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
,
we have identified 54 large-scale filaments and derived mass (
),
length (10–276 pc), linear mass density (54–8625
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.
,
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
survey (Ly et al.) presents the first results on the stellar
mass–gas metallicity relation at
z ≲ 1 using the sample with [O
false positives, and 63 remaining candidates. Our validated systems
span a range of properties, with median values of
R
P =
,
P =
days,
=
K, and
Kp =
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
planets smaller than 2
R
⊕,
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 (
)
and larger for candidates with radii
and/or with
.
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.
and 3.6–4.5
,
respectively.
VLT/HAWK-I integrations of the first four fields reach 5
σ limiting depths of
(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
.
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
crucially fills the gap between the reddest
HST filter (1.6
band) and the IRAC 3.6
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 (
).
Reduced, aligned mosaics of all six survey fields are provided.