Detection of 21-CENTIMETER Hydrogen Absorption in the High-Velocity Component of the Radio Galaxy Perseus a

1973 ◽  
Vol 185 ◽  
pp. 809 ◽  
Author(s):  
David S. de Young ◽  
Morton S. Roberts ◽  
William C. Saslaw
2007 ◽  
Vol 3 (S243) ◽  
pp. 171-182 ◽  
Author(s):  
Suzan Edwards

AbstractThe role of the star-disk interaction region in launching the high velocity component of accretion-driven outflows is examined. Spectroscopic indicators of high velocity inner winds have been recognized in T Tauri stars for decades, but identifying the wind launch site and the accompanying mass loss rates has remained elusive. A promising new diagnostic is He I λ10830, whose metastable lower level results in a powerful probe of the geometry of the outflowing gas in the interaction region. This, together with other atomic and molecular spectral diagnostics covering a wide range of excitation and ionization states, suggests that more than one launch site of the innermost wind is operational in most accreting stars.


1978 ◽  
Vol 225 ◽  
pp. 343
Author(s):  
A. D. Haschick ◽  
W. A. Baan ◽  
B. F. Burke

1981 ◽  
Vol 243 ◽  
pp. L143 ◽  
Author(s):  
W. A. Baan ◽  
A. D. Haschick

1978 ◽  
Vol 219 ◽  
pp. 400 ◽  
Author(s):  
E. M. Burbidge ◽  
G. R. Burbidge ◽  
H. E. Smith
Keyword(s):  

2018 ◽  
Vol 609 ◽  
pp. A87 ◽  
Author(s):  
B. Nisini ◽  
S. Antoniucci ◽  
J. M. Alcalá ◽  
T. Giannini ◽  
C. F. Manara ◽  
...  

Mass loss from jets and winds is a key ingredient in the evolution of accretion discs in young stars. While slow winds have been recently extensively studied in T Tauri stars, little investigation has been devoted on the occurrence of high velocity jets and on how the two mass-loss phenomena are connected with each other, and with the disc mass accretion rates. In this framework, we have analysed the [O i]6300 Å  line in a sample of 131 young stars with discs in the Lupus, Chamaeleon and σ Orionis star forming regions. The stars were observed with the X-shooter spectrograph at the Very Large Telescope and have mass accretion rates spanning from 10-12 to 10-7M⊙ yr-1. The line profile was deconvolved into a low velocity component (LVC, | Vr | < 40 km s-1) and a high velocity component (HVC, | Vr | > 40 km s-1), originating from slow winds and high velocity jets, respectively. The LVC is by far the most frequent component, with a detection rate of 77%, while only 30% of sources have a HVC. The fraction of HVC detections slightly increases (i.e. 39%) in the sub-sample of stronger accretors (i.e. with log (Lacc/L⊙) >−3). The [O i]6300 Å  luminosity of both the LVC and HVC, when detected, correlates with stellar and accretion parameters of the central sources (i.e. L∗, M∗, Lacc, Ṁacc), with similar slopes for the two components. The line luminosity correlates better (i.e. has a lower dispersion) with the accretion luminosity than with the stellar luminosity or stellar mass. We suggest that accretion is the main drivers for the line excitation and that MHD disc-winds are at the origin of both components. In the sub-sample of Lupus sources observed with ALMA a relationship is found between the HVC peak velocity and the outer disc inclination angle, as expected if the HVC traces jets ejected perpendicularly to the disc plane. Mass ejection rates (Ṁjet) measured from the detected HVC [O i]6300 Å  line luminosity span from ~10-13 to ~10-7M⊙ yr-1. The corresponding Ṁjet/Ṁacc  ratio ranges from ~0.01 to ~0.5, with an average value of 0.07. However, considering the upper limits on the HVC, we infer a Ṁjet/Ṁacc  ratio < 0.03 in more than 40% of sources. We argue that most of these sources might lack the physical conditions needed for an efficient magneto-centrifugal acceleration in the star-disc interaction region. Systematic observations of populations of younger stars, that is, class 0/I, are needed to explore how the frequency and role of jets evolve during the pre-main sequence phase. This will be possible in the near future thanks to space facilities such as the James Webb space telescope (JWST).


1986 ◽  
Vol 6 (4) ◽  
pp. 436-439
Author(s):  
D. I. Olsson-Steel ◽  
W. G. Elford

AbstractVisual meteors, due to impinging meteoroids of radius about 1 cm, appear at a rate of a few per hour during non-shower periods. Smaller meteoroids (100 μm – 1 cm) give rise to less bright trails, but are much more abundant. These are usually detected by radars of about 10 m wavelength which, over the past 40 years, have produced a plethora of information concerning mass and height distributions, orbits, etc.Using such ‘conventional radars’, the peak of the measured height distribution is found at about 95 km, with few meteors detected above 105 km. However, the flux detected is only a few percent of the total flux (a) measured using a large (10 m) optical collector, and (b) expected from a comparison with measurements by satellite impacts and zodiacal light observations (radii < 100 μm). One possibility is that the radars detect few low-velocity (V < ~25 km s-1) meteors since these produce little ionization and thus limit their detectability: the ionizing efficiency of meteors varies as ~ V7/2. In direct opposition, our alternative hypothesis is that the undetected flux is held in a faint high-velocity component which ablates at high altitude. These are not detected by conventional radars because meteor trails have ‘initial widths’ of about 3 m at 105 km; for a radar wavelength of 10 m, components scattered from different regions of the trail therefore destructively interfere, and the probability of detecting any meteor above 105 km is small.In order to test our hypothesis we have measured the height distribution with a 150 m radar, and we are commencing ancillary observations at 50 m; compared to these wavelengths the initial width is small to at least 140 km. The results show a peak at 105 km with most meteors being above this, significant numbers occurring right up to 140 km. This suggests that the true flux is at least 10 or 20 times that previously deduced, having implications for the number of cornets in the recent past and the balance of material between the smaller bodies in the solar System.


1978 ◽  
Vol 221 ◽  
pp. L95 ◽  
Author(s):  
H. E. Payne ◽  
J. M. Dickey ◽  
E. E. Salpeter ◽  
Y. Terzian

2016 ◽  
Vol 457 (3) ◽  
pp. 2951-2957 ◽  
Author(s):  
Ken Pounds ◽  
Andrew Lobban ◽  
James Reeves ◽  
Simon Vaughan

2018 ◽  
Vol 480 (2) ◽  
pp. 2365-2376 ◽  
Author(s):  
M L Parker ◽  
G A Matzeu ◽  
M Guainazzi ◽  
E Kalfountzou ◽  
G Miniutti ◽  
...  

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