2,559 research outputs found
Episodic Post-Shock Dust Formation in the Colliding Winds of Eta Carinae
Eta Carinae shows broad peaks in near-infrared (IR) JHKL photometry, roughly
correlated with times of periastron passage in the eccentric binary system.
After correcting for secular changes attributed to reduced extinction from the
thinning Homunculus Nebula, these peaks have IR spectral energy distributions
(SEDs) consistent with emission from hot dust at 1400-1700 K. The excess SEDs
are clearly inconsistent, however, with the excess being entirely due to
free-free wind or photospheric emission. One must conclude, therefore, that the
broad near-IR peaks associated with Eta Carinae's 5.5 yr variability are due to
thermal emission from hot dust. I propose that this transient hot dust results
from episodic formation of grains within compressed post-shock zones of the
colliding winds, analogous to the episodic dust formation in Wolf-Rayet binary
systems like WR140 or the post-shock dust formation seen in some supernovae
like SN2006jc. This dust formation in Eta Carinae seems to occur preferentially
near and after periastron passage; near-IR excess emission then fades as the
new dust disperses and cools. With the high grain temperatures and Eta Car's
C-poor abundances, the grains are probably composed of corundum or similar
species that condense at high temperatures, rather than silicates or graphite.
Episodic dust formation in Eta Car's colliding winds significantly impacts our
understanding of the system, and several observable consequences are discussed.Comment: MNRAS accepted; 8 pages, 5 figs, 2 color fig
Three-dimensional forced-damped dynamical systems with rich dynamics : bifurcations, chaos and unbounded solutions
T.M. is supported by the Grant-in-Aid for JSPS Fellow No. 24·5312. H.O. is partially supported by JSPS KAKENHI 24244007.We consider certain autonomous three-dimensional dynamical systems that can arise in mechanical and fluid-dynamical contexts. Extending a previous study in Craik and Okamoto (2002), to include linear forcing and damping, we find that the four-leaf structure discovered in that paper, and unbounded orbits, persist, but may now be accompanied by three distinct period-doubling cascades to chaos, and by orbits that approach stable equilibrium points. This rich structure is investigated both analytically and numerically, distinguishing three main cases determined by the damping and forcing parameter values.PostprintPeer reviewe
In Hot Pursuit of the Hidden Companion of Eta Carinae: An X-ray Determination of the Wind Parameters
We present X-ray spectral fits to a recently obtained Chandra grating
spectrum of Eta Carinae, one of the most massive and powerful stars in the
Galaxy and which is strongly suspected to be a colliding wind binary system.
Hydrodynamic models of colliding winds are used to generate synthetic X-ray
spectra for a range of mass-loss rates and wind velocities. They are then
fitted against newly acquired Chandra grating data. We find that due to the low
velocity of the primary wind (~500 km/s), most of the observed X-ray emission
appears to arise from the shocked wind of the companion star. We use the
duration of the lightcurve minimum to fix the wind momentum ratio at 0.2. We
are then able to obtain a good fit to the data by varying the mass-loss rate of
the companion and the terminal velocity of its wind. We find that Mdot ~ 1e-5
Msol/yr and v ~ 3000 km/s. With observationally determined values of ~500-700
km/s for the velocity of the primary wind, our fit implies a primary mass-loss
rate of Mdot ~ 2.5e-4 Msol/yr. This value is smaller than commonly inferred,
although we note that a lower mass-loss rate can reduce some of the problems
noted by Hillier et al. (2001) when a value as high as 1e-3 Msol/yr is used.
