2018A&A...616A..77B


Query : 2018A&A...616A..77B

2018A&A...616A..77B - Astronomy and Astrophysics, volume 616A77-77 (2018/8-1)

K2 space photometry reveals rotational modulation and stellar pulsations in chemically peculiar A and B stars.

BOWMAN D.M., BUYSSCHAERT B., NEINER C., PAPICS P.I., OKSALA M.E. and AERTS C.

Abstract (from CDS):


Context. The physics of magnetic hot stars and how a large-scale magnetic field affects their interior properties is largely unknown. Few studies have combined high-quality observations and modelling of magnetic pulsating stars, known as magneto-asteroseismology, primarily because of the dearth of detected pulsations in stars with a confirmed and well-characterised large-scale magnetic field.
Aims. We aim to characterise observational signatures of rotation and pulsation in chemically peculiar candidate magnetic stars using photometry from the K2 space mission. Thus, we identify the best candidate targets for ground-based, optical spectropolarimetric follow-up observations to confirm the presence of a large-scale magnetic field.
Methods. We employed customised reduction and detrending tools to process the K2 photometry into optimised light curves for a variability analysis. We searched for the periodic photometric signatures of rotational modulation caused by surface abundance inhomogeneities in 56 chemically peculiar A and B stars. Furthermore, we searched for intrinsic variability caused by pulsations (coherent or otherwise) in the amplitude spectra of these stars.
Results. The rotation periods of 38 chemically peculiar stars are determined, 16 of which are the first determination of the rotation period in the literature. We confirm the discovery of high-overtone roAp pulsation modes in HD 177765 and find an additional 3 Ap and Bp stars that show evidence of high-overtone pressure modes found in roAp stars in the form of possible Nyquist alias frequencies in their amplitude spectra. Furthermore, we find 6 chemically peculiar stars that show evidence of intrinsic variability caused by gravity or pressure pulsation modes.
Conclusions. The discovery of pulsations in a non-negligible fraction of chemically peculiar stars make these stars high-priority targets for spectropolarimetric campaigns to confirm the presence of their expected large-scale magnetic field. The ultimate goal is to perform magneto-asteroseismology and probe the interior physics of magnetic pulsating stars.

Abstract Copyright: © ESO 2018

Journal keyword(s): stars: chemically peculiar - stars: magnetic field - stars: rotation - stars: oscillations - stars: early-type

