2017A&A...598A..62M


Query : 2017A&A...598A..62M

2017A&A...598A..62M - Astronomy and Astrophysics, volume 598A, 62-62 (2017/2-1)

Dipole modes with depressed amplitudes in red giants are mixed modes.

MOSSER B., BELKACEM K., PINCON C., TAKATA M., VRARD M., BARBAN C., GOUPIL M.-J., KALLINGER T. and SAMADI R.

Abstract (from CDS):

Context. Seismic observations with the space-borne Kepler mission have shown that a number of evolved stars exhibit low-amplitude dipole modes, which is referred to as depressed modes. Recently, these low amplitudes have been attributed to the presence of a strong magnetic field in the stellar core of those stars. Subsequently, and based on this scenario, the prevalence of high magnetic fields in evolved stars has been inferred. It should be noted, however, that this conclusion remains indirect.
Aims. We intend to study the properties of mode depression in evolved stars, which is a necessary condition before reaching conclusions about the physical nature of the mechanism responsible for the reduction of the dipole mode amplitudes.
Methods. We perform a thorough characterization of the global seismic parameters of depressed dipole modes and show that these modes have a mixed character. The observation of stars showing dipole mixed modes that are depressed is especially useful for deriving model-independent conclusions on the dipole mode damping. We use a simple model to explain how mode visibilities are connected to the extra damping seen in depressed modes.
Results. Observations prove that depressed dipole modes in red giants are not pure pressure modes but mixed modes. This result, observed in more than 90% of the bright stars (mV≤11), invalidates the hypothesis that depressed dipole modes result from the suppression of the oscillation in the radiative core of the stars. Observations also show that, except for visibility, seismic properties of the stars with depressed modes are equivalent to those of normal stars. The measurement of the extra damping that is responsible for the reduction of mode amplitudes, without any prior on its physical nature, potentially provides an efficient tool for elucidating the mechanism responsible for the mode depression.
Conclusions. The mixed nature of the depressed modes in red giants and their unperturbed global seismic parameters carry strong constraints on the physical mechanism responsible for the damping of the oscillation in the core. This mechanism is able to damp the oscillation in the core but cannot fully suppress it. Moreover, it cannot modify the radiative cavity probed by the gravity component of the mixed modes. The recent mechanism involving high magnetic fields proposed for explaining depressed modes is not compliant with the observations and cannot be used to infer the strength and prevalence of high magnetic fields in red giants.

Abstract Copyright: © ESO, 2017

Journal keyword(s): stars: oscillations - stars: evolution - stars: magnetic field - stars: interiors

