Circumstellar SiO masers in long period variable stars - PowerPoint PPT Presentation

1 / 13
About This Presentation
Title:

Circumstellar SiO masers in long period variable stars

Description:

In IRC 10011, R Leo y TX Cam, the spatial distribution of the v =1 J=1 0 and J=2 ... When detected, the line profile is composed of narrow peaks near or at the ... – PowerPoint PPT presentation

Number of Views:51
Avg rating:3.0/5.0
Slides: 14
Provided by: rebecaso
Category:

less

Transcript and Presenter's Notes

Title: Circumstellar SiO masers in long period variable stars


1
Circumstellar SiO masers in long period variable
stars
  • Rebeca Soria Ruiz
  • F. Colomer, J. Alcolea, V. Bujarrabal J.-F.
    Desmurs

OAN
2
Why SiO masers ?
Produced in the innermost regions of the
circumstellar envelopes around AGB stars
Ring-like structures at 2?4 R (Diamond et al
1994) composed of compact spots, with typical
sizes of a few mas, and high brightness
temperatures ? perfect targets for VLBI
Maser emission is shown in 28SiO, 29SiO and 30SiO
in many rotational transitions, which have been
extensively studied in single-dish
Multi-line simultaneous observations help in
constraining the current pumping mechanisms
3
Radiative or collisional?
Bujarrabal (1994)
Humphreys et al (2000 2002)
4
Observations
5
AGB sample
6
R Leo
7
TX Cam ( I )
28SiO v2 J1?0
28SiO v1 J1?0
8
TX Cam ( II )
28SiO v2 J2?1
28SiO v1 J2?1
28SiO v2 J1?0
28SiO v1 J1?0
9
Summary of results
Similar spatial distribution of the v 1 and v 2
J 1?0 28SiO maser emissions in the
O-rich stars. The v 2 emission is located in an
inner region, with a separation of ? 1?3 mas
In IRC10011, R Leo y TX Cam, the spatial
distribution of the v 1 J1?0 and J2?1 is
completely different, the latter being produced
in an outer region BUT in chi Cyg, an S-type
star, the sizes are comparable
10
Pumping models line overlaps
  • Proposed by Olofsson (1981 1985) to explain
    the quenching of the
  • 28SiO v 2 J 2?1 maser in O-rich stars
  • If Tex (H2O) Tb and the H2O line is
    optically thick, the v 2 J 1
  • rotational level is overpopulated
  • H2O ?2 0 127,5 ? ?2 1 116,6
    SiO v 1 J 0 ? v 2 J 1

The model (based on Bujarrabal et al 1996)
Excitation of both molecules under the Large
Velocity Gradient approximation H2O not
including the overlap SiO including the overlap
11
Line overlaps results
12
Summary
28SiO masers In O-rich envelopes
Similar spatial distribution of the 7mm emissions
with the v2 located in an inner region. The 3mm
is produced further away (not in S-type envelopes
where the 7 3mm regions have comparable
sizes). Current models dont explain the
observed results in O-rich stars. The line
overlaps strongly affect the excitation of SiO
and should be introduced in the pumping models.
29SiO masers First maps of the 29SiO v 0
J 1 0 maser transition in a circumstellar
envelope. When detected, the line profile is
composed of narrow peaks near or at the
stellar velocity, suggesting tangential
amplification as in the 28SiO maser lines.
13
Work in progress
  • 28SiO v1 and v2 J1?0 (_at_ 43 GHz) with the
    High Sensitivity Array
  • in the OH/IR variable IRC10011
  • Global VLBI observations of the 28SiO v1 and
    v2 J2?1 in O-rich
  • envelopes
  • Monitoring of the HCN (0, 20, 0) J1?0 maser
    in C-rich envelopes using
  • the Pico de Veleta (IRAM, Spain) 30m
    telescope
  • VLBA observations of HCN maser transitions in
    the variable CIT6
Write a Comment
User Comments (0)
About PowerShow.com