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VLBI observations of two 43GHz SiO masers in R Cas

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Korea Astronomy and Space Science Institute. In collaboration with. R. Booth 1,2 and J. Conway 1. 1.Onsala Space Observatory, Sweden ... – PowerPoint PPT presentation

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Title: VLBI observations of two 43GHz SiO masers in R Cas


1
VLBI observations of two 43-GHz SiO masers in R
Cas
  • Jiyune Yi
  • Korea VLBI Network ( KVN ) group
  • Korea Astronomy and Space Science Institute
  • In collaboration with
  • R. Booth 1,2 and J. Conway 1
  • 1.Onsala Space Observatory, Sweden
  • 2. Hartebeesthoek Radio Astronomy Observatory



8th EVN Symposium 2006
2
Asymptotic Giant Branch
3
Stellar masers Evolved stars
  • SiO, H2O and OH masers form in the extended
    stellar atmosphere
  • circumstellar envelope of evolved star (AGB
    stars)

?High resolution studies of SiO masers ? unique
tool to study extended stellar
atmosphere of AGB stars
4
SiO maser in AGB star
adopted by J. Hron, original idea by T. Le Bertre
5
Scientific goalsVLBA observations of SiO masers
  • To find significant constraints on SiO maser
    modellings ? evidence of stellar phase dependence
  • To provide highly plausible inputs for new models
  • To extend our understanding on the physical and
    dynamical properties of CSEs ? positions of
    individual maser clumps measured down to
    sub-milliarcsecond accuracy
  • To put confidence in non-standard VLBI
    techniques, (both observations and calibrations)

6
Technical challenge
  • To track the delay across the 301 MHz frequency
    gap between the v1 and v2 transitions
  • ?Simultaneous observations of the two maser
    transitions required
  • To determine the relative position of the masers
  • in the two transitions
  • ?Imaging the two maser maps relative to each
    other using cross-phase referencing

7
4 epochs of VLBA observations R Cas
R Cas Light curve (courtesy,AAVSO)
8
Epoch I (F 0.25)
9
Epoch II (F 0.68)
10
Epoch III (F 0.95)
10 mas 1.07 AU
11
Epoch IV (F 0.23)
12

R Cas image at 671 nm (Weigelt et al. 1996)
13
R Cas photospheric size measured by optical/IR
  • Weigelt et al. 1996
  • 36 mas(700 nm), 49 mas(714)
  • Hofmann et al. 2000
  • 44 mas(671), 37 mas(700)
  • 49 mas(714), 30 mas(1045)
  • Mennesson et al. 2002
  • 24.78 mas (F 0.09) at 2.16 mm
  • 31.09 mas (F 0.17) at 3.79 mm
  • ?
  • 700 nm
  • R Cas
  • 714 nm
  • R Cas

Weigelt et al. 1996
14
Stellar photospheric size versus SiO maser shell
size of R Cas
  • Angular diameter lt 30 mas, at near IR continuum
  • Angular diameter gt 30 mas, at visible
  • ?
  • Comparison with 3.8 2.2 mm radii, R(3.8)
    R(2.2)
  • at F0.17 0.09, respectively
  • (obs. by Mennesson et al. 2002)

15
Summary R Cas
  • Instead of ring disruption at near maser minimum
    (Epoch II) both masers formed circular rings.
  • Both maser rings expanded and contracted
    depending on the stellar phase. At maser maximum,
    both masers showed many coincident masers.
  • Outward-extending flare-like structure of
    emission survived over 2 epochs ( 0.3 stellar
    phase) .
  • SiO maser shell diameters estimated around 1 2
    stellar diameter.
  • Asymmetry found at Epoch I , asymmetric ejection
    of material directed away from us ?
  • Models which are predominantly collisionally
    pumped are in good agreement with our results.
  • Missing flux (typically more than 50 ) density
    found,
  • estimated a lower limit of the structure,
    34 mas

16
TX Cam maps at 4 epochs (Jiyune Yi et al. 2005)
10 mas 3.8 AU
17
Analysis of MASER ring radius
18
Comparison with models
19
Comparison with models
  • Ring shape ?
  • Disruption of the ring structure at maser
    minimum
  • development of the ring afterwards
  • Ring radius ?
  • Expansion and contraction along the stellar
    cycle
  • Ratio of the ring radius, v2/v1 ?
  • 96 (III) vs 94 (M) 91 (IV) vs 92
    (M)
  • relatively smaller R at IV ? v2, contracting
    while
  • v1, constant
  • Ring thickness (2575 percentiles) , v1 vs v2
    ?
  • 15.6 vs 14.9 (III) 19.5 vs 18.6
    (IV) of the ring radius ?? twice thicker in the
    v1 ring (M)

20
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21
Constraint on SiO maser models
  • To excite the lowest vibrational state ,v1
  • Required temperature gt1800 K
  • Unable to have spatial coincidence of masers in
    various v-states by
  • radiative pumping

3600 K
22
Velocity field of the masers
Epoch III
V1
V2
23
Spoke-like features
Epoch IV
24
Radial Spokes
Rectangles ? spokes of gas flowing outward at
different angle Thick rect. ? the brightest
spokes which we observe
25
Models of SiO masers in M-Miras (Humphreys et
al. 2002 Gray Humphreys 2000)
86 GHz v1,J1-0 v2,J1-0
26
Comparison with other observations
27
43.1-GHz SiO maser NIR observations in S
Orionis ?SiO maser at 2 photospheric radii
(Boboltz Wittkowski 2005)
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