2013A&A...550A.126M


Query : 2013A&A...550A.126M

2013A&A...550A.126M - Astronomy and Astrophysics, volume 550A, 126-126 (2013/2-1)

Asymptotic and measured large frequency separations.

MOSSER B., MICHEL E., BELKACEM K., GOUPIL M.J., BAGLIN A., BARBAN C., PROVOST J., SAMADI R., AUVERGNE M. and CATALA C.

Abstract (from CDS):

With the space-borne missions CoRoT and Kepler, a large amount of asteroseismic data is now available and has led to a variety of work. So-called global oscillation parameters are inferred to characterize the large sets of stars, perform ensemble asteroseismology, and derive scaling relations. The mean large separation is such a key parameter, easily deduced from the radial-frequency differences in the observed oscillation spectrum and closely related to the mean stellar density. It is therefore crucial to measure it with the highest accuracy in order to obtain the most precise asteroseismic indices. As the conditions of measurement of the large separation do not coincide with its theoretical definition, we revisit the asymptotic expressions used for analyzing the observed oscillation spectra. Then, we examine the consequence of the difference between the observed and asymptotic values of the mean large separation. The analysis is focused on radial modes. We use series of radial-mode frequencies in published analyses of stars with solar-like oscillations to compare the asymptotic and observational values of the large separation. This comparison relies on the proper use of the second-order asymptotic expansion. We propose a simple formulation to correct the observed value of the large separation and then derive its asymptotic counterpart. The measurement of the curvature of the radial ridges in the echelle diagram provides the correcting factor. We prove that, apart from glitches due to stellar structure discontinuities, the asymptotic expansion is valid from main-sequence stars to red giants. Our model shows that the asymptotic offset is close to 1/4, as in the theoretical development, for low-mass, main-sequence stars, subgiants and red giants. High-quality solar-like oscillation spectra derived from precise photometric measurements are definitely better described with the second-order asymptotic expansion. The second-order term is responsible for the curvature observed in the echelle diagrams used for analyzing the oscillation spectra, and this curvature is responsible for the difference between the observed and asymptotic values of the large separation. Taking it into account yields a revision of the scaling relations, which provides more accurate asteroseismic estimates of the stellar mass and radius. After correction of the bias (6% for the stellar radius and 3% for the mass), the performance of the calibrated relation is about 4% and 8% for estimating, respectively, the stellar radius and the stellar mass for masses less than 1.3M; the accuracy is twice as bad for higher mass stars and red giants.

Abstract Copyright:

Journal keyword(s): stars: oscillations - stars: interiors - methods: analytical - methods: data analysis

