Articles
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02/02/2006--
11/15/2005
Turbulent Gas Flows in the Rosette and G216-2.5 Molecular Clouds: Assessing Turbulent Fragmentation Descriptions of Star Formation
The role of turbulent fragmentation in regulating the efficiency of star
formation in interstellar clouds is examined from new wide field imaging of
12CO and 13CO J=1-0 emission from the Rosette and G216-2.5 molecular clouds.
The Rosette molecular cloud is a typical star forming giant molecular cloud and
G215-2.5 is a massive molecular cloud with no OB stars and very little low mass
star formation. The properties of the turbulent gas flow are derived from the
set of eigenvectors and eigenimages generated by Principal Component Analysis
of the spectroscopic data cubes. While the two clouds represent quite divergent
states of star formation activity, the velocity structure functions for both
clouds are similar. The sonic scale, lambda_S, defined as the spatial scale at
which turbulent velocity fluctuations are equivalent to the local sound speed,
and the turbulent Mach number evaluated at 1 pc, M_{1pc}, are derived for an
ensemble of clouds including the Rosette and, G216-2.5 regions that span a
large range in star formation activity. We find no evidence for the positive
correlations between these quantities and the star formation efficiency, that
are predicted by turbulent fragmentation models. A correlation does exist
between the star formation efficiency and the sonic scale for a subset of
clouds with L_{FIR}/M(H_2) > 1 that are generating young stellar clusters.
Turbulent fragmentation must play a limited and non-exclusive role in
determining the yield of stellar masses within interstellar clouds.
M. Heyer
J. Williams
C. Brunt
06/28/2016--
06/28/2016
Striations in the Taurus molecular cloud: Kelvin-Helmholtz instability or MHD waves?
The origin of striations aligned along the local magnetic field direction in
the translucent envelope of the Taurus molecular cloud is examined with new
observations of 12CO and 13CO J=2-1 emission obtained with the 10~m
submillimeter telescope of the Arizona Radio Observatory. These data identify a
periodic pattern of excess blue and redshifted emission that is responsible for
the striations. For both 12CO and 13CO, spatial variations of the J=2-1 to
J=1-0 line ratio are small and are not spatially correlated with the striation
locations. A medium comprised of unresolved CO emitting substructures (cells)
with a beam area filling factor less than unity at any velocity is required to
explain the average line ratios and brightness temperatures. We propose that
the striations result from the modulation of velocities and the beam filling
factor of the cells as a result of either the Kelvin-Helmholtz instability or
magnetosonic waves propagating through the envelope of the Taurus molecular
cloud. Both processes are likely common features in molecular clouds that are
sub-Alfvenic and may explain low column density, cirrus-like features similarly
aligned with the magnetic field observed throughout the interstellar medium in
far-infrared surveys of dust emission.
M. Heyer
P. F. Goldsmith
U. A. Yildiz
R. L. Snell
E. Falgarone
J. Pineda
09/26/2017--
09/26/2017
Early Science with the Large Millimetre Telescope: Fragmentation of molecular clumps in the Galaxy
Sensitive, imaging observations of the 1.1 mm dust continuum emission from a
1 deg^2 area collected with the AzTEC bolometer camera on the Large Millimeter
Telescope are presented. A catalog of 1545 compact sources is constructed based
on a Wiener-optimization filter. These sources are linked to larger clump
structures identified in the Bolocam Galactic Plane Survey. Hydrogen column
densities are calculated for all sources and mass and mean volume densities are
derived for the subset of sources for which kinematic distances can be
assigned. The AzTEC sources are localized, high density peaks within the
massive clumps of molecular clouds and comprise 5-15% of the clump mass. We
examine the role of the gravitational instability in generating these fragments
by comparing the mass of embedded AzTEC sources to the Jeans' mass of the
parent BGPS object. For sources with distances less than 6 kpc the fragment
masses are comparable to the clump Jeans' mass, despite having isothermal Mach
numbers between 1.6 and 7.2. AzTEC sources linked to ultra-compact HII regions
have mass surface densities greater than the critical value implied by the
mass-size relationship of infrared dark clouds with high mass star formation
while AzTEC sources associated with Class II methanol masers have mass surface
densities greater than 0.7 g cm^{-2} that approaches the proposed threshold
required to form massive stars.