VizieR on-line data: <Available at CDS (J/A+A/598/A62): tablea1.dat>

Simbad objects: 74

goto Full paper

goto View the references in ADS

Number of rows : 74
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 UCAC4 673-069070 RG* 18 50 11.0733394632 +44 33 18.507142656   14.992 13.749 13.488   K2III 9 0
2 TYC 3123-1482-1 HB* 18 52 28.6937576352 +40 33 21.923258184   12.92 11.36     G9IIIb 21 0
3 TYC 3131-790-1 HB* 18 52 58.2023403384 +43 51 57.462118488   11.91 10.81     ~ 11 0
4 TYC 3549-1607-1 HB* 18 57 17.6820503784 +49 40 38.833894416   11.28 10.09     ~ 25 0
5 2MASS J18583349+4412000 RG* 18 58 33.4995751272 +44 12 00.060339240           ~ 24 0
6 TYC 3120-964-1 HB* 19 03 49.8342286728 +37 55 46.305492888   11.60 10.36     K1.5III 23 0
7 2MASS J19040060+4119524 RG* 19 04 00.5987046840 +41 19 52.380351012           ~ 18 0
8 TYC 3545-1014-1 HB* 19 04 57.2221944864 +47 55 32.311192548   12.05 11.15     ~ 25 0
9 UCAC4 666-072370 * 19 05 59.7275426472 +43 09 07.870920912   14.068 12.923 12.660   ~ 8 0
10 TYC 3554-327-1 HB* 19 10 00.7877998680 +51 21 04.651608672   10.83 9.72     ~ 10 0
11 2MASS J19102313+4311562 RG* 19 10 23.1345565608 +43 11 56.232752604           ~ 27 0
12 2MASS J19111567+3838265 RG* 19 11 15.6726937896 +38 38 26.567389176           ~ 21 0
13 UCAC4 657-070295 RG* 19 13 48.1179236616 +41 15 35.144646948   14.713 13.532 13.303   ~ 6 0
14 TYC 3546-946-1 HB* 19 15 01.6214949120 +48 14 44.185502616   12.06 11.17     G6III 12 0
15 UCAC4 682-066474 HB* 19 16 27.8202048672 +46 14 41.475582276   14.396 13.160 12.829   ~ 13 0
16 UCAC4 689-066583 RG* 19 17 07.8407607528 +47 46 57.961323372   15.340 14.244 13.967   ~ 5 0
17 UCAC4 652-069505 RG* 19 18 16.4945188176 +40 23 42.877696488   14.531 13.355 12.978   G6V 8 0
18 2MASS J19182638+5031006 RG* 19 18 26.3879204280 +50 31 00.642868536           K2III 9 0
19 UCAC4 668-074656 RG* 19 18 45.1350415680 +43 29 19.330339416   14.606 13.473 13.155   K1IV 19 0
20 UCAC4 685-067400 * 19 20 46.8052052928 +46 51 50.441730624   14.320 13.029 12.683   ~ 7 0
21 TYC 3142-1466-1 HB* 19 21 15.4792116480 +41 21 56.206595520   11.32 10.04     ~ 22 0
22 TYC 3555-1444-1 HB* 19 22 00.7621712664 +51 48 12.890323260   12.673 11.460 11.167   G8Iab: 13 0
23 TYC 3551-354-1 HB* 19 22 27.1033767768 +50 36 49.089784896   12.49 11.14     ~ 8 0
24 UCAC4 670-073581 RG* 19 22 28.8943116168 +43 53 19.178170044   14.360 13.058 12.762   ~ 10 0
25 UCAC4 651-070552 RG* 19 22 30.5525070720 +40 06 42.087692484   14.321 13.082 12.854   ~ 18 0
26 TYC 3134-1884-1 HB* 19 23 25.7165393976 +37 52 33.637126908   12.85 11.70     ~ 22 0
27 UCAC4 675-072191 RG* 19 24 15.9652049616 +44 50 24.426974796   14.704 13.403 13.116   ~ 18 0
28 UCAC4 679-068653 RG* 19 25 06.7188297744 +45 44 53.698829604   14.363 13.172 12.906   ~ 17 0
29 TYC 3134-244-1 RG* 19 25 35.1712231104 +38 32 01.802462784   13.13 11.81     K1IV 27 0
30 TYC 3547-1469-1 HB* 19 26 54.0397773000 +47 41 29.449369644   12.04 10.87     ~ 22 0
31 UCAC4 675-072867 HB* 19 27 45.1716806136 +44 53 55.799978568   14.373 13.332 13.031   ~ 15 0
32 TYC 3134-64-1 HB* 19 28 05.3266046544 +38 06 14.801339592   10.79 9.75     ~ 22 0
33 TYC 3138-727-1 HB* 19 28 10.6060005984 +40 48 48.832621380   13.23 11.41     ~ 17 0
34 TYC 3543-1440-1 HB* 19 28 43.9785030672 +46 21 26.712358560   12.85 11.93     G9III 24 0
35 TYC 3543-1535-1 HB* 19 28 59.6345754888 +46 24 42.575677056   11.28 10.13     K2IV 25 0
36 BD+44 3149 RG* 19 29 08.4405017304 +44 38 28.452855300   10.84 10.08 9.843   G9.5IV 40 0
37 TYC 3146-1176-1 HB* 19 29 30.3205845408 +44 26 06.350069400   13.14 11.89     ~ 21 0
