6,733 research outputs found
Nature of W51e2: Massive Cores at Different Phases of Star Formation
We present high-resolution continuum images of the W51e2 complex processed
from archival data of the Submillimeter Array (SMA) at 0.85 and 1.3 mm and the
Very Large Array (VLA) at 7 and 13 mm. We also made line images and profiles of
W51e2 for three hydrogen radio recombination lines (H26\alpha, H53\alpha, and
H66\alpha) and absorption of two molecular lines of HCN(4-3) and CO(2-1). At
least four distinct continuum components have been detected in the 3" region of
W51e2 from the SMA continuum images at 0.85 and 1.3 mm with resolutions of
0.3"x0.2" and 1.4"x0.7", respectively. The west component, W51e2-W, coincides
with the UC HII region reported from previous radio observations. The H26\alpha
line observation reveals an unresolved hyper-compact ionized core (<0.06" or
<310 AU) with a high electron temperature of 1.2x10^4 K, with corresponding
emission measure EM>7x10^{10} pc cm^{-6} and electron density N_e>7x10^6
cm^{-3}. The inferred Lyman continuum flux implies that the HII region W51e2-W
requires a newly formed massive star, an O8 star or a cluster of B-type stars,
to maintain the ionization. The east component, W51e2-E, has a total mass of
~140 M_{\sun} according to our SED analysis and a large infall rate of >
1.3x10^{-3} M_{\sun}yr^{-1} inferred from the absorption of HCN. W51e2-E
appears to be the accretion center in W51e2 and to host one or more growing
massive proto-stars. Located 2" northwest from W51e2-E, W51e2-NW is not
detected in the continuum emission at \lambda>=7 mm. Along with the maser
activities previously observed, our analysis suggests that W51e2-NW is at an
earlier phase of star formation. W51e2-N is located 2" north of W51e2-E and has
only been detected at 1.3 mm with a lower angular resolution (~1"), suggesting
that it is a primordial, massive gas clump in the W51e2 complex.Comment: 10 pages, 5 figures, 3 table, accepted for publication in Ap
The long-range interactions between branes in diverse dimensions
We calculate the long-range interactions between two simple branes placed
parallel at a separation in diverse dimensions via an effective field theory
approach. We also compute for the first time the explicit long-range
interaction between two D-branes with each carrying a world-volume non-abelian
magnetic flux in three special cases, respectively. In particular, we
demonstrate that the half-string creation between a D-brane and a
D-brane continues to hold even in the present context, therefore lending
further support to the previous assertion of this. Our computations re-raise
also the issue in one case on whether so constructed (D, D) bound state
is actually a marginal one.Comment: 28 pages, various discussions expanded and references adde
Quantitative characterization of short-range orthorhombic fluctuations in FeSe through pair distribution function analysis
Neutron and x-ray total scattering measurements have been performed on powder
samples of the iron chalcogenide superconductor FeSe. Using pair distribution
function (PDF) analysis of the total scattering data to investigate short-range
atomic correlations, we establish the existence of an instantaneous, local
orthorhombic structural distortion attributable to nematic fluctuations that
persists well into the high-temperature tetragonal phase, at least up to 300 K
and likely to significantly higher temperatures. This short-range orthorhombic
distortion is correlated over a length scale of about 1 nm at 300 K and grows
to several nm as the temperature is lowered toward the long-range structural
transition temperature. In the low-temperature nematic state, the local
instantaneous structure exhibits an enhanced orthorhombic distortion relative
to the average structure with a typical relaxation length of 3 nm. The
quantitative characterization of these orthorhombic fluctuations sheds light on
nematicity in this canonical iron-based superconductor
Neutron-Diffraction Measurements of an Antiferromagnetic Semiconducting Phase in the Vicinity of the High-Temperature Superconducting State of KFeSe
The recently discovered K-Fe-Se high temperature superconductor has caused
heated debate regarding the nature of its parent compound. Transport,
angle-resolved photoemission spectroscopy, and STM measurements have suggested
that its parent compound could be insulating, semiconducting or even metallic
[M. H. Fang, H.-D. Wang, C.-H. Dong, Z.-J. Li, C.-M. Feng, J. Chen, and H. Q.
Yuan, Europhys. Lett. 94, 27009 (2011); F. Chen et al. Phys. Rev. X 1, 021020
(2011); and W. Li et al.,Phys. Rev. Lett. 109, 057003 (2012)]. Because the
magnetic ground states associated with these different phases have not yet been
identified and the relationship between magnetism and superconductivity is not
fully understood, the real parent compound of this system remains elusive.
Here, we report neutron-diffraction experiments that reveal a semiconducting
antiferromagnetic (AFM) phase with rhombus iron vacancy order. The magnetic
order of the semiconducting phase is the same as the stripe AFM order of the
iron pnictide parent compounds. Moreover, while the root5*root5 block AFM phase
coexists with superconductivity, the stripe AFM order is suppressed by it. This
leads us to conjecture that the new semiconducting magnetic ordered phase is
the true parent phase of this superconductor.Comment: 1 table, 4 figures,5 page
Do Linear Dispersions of Classical Waves Mean Dirac Cones?
By using the \vec{k}\cdot\vec{p} method, we propose a first-principles theory
to study the linear dispersions in phononic and photonic crystals. The theory
reveals that only those linear dispersions created by doubly-degenerate states
can be described by a reduced Hamiltonian that can be mapped into the Dirac
Hamiltonian and possess a Berry phase of -\pi. Triply-degenerate states can
also generate Dirac-like cone dispersions, but the wavefunctions transform like
a spin-1 particle and the Berry phase is zero. Our theory is capable of
predicting accurately the linear slopes of Dirac/Dirac-like cones at various
symmetry points in a Brilliouin zone, independent of frequency and lattice
structure
SUSY-QCD Corrections to Associated Production at the CERN Large Hadron Collider
We calculate the SUSY-QCD corrections to the inclusive total cross sections
of the associated production processes in the Minimal
Supersymmetric Standard Model(MSSM) at the CERN Large Hadron Collider(LHC). The
SUSY-QCD corrections can increase and decrease the total cross sections
depending on the choice of the SUSY parameters. When the SUSY-QCD
corrections increase the leading-order (LO) total cross sections significantly
for large tan (), which can exceed 10% and have the opposite
sign with respect to the QCD and the SUSY-EW corrections, and thus cancel with
them to some extent. Moreover, we also investigate the effects of the SUSY-QCD
on the differential distribution of cross sections in transverse momentum
and rapidity Y of W-boson, and the invariant mass .Comment: 24 pages, 10 figures; minor changes in references; two figures and
the corresponding disccusions added; a version to appear in PR
Doping evoluton of antiferromagnetic order and structural distortion in LaFeAsOF
We use neutron scattering to study the structural distortion and
antiferromagnetic (AFM) order in LaFeAsOF as the system is doped
with fluorine (F) to induce superconductivity. In the undoped state, LaFeAsO
exhibits a structural distortion, changing the symmetry from tetragonal (space
group ) to orthorhombic (space group ) at 155 K, and then
followed by an AFM order at 137 K. Doping the system with F gradually decreases
the structural distortion temperature, but suppresses the long range AFM order
before the emergence of superconductivity. Therefore, while superconductivity
in these Fe oxypnictides can survive in either the tetragonal or the
orthorhombic crystal structure, it competes directly with static AFM order.Comment: reference update
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