M. Heyer
G. W. Wilson
R. Gutermuth
S. Lizano
A. Gomez-Ruiz
S. Kurtz
A. Luna
E. O. Serrano-Bernal
F. P. Schloerb
06/22/2020--
06/18/2020
The relative orientation between the magnetic field and gradients of surface brightness within thin velocity slices of 12CO and 13CO emission from the Taurus molecular cloud
We examine the role of the interstellar magnetic field to modulate the
orientation of turbulent flows within the Taurus molecular cloud using spatial
gradients of thin velocity slices of 12CO and 13CO antenna temperatures. Our
analysis accounts for the random errors of the gradients that arise from the
thermal noise of the spectra. The orientations of the vectors normal to the
antenna temperature gradient vectors are compared to the magnetic field
orientations that are calculated from Planck 353~GHz polarization data. These
relative orientations are parameterized with the projected Rayleigh statistic
and mean resultant vector. For 12CO, 28 percent and 39 percent of the cloud
area exhibit strongly parallel or strongly perpendicular relative orientations
respectively. For the lower opacity 13CO emission, strongly parallel and
strongly perpendicular orientations are found in 7 percent and 43 percent of
the cloud area respectively. For both isotopologues, strongly parallel or
perpendicular alignments are restricted to localized regions with low levels of
turbulence. If the relative orientations serve as an observational proxy to the
Alfvenic Mach number then our results imply local variations of the Alfvenic
Mach number throughout the cloud.
M. Heyer
J. D. Soler
B. Burkhart
08/14/2006--
08/14/2006
Analysis and geometry on marked configuration spaces
We carry out analysis and geometry on a marked configuration space
$\Omega^M_X$ over a Riemannian manifold $X$ with marks from a space $M$. We
suppose that $M$ is a homogeneous space $M$ of a Lie group $G$. As a
transformation group $\frak A$ on $\Omega_X^M$ we take the ``lifting'' to
$\Omega_X^M$ of the action on $X\times M$ of the semidirect product of the
group $\operatorname{Diff}_0(X)$ of diffeomorphisms on $X$ with compact support
and the group $G^X$ of smooth currents, i.e., all $C^\infty$ mappings of $X$
into $G$ which are equal to the identity element outside of a compact set. The
marked Poisson measure $\pi_\sigma$ on $\Omega_X^M$ with L\'evy measure
$\sigma$ on $X\times M$ is proven to be quasiinvariant under the action of
$\frak A$. Then, we derive a geometry on $\Omega_X^M$ by a natural ``lifting''
of the corresponding geometry on $X\times M$. In particular, we construct a
gradient $\nabla^\Omega$ and a divergence $\operatorname{div}^\Omega$. The
associated volume elements, i.e., all probability measures $\mu$ on
$\Omega_X^M$ with respect to which $\nabla^\Omega$ and
$\operatorname{div}^\Omega$ become dual operators on $L^2(\Omega_X^M;\mu)$, are
identified as the mixed marked Poisson measures with mean measure equal to a
multiple of $\sigma$. As a direct consequence of our results, we obtain marked
Poisson space representations of the group $\frak A$ and its Lie algebra $\frak
a$. We investigate also Dirichlet forms and Dirichlet operators connected with
(mixed) marked Poisson measures.
S. Albeverio
Yu. G. Kondratiev
E. W. Lytvynov
g. F. Us
12/11/2013--
12/11/2013
Formation of Molecular Clouds and Global Conditions for Star Formation
Giant molecular clouds (GMCs) are the primary reservoirs of cold,
star-forming molecular gas in the Milky Way and similar galaxies, and thus any
understanding of star formation must encompass a model for GMC formation,
evolution, and destruction. These models are necessarily constrained by
measurements of interstellar molecular and atomic gas, and the emergent,
newborn stars. Both observations and theory have undergone great advances in
recent years, the latter driven largely by improved numerical simulations, and
the former by the advent of large-scale surveys with new telescopes and
instruments. This chapter offers a thorough review of the current state of the
field.