The wind parameters of the companion are indicative of a massive star which may
or may not be evolved. The line strengths appear to show slightly sub-solar
abundances, although this needs further confirmation. Based on the
over-estimation of the X-ray line strengths in our model, and re-interpretation
of the HST/FOS results, it appears that the homunculus nebula was produced by
the primary star.Comment: 12 pages, 7 figures, accepted by A&
Prediction for the He I 10830A Absorption Wing in the Coming Event of Eta Carinae
We propose an explanation to the puzzling appearance of a wide blue
absorption wing in the He I 10830A P-Cygni profile of the massive binary star
Eta Carinae several months before periastron passage. Our basic assumption is
that the colliding winds region is responsible for the blue wing absorption. By
fitting observations, we find that the maximum outflow velocity of this
absorbing material is ~2300 km/s. We also assume that the secondary star is
toward the observer at periastron passage. With a toy-model we achieve two
significant results. (1) We show that the semimajor axis orientation we use can
account for the appearance and evolution of the wide blue wing under our basic
assumption. (2) We predict that the Doppler shift (the edge of the absorption
profile) will reach a maximum 0-3 weeks before periastron passage, and not
necessarily exactly at periastron passage or after periastron passage.Comment: 15 pages, 6 figures. Accepted for publication in MNRA
Modeling the RXTE light curve of Carinae from a 3-D SPH simulation of its binary wind collision
The very massive star system Carinae exhibits regular 5.54-year
(2024-day) period disruptive events in wavebands ranging from the radio to
X-ray. There is a growing consensus that these events likely stem from
periastron passage of an (as yet) unseen companion in a highly eccentric
() orbit. This paper presents three-dimensional (3-D)
Smoothed Particle Hydrodynamics (SPH) simulations of the orbital variation of
the binary wind-wind collision, and applies these to modeling the X-ray light
curve observed by the Rossi X-ray Timing Explorer (RXTE). By providing a global
3-D model of the phase variation of the density of the interacting winds, the
simulations allow computation of the associated variation in X-ray absorption,
presumed here to originate from near the apex of the wind-wind interaction
cone. We find that the observed RXTE light curve can be readily fit if the
observer's line of sight is within this cone along the general direction of
apastron. Specifically, the data are well fit by an assumed inclination for the orbit's polar axis, which is thus consistent with orbital
angular momentum being along the inferred polar axis of the Homunculus nebula.
The fits also constrain the position angle that an orbital-plane
projection makes with the apastron side of the semi-major axis, strongly
excluding positions along or to the retrograde side of the
axis, with the best fit position given by . Overall the
results demonstrate the utility of a fully 3-D dynamical model for constraining
the geometric and physical properties of this complex colliding-wind binary
system.Comment: 5 pages, 4 figures, accepted to MNRAS Letter
Determination of metal ion concentrations by SERS using 2,2’-bipyridyl complexes
Surface enhanced Raman scattering (SERS) can generate characteristic spectral “fingerprints” from metal complexes, thus providing the potential for the development of methods of analysis for the identification and quantitation of a range of metal ions in solution. The advantages include sensitivity and the use of one ligand for several metals without the need for a specific chromophore. Aqueous solutions of Fe(II), Ni(II), Zn(II), Cu(II), Cr(III) and Cd(II) in the presence of excess 2,2′-bipyridyl (bipy) were analysed using SERS. Specific marker bands enabled the identification of each metal ion and the limit of detection for each metal ion was estimated. Two of the ions, Zn(II) and Cu(II), could be detected below the World Health Organisation's (WHO) recommended limits for drinking water at levels of 0.22 and 0.6 mg L−1, respectively
Detection of potentially toxic metals by SERS using salen complexes
