6,985 research outputs found
Faint Submillimeter Galaxies Revealed by Multifield Deep ALMA Observations: Number Counts, Spatial Clustering, and A Dark Submillimeter Line Emitter
We present the statistics of faint submillimeter/millimeter galaxies (SMGs)
and serendipitous detections of a submillimeter/millimeter line emitter (SLE)
with no multi-wavelength continuum counterpart revealed by the deep ALMA
observations. We identify faint SMGs with flux densities of 0.1-1.0 mJy in the
deep Band 6 and Band 7 maps of 10 independent fields that reduce cosmic
variance effects. The differential number counts at 1.2 mm are found to
increase with decreasing flux density down to 0.1 mJy. Our number counts
indicate that the faint (0.1-1.0 mJy, or SFR_IR ~ 30-300 Msun/yr) SMGs
contribute nearly a half of the extragalactic background light (EBL), while the
remaining half of the EBL is mostly contributed by very faint sources with flux
densities of <0.1 mJy (SFR_IR <~ 30 Msun/yr). We conduct counts-in-cells
analysis with the multifield ALMA data for the faint SMGs, and obtain a coarse
estimate of galaxy bias, b_g <4. The galaxy bias suggests that the dark halo
masses of the faint SMGs are <~ 7x10^12 Msun, which is smaller than those of
bright (>1 mJy) SMGs, but consistent with abundant high-z star-forming
populations such as sBzKs, LBGs, and LAEs. Finally, we report the serendipitous
detection of SLE-1 with continuum counterparts neither in our 1.2 mm-band nor
multi-wavelength images including ultra deep HST/WFC3 and Spitzer data. The SLE
has a significant line at 249.9 GHz with a signal-to-noise ratio of 7.1. If the
SLE is not a spurious source made by unknown systematic noise of ALMA, the
strong upper limits of our multi-wavelength data suggest that the SLE would be
a faint galaxy at z >~ 6.Comment: 20 pages, 16 figures, accepted for publication in Ap
Anapole moment of a chiral molecule revisited
Parity violation in a chiral, four-atom molecule is discussed. Given the
geometrical positions of the four atoms, we calculate the anapole moment of it.
This problem was first discussed by Khriplovich and Pospelov. We give a
detailed derivation for it so that it can be more accessible to wider range of
scientists. We correct errors in their results and generalize their initial
state to |s_{1/2}\rangle and |p_{1/2}\rangle states. We also discuss realistic
candidates of the chiral molecules to which this approach can be applied.Comment: 21 pages, 2 figures. v2: Appendix added, references added, typos
corrected, version to appear in Eur. Phys. J.
Mass Estimates of a Giant Planet in a Protoplanetary Disk from the Gap Structures
A giant planet embedded in a protoplanetary disk forms a gap. An analytic
relationship among the gap depth, planet mass , disk aspect ratio ,
and viscosity has been found recently, and the gap depth can be
written in terms of a single parameter . We discuss how observed gap features can be used to constrain the
disk and/or planet parameters based on the analytic formula for the gap depth.
The constraint on the disk aspect ratio is critical in determining the planet
mass so the combination of the observations of the temperature and the image
can provide a constraint on the planet mass. We apply the formula for the gap
depth to observations of HL~Tau and HD~169142. In the case of HL~Tau, we
propose that a planet with is responsible for the observed gap at
~AU from the central star based on the estimate that the gap depth is
. In the case of HD~169142, the planet mass that causes the gap
structure recently found by VLA is . We also argue that the
spiral structure, if observed, can be used to estimate the lower limit of the
disk aspect ratio and the planet mass.Comment: 16 pages, 5 figures, accepted for publication in The Astrophysical
Journal Letter
High Angular Resolution, Sensitive CS J=2-1 and J=3-2 Imaging of the Protostar L1551 NE: Evidence for Outflow-Triggered Star Formation ?
High angular resolution and sensitive aperture synthesis observations of CS
() and CS () emissions toward L1551 NE, the second brightest
protostar in the Taurus Molecular Cloud, made with the Nobeyama Millimeter
Array are presented. L1551 NE is categorized as a class 0 object deeply
embedded in the red-shifted outflow lobe of L1551 IRS 5. Previous studies of
the L1551 NE region in CS emission revealed the presence of shell-like
components open toward L1551 IRS 5, which seem to trace low-velocity shocks in
the swept-up shell driven by the outflow from L1551 IRS 5. In this study,
significant CS emission around L1551 NE was detected at the eastern tip of the
swept-up shell from = 5.3 km s to 10.1 km s, and
the total mass of the dense gas is estimated to be 0.18 0.02 .
Additionally, the following new structures were successfully revealed: a
compact disklike component with a size of 1000 AU just at L1551 NE,
an arc-shaped structure around L1551 NE, open toward L1551 NE, with a size of
AU, i.e., a bow shock, and a distinct velocity gradient of the
dense gas, i.e., deceleration along the outflow axis of L1551 IRS 5. These
features suggest that the CS emission traces the post-shocked region where the
dense gas associated with L1551 NE and the swept-up shell of the outflow from
L1551 IRS 5 interact. Since the age of L1551 NE is comparable to the timescale
of the interaction, it is plausible that the formation of L1551 NE was induced
by the outflow impact. The compact structure of L1551 NE with a tiny envelope
was also revealed, suggesting that the outer envelope of L1551 NE has been
blown off by the outflow from L1551 IRS 5.Comment: 29 pages, 12 figures, Accepted for Publication in the Astrophysical
Journa
Excitation and emission spectra of rubidium in rare-gas thin-films
To understand the optical properties of atoms in solid state matrices, the
absorption, excitation and emission spectra of rubidium doped thin-films of
argon, krypton and xenon were investigated in detail. A two-dimensional
spectral analysis extends earlier reports on the excitation and emission
properties of rubidium in rare-gas hosts. We found that the doped crystals of
krypton and xenon exhibit a simple absorption-emission relation, whereas
rubidium in argon showed more complicated spectral structures. Our sample
preparation employed in the present work yielded different results for the Ar
crystal, but our peak positions were consistent with the prediction based on
the linear extrapolation of Xe and Kr data. We also observed a bleaching
behavior in rubidium excitation spectra, which suggests a population transfer
from one to another spectral feature due to hole-burning. The observed optical
response implies that rubidium in rare-gas thin-films is detectable with
extremely high sensitivity, possibly down to a single atom level, in low
concentration samples.Comment: 7 pages, 5 figure
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