Simbad objects: 98

goto Full paper

goto View the references in ADS

Number of rows : 98
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2023
#notes
1 HD 46375 PM* 06 33 12.6224391648 +05 27 46.528531452   8.70 7.84     G9V 230 2
2 HD 49385A PM* 06 48 11.5030769640 +00 18 17.894873196   7.952 7.399 8.28   G0V 86 1
3 HD 49933 PM* 06 50 49.8309774552 -00 32 27.167495244   6.147 5.771 7.04   F3V 372 2
4 HD 50890 RG* 06 54 58.9171473552 -02 48 12.922874748   7.112 6.017     K2III 39 0
5 HD 52265 PM* 07 00 18.0357115416 -05 22 01.780929120   6.845 6.282     G0V 322 1
6 * alf CMi SB* 07 39 18.11950 +05 13 29.9552 0.82 0.79 0.37 -0.05 -0.28 F5IV-V+DQZ 1851 0
7 * alf Cen B PM* 14 39 35.06311 -60 50 15.0992 2.89 2.21 1.33     K1V 1005 2
8 * alf Cen A SB* 14 39 36.49400 -60 50 02.3737 0.96 0.72 0.01     G2V 1258 1
9 * 18 Sco PM* 16 15 37.2702755653 -08 22 09.982125430   6.15 5.50     G2Va 585 0
10 * mu. Ara PM* 17 44 08.7031414872 -51 50 02.591603160   5.85 5.15     G3IV-V 523 2
11 HD 169392A SB* 18 24 42.9854204880 -06 36 13.674463524   7.98 7.41     G0IV 41 0
12 BD+47 2683 * 18 43 42.4230433392 +47 56 16.009897416   9.85 9.26     G0V 70 0
13 2MASS J18441281+4332024 RG* 18 44 12.8095920264 +43 32 02.367065760   10.756 9.676 9.465   K1IV 34 0
14 HD 173701 PM* 18 44 35.1191008536 +43 49 59.790008892   8.37 7.52     G8V 165 0
15 BD+46 2555 Ro* 18 47 39.2486448504 +46 41 09.979229364   9.98 9.52     F6IV 47 0
16 BD+47 2703 Er* 18 49 33.6586835784 +47 42 39.607192296   10.16 9.54 9.473   F9IV-V 45 0
17 BD+42 3187 RG* 18 54 16.9544655840 +42 59 00.384912816   10.495 9.939 10.086   G2 84 0
18 BD+45 2796 PM* 18 56 21.2642726544 +45 30 53.234154468   9.80 9.29     G0.5IV 87 0
19 HD 176071 Er* 18 56 22.1268370056 +45 30 25.361404632   8.81 8.33     F8IV 82 0
20 HD 176153 Ro* 18 56 36.6514583496 +47 39 23.133492756   9.20 8.68     F9IV-V 78 0
21 TYC 3127-1472-1 RG* 18 57 58.6494188088 +42 27 31.613965236   12.32 11.52     ~ 30 0
22 HD 176693 Er* 18 59 08.6844743448 +48 25 23.600359776   9.34 8.83 8.996   F8V 115 0
23 TYC 3541-1117-1 RG* 18 59 09.8407415520 +46 17 05.703253368   11.99 10.99     ~ 23 0
24 TYC 3541-1197-1 RG* 18 59 58.6326219840 +46 14 30.262140816   12.71 11.81     K0II 31 0
25 2MASS J19000746+4545325 RG* 19 00 07.4662254528 +45 45 32.505588612           K1IV 39 0
26 TYC 3124-2345-1 RG* 19 01 13.9637622744 +41 09 06.025364748   12.13 11.73     ~ 28 0
27 HD 177153 PM* 19 01 39.6780721176 +41 29 24.328113936   7.76 7.21     G0 110 0
28 TYC 3545-1033-1 * 19 04 45.6026995824 +48 21 33.390090000   11.349 10.909 10.871   F6IV 24 0
29 BD+38 3428 PM* 19 05 45.2617733112 +38 31 22.560830328   9.77 9.22     F9IV-V 59 0
30 HD 178509 Ro* 19 06 55.9481056080 +42 40 19.342963020   9.39 8.86     F8IV 49 0
31 BD+42 3247 SB* 19 06 58.3280630808 +42 26 08.260897020   10.32 9.75     G0.5IV 64 0
32 BD+49 2935 RG* 19 06 59.9011441032 +49 32 24.408913668   10.68 9.54     K0 30 0
33 HD 179070 Er* 19 09 26.8349590368 +38 42 50.455534860   8.767 8.25 8.00   F6IV 160 1
