2002NewA....7....9H


Query : 2002NewA....7....9H

2002NewA....7....9H - New Astronomy, 7, 9-20 (2002/January-0)

Observations of Mira stars with the IOTA/FLUOR interferometer and comparison with Mira star models.

HOFMANN K.-H., BECKMANN U., BLOECKER T., COUDE DU FORESTO V., LACASSE M., MENNESSON B., MILLAN-GABET R., MOREL S., PERRIN G., PRAS B., RUILIER C., SCHERTL D., SCHOELLER M., SCHOLZ M., SHENAVRIN V., TRAUB W., WEIGELT G., WITTKOWSKI M. and YUDIN B.

Abstract (from CDS):

ABSTRACT: We present K'-band observations of five Mira stars with the IOTA interferometer. The interferograms were obtained with the FLUOR fiber optics beam combiner, which provides high-accuracy visibility measurements in spite of time-variable atmospheric conditions. For the M-type Miras X Oph, R Aql, RU Her, R Ser, and the C-type Mira V CrB we derived the uniform-disk diameters 11.7 mas, 10.9 mas, 8.4 mas, 8.1 mas, and 7.9 mas (±0.3 mas), respectively. Simultaneous photometric observations yielded the bolometric fluxes. The derived angular Rosseland radii and the bolometric fluxes allowed the determination of effective temperatures. For instance, the effective temperature of R Aql was determined to be 2970±110 K. A linear Rosseland radius for R Aql of 250+100-60R☉ was derived from the angular Rosseland radius of 5.5±0.2mas and the HIPPARCOS parallax of 4.73±1.19mas. The observations were compared with theoretical Mira star models of Bessel et al. [1996A&A...307..481B] and Hofmann et al. [1998A&A...339..846H]. The effective temperatures of the M-type Miras and the linear radius of R Aql indicate fundamental mode pulsation.

Abstract Copyright: ∼

Journal keyword(s): Instrumentation: interferometers - Stars: AGB and post-AGB - Stars: late-type - Stars: variables

Simbad objects: 16

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Number of rows : 16
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 V* FW Vir LP* 12 38 22.4057053224 +01 51 16.779667860 9.13 7.31 5.71 4.15 2.73 M3+IIICa0.5 74 0
2 * rho Boo PM* 14 31 49.7893292450 +30 22 17.171652275 6.33 4.89 3.59 2.67 2.02 K3-III 270 0
3 * bet Boo PM* 15 01 56.7623044453 +40 23 26.046853660 5.21 4.47 3.52 2.85 2.37 G8IIIaFe-0.5 267 0
4 * tau01 Ser * 15 25 47.3973646296 +15 25 40.930863888 8.78 6.83 5.17     M1III 90 0
5 V* V CrB C* 15 49 31.3121978280 +39 34 17.892629256     6.90 7.23   C6,2e_MS3 275 0
6 V* R Ser Mi* 15 50 41.7343255200 +15 08 01.089879792   8.49 7.10     M5-8e 237 0
7 * eps CrB PM* 15 57 35.2514020181 +26 52 40.366652765 6.650 5.360 4.130 3.27 2.64 K2IIIab 280 1
8 V* RU Her Mi* 16 10 14.5126789272 +25 04 14.306977524   13.82 12.24 7.56 4.15 M6-7e 224 0
9 * eta Her PM* 16 42 53.7649454572 +38 55 20.117710727 5.03 4.42 3.50 2.83 2.35 G7IIIFe-1 296 0
10 V* V642 Her LP* 17 33 42.7800367704 +14 50 29.753869452 9.66 8.08 6.48     M4III 42 0
11 * bet Oph PM* 17 43 28.3519097803 +04 34 02.293206489 5.150 3.930 2.750 1.96 1.38 K2IIICN0.5 490 0
12 V* X Oph Mi* 18 38 21.1323356928 +08 50 02.806199880 8.61 7.72 6.40     M0-8e+K2:III 288 0
13 V* R Aql OH* 19 06 22.2510922392 +08 13 48.012661776 8.06 7.69 6.09     M6.5-9e 579 2
14 * gam Aql * 19 46 15.5789542266 +10 36 47.731401477 5.93 4.23 2.72 1.65 0.87 K3II 450 0
15 * gam Sge PM* 19 58 45.4282303572 +19 29 31.726069716 6.97 5.04 3.47 2.27 1.35 M0-III 276 0
16 * 13 Sge LP* 20 00 03.3079177416 +17 30 59.428510704 8.75 7.00 5.35     M3/5III 66 0

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