Clare L. Dobbs
Mark R. Krumholz
Javier Ballesteros-Paredes
Alberto D. Bolatto
Yasuo Fukui
Mark Heyer
Mordecai-Mark Mac Low
Eve C. Ostriker
Enrique Vázquez-Semadeni
04/28/2009--
09/08/2008
Re-examining Larson's Scaling Relationships in Galactic Molecular Clouds
The properties of Galactic molecular clouds tabulated by Solomon etal (1987)
(SRBY) are re-examined using the Boston University-FCRAO Galactic Ring Survey
of 13CO J=1-0 emission. These new data provide a lower opacity tracer of
molecular clouds and improved angular and spectral resolution than previous
surveys of molecular line emission along the Galactic Plane. We calculate GMC
masses within the SRBY cloud boundaries assuming LTE conditions throughout the
cloud and a constant H2 to 13CO abundance, while accounting for the variation
of the 12C/13C with Galacto-centric radius. The LTE derived masses are
typically five times smaller than the SRBY virial masses. The corresponding
median mass surface density of molecular hydrogen for this sample is 42
Msun/pc^2, which is significantly lower than the value derived by SRBY (median
206 Msun/pc^2) that has been widely adopted by most models of cloud evolution
and star formation. This discrepancy arises from both the extrapolation by SRBY
of velocity dispersion, size, and CO luminosity to the 1K antenna temperature
isophote that likely overestimates the GMC masses and our assumption of
constant 13CO abundance over the projected area of each cloud. Owing to the
uncertainty of molecular abundances in the envelopes of clouds, the mass
surface density of giant molecular clouds could be larger than the values
derived from our 13CO measurements. From velocity dispersions derived from the
13CO data, we find that the coefficient of the cloud structure functions,
vo=sigma_v/R^{1/2}, is not constant, as required to satisfy Larson's scaling
relationships, but rather systematically varies with the surface density of the
cloud as Sigma^{0.5} as expected for clouds in self-gravitational equlibrium.
Mark Heyer
Coleman Krawczyk
Julia Duval
James M. Jackson
04/20/2022--
04/20/2022
The Dense Gas Mass Fraction and the Relationship to Star Formation in M51
Observations of 12CO J=1-0 and HCN J=1-0 emission from NGC 5194 (M51) made
with the 50~meter Large Millimeter Telescope and the SEQUOIA focal plane array
are presented. Using the HCN to CO ratio, we examine the dense gas mass
fraction over a range of environmental conditions within the galaxy. Within the
disk, the dense gas mass fraction varies along spiral arms but the average
value over all spiral arms is comparable to the mean value of interarm regions.
We suggest that the near constant dense gas mass fraction throughout the disk
arises from a population of density stratified, self gravitating molecular
clouds and the required density threshold to detect each spectral line. The
measured dense gas fraction significantly increases in the central bulge in
response to the effective pressure, P_e, from the weight from the stellar and
gas components. This pressure modifies the dynamical state of the molecular
cloud population and possibly, the HCN emitting regions, in the central bulge
from self-gravitating to diffuse configurations in which P_e is greater than
the gravitational energy density of individual clouds. Diffuse molecular clouds
comprise a significant fraction of the molecular gas mass in the central bulge,
which may account for the measured sublinear relationships between the surface
densities of the star formation rate and molecular and dense gas.
Mark Heyer
Benjamin Gregg
Daniela Calzetti
Bruce G. Elmegreen
Robert Kennicutt
Angela Adamo
Aaron S. Evans
Kathryn Grasha
James D. Lowenthal
Gopal Narayanan
Daniel Rosa-Gonzalez
F. P. Schloerb
Kamal Souccar
Yuping Tang
Peter Teuben
Olga Vega
William F. Wall
Min S. Yun
02/18/2008--
02/18/2008
The Five College Radio Astronomy Observatory CO Mapping Survey of the Taurus Molecular Cloud
The FCRAO Survey of the Taurus Molecular Cloud observed the 12CO and 13CO
J=1-0 emission from 98 square degrees of this important, nearby star forming
region. This set of data with 45" resolution comprises the highest spatial
dynamic range image of an individual molecular cloud constructed to date, and
provides valuable insights to the molecular gas distribution, kinematics, and
the star formation process. In this contribution, we describe the observations,
calibration, data processing, and characteristics of the noise and line
emission of the survey. The angular distribution of 12CO and 13CO emission over
1 km/s velocity intervals and the full velocity extent of the cloud are
presented. These reveal a complex, dynamic medium of cold, molecular gas.
Gopal Narayanan
Mark H. Heyer
Christopher Brunt
Paul F. Goldsmith
Ronald Snell
Di Li
11/20/2008--
11/20/2008
Spectra of Nearby Galaxies Measured with a New Very Broadband Receiver
Three-millimeter-wavelength spectra of a number of nearby galaxies have been
obtained at the Five College Radio Astronomy Observatory (FCRAO) using a new,
very broadband receiver. This instrument, which we call the Redshift Search
Receiver, has an instantaneous bandwidth of 36 GHz and operates from 74 to
110.5 GHz. The receiver has been built at UMass/FCRAO to be part of the initial
instrumentation for the Large Millimeter Telescope (LMT) and is intended
primarily for determination of the redshift of distant, dust-obscured galaxies.
It is being tested on the FCRAO 14m by measuring the 3mm spectra of a number of
nearby galaxies. There are interesting differences in the chemistry of these
galaxies.
Gopal Narayanan
Ronald L. Snell
Neal R. Erickson
Aeree Chung
Mark H. Heyer
Min Yun
William M. Irvine
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