  $8.6$ days, ${T}_{\mathrm{eff}}$ =  $5300$ K, and Kp =  $12.7$ mag. Stellar spectroscopy provides precise stellar and planetary parameters for most of these systems. We show that K2 has increased by 30% the number of small planets known to orbit moderately bright stars (1–4 R , Kp = 9–13 mag). Of particular interest are $76$ planets smaller than 2 R , $15$ orbiting stars brighter than Kp = 11.5 mag, 5 receiving Earth-like irradiation levels, and several multi-planet systems—including 4 planets orbiting the M dwarf K2–72 near mean-motion resonances. By quantifying the likelihood that each candidate is a planet we demonstrate that our candidate sample has an overall false positive rate of 15%–30%, with rates substantially lower for small candidates ( $\lt 2{R}_{\oplus }$) and larger for candidates with radii $\gt 8{R}_{\oplus }$ and/or with $P\lt 3\,{\rm{days}}$. Extrapolation of the current planetary yield suggests that K2 will discover between 500 and 1000 planets in its planned four-year mission, assuming sufficient follow-up resources are available. Efficient observing and analysis, together with an organized and coherent follow-up strategy, are essential for maximizing the efficacy of planet-validation efforts for K2, TESS, and future large-scale surveys.

Ultra-deep K S-band Imaging of the Hubble Frontier Fields

Gabriel B. Brammer et al. 2016 ApJS 226 6

We present an overview of the “KIFF” project, which provides ultra-deep K s -band imaging of all six of the Hubble Frontier Fields clusters, Abell 2744, MACS-0416, Abell S1063, Abell 370, MACS-0717, and MACS-1149. All of these fields have recently been observed with large allocations of Directors’ Discretionary Time with the Hubble and Spitzer telescopes, covering $0.4\lt \lambda \lt 1.6$ $\mu {\rm{m}}$ and 3.6–4.5 $\mu {\rm{m}}$, respectively. VLT/HAWK-I integrations of the first four fields reach 5 σ limiting depths of ${K}_{s}\sim 26.0$ (AB, point sources) and have excellent image quality (FWHM ∼ 0.″4). The MACS-0717 and MACS-1149 fields are observable from the northern hemisphere, and shorter Keck/MOSFIRE integrations on those fields reach limiting depths of K s  = 25.5 and 25.1, with a seeing FWHM of ∼ 0.″4 and $0\buildrel{\prime\prime}\over{.} 5$. In all cases the K s -band mosaics cover the primary cluster and parallel HST/ACS+WFC3 fields. The total area of the K s -band coverage is 490 arcmin 2. The K s -band at 2.2 $\mu {\rm{m}}$ crucially fills the gap between the reddest HST filter (1.6 $\mu {\rm{m}}$ $\sim \,H$ band) and the IRAC 3.6 $\mu {\rm{m}}$ passband. While reaching the full depths of the space-based imaging is not currently feasible from the ground, the deep K s -band images provide important constraints on both the redshifts and the stellar population properties of galaxies extending well below the characteristic stellar mass across most of the age of the universe, down to and including the redshifts of the targeted galaxy clusters ( $z\lesssim 0.5$). Reduced, aligned mosaics of all six survey fields are provided.