34 2MASS J19092934+4549339 HB* 19 09 29.3465155728 +45 49 33.892808916           G9.5III 27 0
35 TYC 3124-914-1 RG* 19 09 35.6700770712 +39 29 50.700358356   11.25 10.19 9.835   ~ 31 0
36 TYC 3550-300-1 * 19 09 55.5029520480 +49 15 04.351525056   11.69 10.95     G4-5IV-V 34 0
37 TYC 3125-915-1 Er* 19 10 35.1292987128 +40 50 35.025862956   11.61 10.751 10.697   G3.5III 23 0
38 HD 179421 HB* 19 10 50.6161659624 +39 10 17.977985760   9.36 7.7957     K5 25 0
39 2MASS J19105863+4646538 RG* 19 10 58.6392294552 +46 46 53.811228432           G8IV-V 35 0
40 TYC 3125-2310-1 HB* 19 13 39.1172473224 +40 11 04.687016100   11.99 11.43     G8IV-V 35 0
41 TYC 3550-257-1 RG* 19 16 23.1882620664 +50 25 37.850253564   13.53 11.94     K1III 24 0
42 BD+39 3706 SB* 19 16 34.9026130056 +40 02 50.359631244       9.1   G1.5V 75 0
43 HD 234856 Ro* 19 17 45.8018919144 +50 28 48.274775580   9.87 9.32     F9IV-V 76 0
44 HD 181207 PM* 19 17 46.3565007888 +41 24 36.838219932   9.06 8.47     F9IV-V 81 0
45 BD+43 3209 * 19 18 54.1337809824 +43 29 46.691977452   10.14 9.52 9.46   F9IV-V 44 0
46 2MASS J19192456+4031447 RG* 19 19 24.5600967384 +40 31 44.799282444           K2III 26 0
47 HD 181420 PM* 19 20 27.0720449304 -01 18 35.132869692   6.98 6.55     F6V 87 0
48 BD+41 3315 PM* 19 20 29.3442099120 +41 17 28.510142676   9.92 9.38     F9IV-V 42 0
49 BD+43 3221 * 19 20 47.9392965792 +44 09 18.751522032   10.03 9.50     F9IV-V 74 0
50 TYC 3555-1403-1 * 19 20 52.7286151344 +51 28 18.186868416   10.68 9.78     K0III-IV 34 0
51 BD+48 2882 ** 19 21 24.640392 +48 30 53.31924   10.27 9.45 9.36   G1V 55 0
52 BD+48 2887 * 19 22 20.2267974168 +48 41 43.496977812   9.43 9.01     F5IV 41 0
53 HD 181907 RG* 19 22 21.5480809056 -00 15 08.508393504   6.906 5.811     K1III 61 0
54 BD+38 3559 RG* 19 22 27.4541289912 +38 50 52.908872712   10.79 9.81     K2 43 0
55 HD 182633 * 19 23 36.9148636608 +43 53 28.653685440   8.97 8.47     F5IV-V 30 0
56 BD+43 3228 Er* 19 23 56.4112114464 +43 18 52.537486464   10.830 10.170 10.035   G0V 56 0
57 HD 182736 Er* 19 24 03.3792608280 +44 56 00.738992328   7.82 7.01     G8IV 71 0
58 BD+41 3338 * 19 24 11.1933479232 +42 03 09.726975180   9.97 9.19     G8IV-V 67 0
59 HD 182756 * 19 24 30.3488274144 +40 19 23.671912908   9.01 8.31     G1V 66 0
60 TYC 2666-485-1 HB* 19 24 45.8456098488 +37 29 38.560339284   12.36 11.52     K1III 29 0
61 TYC 3547-2260-1 * 19 26 05.7608041584 +47 21 30.042774432   11.40 10.80 10.77   F9IV-V 27 0
62 HD 183298 PM* 19 26 22.0906256352 +50 59 14.334181836   8.71 8.16     G0.5IV 95 0
63 TYC 3551-149-1 PM* 19 27 20.4900952416 +48 57 12.010523580   10.59 9.85     G5IV 50 0
64 TYC 3547-1968-1 * 19 27 45.7618590576 +48 19 45.419795472   12.04 11.64 12.02   G1.5IV-V 26 0
65 TYC 3146-611-1 RG* 19 28 19.0903164432 +44 19 18.595247268   13.35 11.71     G6V 51 0
66 BD+36 3570 Ro* 19 28 19.8441075024 +37 03 35.403120000   9.40 8.97     F8IV 58 0
67 TYC 3551-1158-1 * 19 29 01.8626404752 +49 51 54.860504292   11.39 10.83     G2V 23 0