38 UCAC4 641-070743 RG* 19 30 31.9950713016 +38 05 24.068792688   15.250 14.094 13.934   ~ 5 0
39 BD+41 3381 HB* 19 32 15.6348837408 +42 02 58.310721924   10.35 9.49     F8 19 0
40 UCAC4 656-074426 RG* 19 33 12.5229849456 +41 07 29.063297964   14.839 13.614 13.325   ~ 5 0
41 UCAC4 658-076099 HB* 19 33 56.0877585000 +41 33 31.483825560   13.481 12.367 12.074   ~ 17 0
42 UCAC4 674-073273 * 19 34 05.6609897640 +44 36 19.075022424   14.921 13.600 13.333   ~ 7 0
43 TYC 3147-77-1 HB* 19 34 31.1136955296 +44 41 58.993158984   12.87 11.86     K0III 24 0
44 UCAC4 658-076639 RG* 19 36 08.1049396584 +41 26 03.930923616       13.486   K0III 6 0
45 UCAC4 645-073414 RG* 19 37 28.6286177856 +38 49 03.270672912   14.146 13.174 12.854   ~ 17 0
46 UCAC4 644-073082 RG* 19 40 15.6920170680 +38 44 55.440869532   15.462 14.070 13.785   ~ 6 0
47 TYC 3556-3559-1 HB* 19 40 50.0116732344 +45 03 47.055032892   12.04 11.01     K2III 22 0
48 TYC 3148-2052-1 RG* 19 41 42.0433589832 +43 21 51.409045404   12.53 12.06     F8IV 22 0
49 TYC 3565-404-1 HB* 19 42 16.4619809448 +49 19 08.061520008   11.18 10.18     ~ 24 0
50 UCAC4 650-075371 RG* 19 42 23.8463241144 +39 53 00.072357288   14.691 13.944 13.667   ~ 5 0
51 UCAC4 683-073702 RG* 19 42 26.5439340528 +46 27 42.834440232   14.643 13.470 13.140   G6V 6 0
52 TYC 3148-1485-1 HB* 19 43 35.2170926712 +44 42 53.193903480   10.31 9.26     K0III 8 0
53 UCAC4 703-067940 HB* 19 43 36.6739093368 +50 35 48.721736580   13.643 12.588 12.343   ~ 8 0
54 TYC 3557-1630-1 HB* 19 43 53.2833514824 +45 42 53.260159428   12.63 11.44     ~ 20 0
55 UCAC4 679-072396 RG* 19 44 12.8056084032 +45 39 55.873891872   14.337 13.183 12.917   ~ 17 0
56 TYC 3565-1220-1 HB* 19 46 04.5861472248 +49 16 00.329863728   11.78 10.70     ~ 22 0
57 2MASS J19463521+3914028 RG* 19 46 35.2191073224 +39 14 02.818032000   13.764 12.595 12.354   ~ 6 0
58 UCAC4 653-080362 RG* 19 48 15.7141668624 +40 28 59.606164272   13.642 12.562 12.222   G6V 18 0
59 2MASS J19483816+4926398 RG* 19 48 38.1634028472 +49 26 39.783509196           ~ 20 0
60 UCAC4 688-073465 RG* 19 49 55.6525599576 +47 32 31.534383336   14.684 13.646 13.406   ~ 5 0
61 UCAC4 649-076706 RG* 19 50 19.7555814264 +39 38 48.892252020   14.564 13.534 13.235   ~ 16 0
62 2MASS J19503485+4703394 HB* 19 50 34.8547228944 +47 03 39.365751384           K1IV 15 0
63 2MASS J19511407+4456119 HB* 19 51 14.0734373784 +44 56 11.975721900           K1IV 20 0
64 TYC 3141-109-1 HB* 19 51 34.1007806352 +39 52 16.263810372   12.43 11.83     ~ 19 0
65 UCAC4 688-073917 HB* 19 52 01.5915842688 +47 35 26.070224028       13.161   ~ 15 0
66 UCAC4 685-072991 HB* 19 52 51.6797631528 +46 55 59.830795992   13.504 12.410 12.206   ~ 17 0
67 UCAC4 663-082974 RG* 19 53 30.4113774168 +42 25 44.598677592   14.561 13.461 13.087   ~ 19 0
68 TYC 3145-2124-1 HB* 19 55 42.6605988864 +41 31 21.827067276   11.74 10.54     ~ 18 0
69 2MASS J19554808+4532293 HB* 19 55 48.0879951912 +45 32 29.344806276           ~ 20 0
70 UCAC4 653-083678 RG* 19 56 42.1438075272 +40 27 22.861977084   14.676 13.498 13.065   ~ 8 0
71 UCAC4 672-079411 RG* 19 58 15.7444822824 +44 21 13.108439556   13.819 12.675 12.282   ~ 15 0
72 TYC 3558-2338-1 HB* 19 59 04.7263610496 +45 28 35.466827484   12.85 11.90     ~ 16 0
73 UCAC4 673-082387 HB* 20 00 01.7472242664 +44 34 47.783758620   13.311 12.313 12.089   G5V: 21 0
74 TYC 3162-184-1 HB* 20 04 44.2330215552 +44 19 54.254896032   12.78 12.08     G6V 21 0

To bookmark this query, right click on this link: simbad:objects in 2017A&A...598A..62M and select 'bookmark this link' or equivalent in the popup menu


2023.11.28-23:12:45

© Université de Strasbourg/CNRS

    • Contact