Surfaced enhanced Raman scattering (SERS) can discriminate between metal complexes due to the characteristic “spectral fingerprints” obtained. As a result, SERS has the potential to develop relatively simple and sensitive methods of detecting and quantifying a range of metal ions in solution. This could be beneficial for the environmental monitoring of potentially toxic metals (PTMs). Here, salen (C16H16N2O2) was used as a ligand to form complexes of Ni(II), Cu(II), Mn(II) and Co(II) in solution. The SERS spectra showed characteristic spectral differences specific to each metal complex, thus allowing the identification of each of these metal ions. This method allows a number of metal ions to be detected using the same ligand and an identical preparation procedure. The limit of detection (LOD) was determined for each metal ion, and it was found that Ni(II), Cu(II) and Mn(II) could be detected below the WHO’s recommended limits in drinking water at 1, 2 and 2 µg L-1, respectively. Co(II) was found to have an LOD of 20 µg L-1, however no limit has been set for this ion by the WHO as the concentration of Co(II) in drinking water is generally <1-2 μg L-1. A contaminated water sample was also analysed where Mn(II) was detected at a level of 800 µg L-1
Constraining the Absolute Orientation of Eta Carinae's Binary Orbit: A 3-D Dynamical Model for the Broad [Fe III] Emission
We present a three-dimensional (3-D) dynamical model for the broad [Fe III]
emission observed in Eta Carinae using the Hubble Space Telescope/Space
Telescope Imaging Spectrograph (HST/STIS). This model is based on full 3-D
Smoothed Particle Hydrodynamics (SPH) simulations of Eta Car's binary colliding
winds. Radiative transfer codes are used to generate synthetic spectro-images
of [Fe III] emission line structures at various observed orbital phases and
STIS slit position angles (PAs). Through a parameter study that varies the
orbital inclination i, the PA {\theta} that the orbital plane projection of the
line-of-sight makes with the apastron side of the semi-major axis, and the PA
on the sky of the orbital axis, we are able, for the first time, to tightly
constrain the absolute 3-D orientation of the binary orbit. To simultaneously
reproduce the blue-shifted emission arcs observed at orbital phase 0.976, STIS
slit PA = +38 degrees, and the temporal variations in emission seen at negative
slit PAs, the binary needs to have an i \approx 130 to 145 degrees, {\theta}
\approx -15 to +30 degrees, and an orbital axis projected on the sky at a PA
\approx 302 to 327 degrees east of north. This represents a system with an
orbital axis that is closely aligned with the inferred polar axis of the
Homunculus nebula, in 3-D. The companion star, Eta B, thus orbits clockwise on
the sky and is on the observer's side of the system at apastron. This
orientation has important implications for theories for the formation of the
Homunculus and helps lay the groundwork for orbital modeling to determine the
stellar masses.Comment: 23 pages, 12 color figures, plus 2 online-only appendices (available
in the /anc folder of the Source directory). Accepted for publication in
MNRA
Explaining the transient fast blue absorption lines in the massive binary system Eta Carinae
We use recent observations of the He I absorption line and
3D hydrodynamical numerical simulations of the winds collision, to strengthen
the case for an orientation of the semimajor axis of the massive binary system
Eta Carinae where the secondary star is toward us at periastron passage. Those
observations show that the fast blue absorption component exists for only
several weeks prior to the periastron passage. We show that the transient
nature of the fast blue absorption component supports a geometry where the fast
secondary wind, both pre and post-shock material, passes in front of the
primary star near periastron passage.Comment: 8 pages, 5 figures, accepted by MNRAS, includes astro-ph only
appendice
Accretion onto the Companion of Eta Carinae During the Spectroscopic Event. V. the Infrared Decline
We propose that the decline in the near-IR flux from the massive binary
system Eta Carinae during the spectroscopic event might be explained by
accreted mass that absorbs the radiation from the secondary star, and by that
reduces the heating of the dust that is responsible for the near-IR emission.
This binary system has an orbital period of 2024 days and eccentricity of
e~0.9. The emission in several bands declines for several weeks near every
periastron passages, in what is termed the spectroscopic event. In the
accretion model for the spectroscopic event the secondary star accretes mass
from the primary's wind for ~10 weeks near every periastron passage. The mass
is accreted mainly in the equatorial plane. The disk and its wind block the
secondary's radiation from heating dust that does not reside within narrow
cones along the symmetry axis. This, we propose, might explain the decline in
the near-IR flux occurring at the beginning of each spectroscopic event. We
also argue that the increase in the near-IR prior to the event might be
accounted for by enhanced hot (T~1700 K) dust formation in the collision region
of the winds from the two stars. This dust resides within ~60 degrees from the
equatorial plane, and most of it cannot be heated by the secondary during the
accretion phase.Comment: Accepted for publication by New Astronom
- …