68 HD 184401 PM* 19 32 14.5949892072 +45 18 38.308886100   9.63 8.95     G4V 50 0
69 TYC 3564-2640-1 Ro* 19 34 00.2762796624 +48 50 08.883866472   11.60 10.88     G8IV-V 27 0
70 BD+46 2726 Er* 19 34 43.0022454096 +46 51 09.938179044   10.36 9.64 9.438   K0V 115 0
71 TYC 3143-53-1 Ro* 19 35 03.7372740120 +42 44 16.724850540   10.31 9.85     F8IV 61 0
72 BD+44 3183 PM* 19 35 50.5739000112 +44 52 50.022974316   9.38 8.92     hF6mF2gF5V 56 0
73 TYC 3560-968-1 RG* 19 35 59.6201211312 +48 17 30.376997520   12.64 11.52     K1IV 33 0
74 BD+49 3061 * 19 36 18.8482043712 +49 49 26.946226164   10.32 9.49     G8IV 32 0
75 TYC 3135-624-1 PM* 19 36 48.8136243480 +38 42 56.789855496   10.35 9.55     G5IV 72 0
76 BD+44 3197 Er* 19 37 54.5252033200 +44 59 04.630621506   10.287 9.641 9.546   G0IV 71 0
77 TYC 3556-909-1 Er* 19 37 56.6968217208 +45 57 52.273038852   11.31 10.78 10.643   F6V 45 0
78 HD 185834 * 19 39 00.6724153968 +46 54 06.984718740   9.26 8.78     F6IV 40 0
79 TYC 3556-3445-1 PM* 19 40 21.2108930904 +45 29 20.963746392   10.48 9.91     G3V 68 0
80 HD 186355 RG* 19 41 35.3530024032 +49 41 43.288852740   8.90 7.93     G5 26 0
81 * 16 Cyg A ** 19 41 48.9534996168 +50 31 30.219536784 6.79 6.59 5.95 5.50 5.17 G1.5Vb 743 0
82 * 16 Cyg B PM* 19 41 51.9726777456 +50 31 03.089030916 7.07 6.86 6.20 5.76 5.42 G3V 871 1
83 HD 186700 PM* 19 43 39.6223173216 +48 55 43.808906244   8.86 8.47     F5IV-V 68 0
84 TYC 3565-1303-1 Er* 19 43 57.7105385736 +49 55 21.497410956   12.02 11.471 11.290   G0 31 0
85 TYC 3148-712-1 HB* 19 44 58.1937477240 +44 19 05.089463364   12.76 11.40     G9III 24 0
86 TYC 3565-1235-1 Er* 19 45 45.9639229488 +49 59 18.851817444   10.68 9.84 9.677   K1V 38 0
87 BD+44 3244 * 19 46 17.8465825824 +44 49 39.614328156   10.24 9.51     G5IV-V 40 0
88 HD 234998 PM* 19 46 37.7417153592 +51 01 13.527778440   9.16 8.75     F5 49 0
89 HD 187160 SB* 19 46 41.3411982432 +44 20 54.601189476   7.650 7.083     F9IV-V 95 0
90 BD+43 3368 * 19 48 14.2913289840 +43 44 48.961091040   9.63 9.17     F8V 43 0
91 HD 187582 PM* 19 48 22.4074859616 +49 14 11.852056752   9.40 8.71     G3V 40 0
92 TYC 3144-592-1 RG* 19 49 36.5254311768 +41 24 14.228189280   12.22 11.22     ~ 38 0
93 HD 226069 HB* 19 50 04.5839236776 +39 52 21.579614004   10.78 9.767     K1III 31 0
94 BD+47 2934 Ro* 19 50 14.2728443568 +47 28 25.166654760   9.68 9.24     F5IV-V 42 0
95 HD 188819 Ro* 19 54 54.1810396872 +47 08 42.949406328   9.12 8.66     F8IV 63 0
96 HD 190166 Er* 20 01 51.4248305136 +44 21 14.147515008   10.13 9.581 9.523   F8V 53 0
97 HD 190319 PM* 20 02 33.3210896856 +44 31 58.994152536   10.63 9.91     G2.5V 37 0
98 * gam Pav PM* 21 26 26.6049826473 -65 21 58.313057521 4.57 4.70 4.22 3.75 3.45 F9VFe-1.4CH-0.7 410 0

To bookmark this query, right click on this link: simbad:objects in 2013A&A...550A.126M and select 'bookmark this link' or equivalent in the popup menu


2023.09.23-22:58:28

© Université de Strasbourg/CNRS

    • Contact