Simbad objects: 70

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Number of rows : 70
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* V1137 Tau a2* 04 12 51.2508054048 +22 24 48.482221392 6.04 6.31 6.12     B8III 113 0
2 HD 284639 Pe* 04 45 59.1995492976 +23 55 00.585773328   10.13 9.68     A0IVSrSiEu 14 0
3 V* V901 Ori Ro* 05 40 56.3704617744 -01 30 25.856677224 5.96 6.82 6.96     B2V 354 2
4 [M67b] +23 378 * 06 03 08.8183378272 +23 47 23.674998048   12.988 11.804 11.470   F2p 2 0
5 HD 41641 dS* 06 06 40.5782639808 +06 43 49.884406824   8.14 7.86     A5III 32 0
6 [M67b] +22 562 ** 06 07 54.589344 +22 13 57.68400   11.812 11.528 11.272   B9p 7 0
7 HD 43317 Pu* 06 15 47.0134228488 +04 17 01.095049500 5.82 6.456 6.614     B3IV 129 0
8 HD 255134 * 06 19 53.7083224224 +23 15 54.431023536 9.01 9.46 9.18     B1IVp 17 0
9 HD 51452 Be* 06 57 20.6218257456 -04 11 37.423878864 7.51 8.21 8.08     B7Ib/II 53 0
10 NGC 2682 OpC 08 51 23.5 +11 48 54           ~ 2528 0
11 HD 97859 Pe* 11 15 30.8977471992 +04 57 23.494903236 8.695 9.238 9.352 9.387 9.441 B8IVpSi 53 0
12 HD 107000 * 12 18 19.1143455888 +03 06 04.031130240   8.21 8.02     A3IV 30 0
13 V* CU Vir a2* 14 12 15.8055434051 +02 24 33.945178515 4.46 4.90 5.02 5.10 5.23 ApSi 411 0
14 V* V913 Sco Ro* 15 58 34.8665694960 -24 49 53.361727284 4.70 5.34 5.43     B5V 226 0
15 HD 145792 a2* 16 13 45.4979280816 -24 25 19.529982106   6.43 6.43   6.14 B6IV 137 0
16 V* V933 Sco a2* 16 20 05.4927999744 -20 03 23.030685720   7.56 7.40     B8:VpSrTiSiEu 204 0
17 V* V955 Sco a2* 16 39 31.5581287440 -27 17 08.162953368   8.92 8.71     A2IVpSrCrEu 63 0
18 HD 152366 * 16 53 57.7037825496 -25 04 09.279361956   8.11 8.08     ApSi 33 0
19 HD 152834 a2* 16 56 58.0234511112 -26 57 05.597514828   8.85 8.83     ApSi 19 0
20 HD 153192 a2* 16 59 05.5222424856 -27 04 55.155735264   10.12 10.08     ApEuCr(Sr) 14 0
21 HD 153997 a2* 17 03 36.2612386656 -19 27 43.797889548   9.56 9.49     ApSi 15 0
22 HD 155127 a2* 17 10 52.1369607024 -26 27 06.081530724   8.59 8.38     kA0hA5mF0II 24 0
23 HD 158336 a2* 17 29 26.7041018376 -18 39 51.180791868   9.49 9.36     ApSi 23 0
24 HD 158596 a2* 17 31 03.4615721783 -21 29 07.061673182   9.45 9.53 9.67   ApSi 30 0
25 HD 161342 * 17 46 01.0005380856 -22 37 30.577306404   8.95 8.66     B8III(pSi) 11 0
26 HD 161851 * 17 49 00.4162095264 -25 44 58.352498016   8.72 8.61     ApSi 12 0
27 HD 162759 Pe* 17 53 36.1173275448 -24 26 06.660963960   10.41 10.10     ApSi 9 0
28 HD 162814 * 17 53 53.8121260800 -23 22 30.546841476   10.86 10.24     ApSi 13 0
29 V* V2052 Oph bC* 17 56 18.4001168880 +00 40 13.273317228 5.28 5.874 5.820     B3III 222 0
30 HD 164085 a2* 18 00 12.0156365880 -17 05 20.495801400   10.42 10.19     ApSi 11 0
31 2MASS J18002338-2258032 EB* 18 00 23.3865025872 -22 58 03.233451468     12.4     ~ 2 0
32 HD 164068 * 18 00 24.1437834744 -22 57 52.078082184   10.04 9.90     ApSi 9 0
33 HD 164190 * 18 00 51.5245432536 -18 58 04.117632564   9.37 9.13     ApSi 8 0
34 HD 164224 * 18 00 57.6150005880 -20 59 17.208523788   8.67 8.49     ApSiCr 27 0
35 HD 165321 * 18 06 29.7732154224 -24 09 32.985545580   9.13 8.97     A0V(pSi) 17 0
36 HD 165945 * 18 09 02.1213832512 -15 31 42.158436312   9.67 9.41     ApSrEuCr 14 0
37 HD 165972 a2* 18 09 32.5988316144 -24 39 49.949541360   9.02 8.96     B9II(pSi) 14 0
38 HD 166190 * 18 10 21.9353147424 -21 16 35.152376700   10.01 9.81     A(pSi) 8 0
39 HD 166542 * 18 11 51.9590631912 -18 28 52.132753848   9.92 9.94     ApSi 8 0
40 HD 166804 a2* 18 13 03.3926426832 -18 18 44.212796784   8.84 8.90     ApSi 16 0
41 HD 167700 * 18 17 24.8535006672 -24 24 04.422872700   9.87 9.54     ApSrEu(Cr) 8 0
42 HD 168187 * 18 19 17.7490317696 -18 19 55.163637192   10.06 10.02     B8/9Ib/II(pSi) 7 0
43 HD 172480 a2* 18 41 24.6859794216 -23 55 20.889832440   10.22 10.09     ApSi 18 0
44 V* V4404 Sgr a2* 18 45 53.2305662808 -18 21 50.650705260   7.51 7.43     ApSi 27 0
45 HD 173657 a2* 18 47 37.1495689560 -28 16 46.952143212   7.48 7.41     ApSiCr 29 0
46 HD 173857 * 18 48 34.7569607568 -27 06 56.940215688   10.44 10.40     ApSiCr(Sr) 8 0
47 HD 174146 a2* 18 50 05.2794515760 -24 14 02.390758512   10.56 10.03     ApSi(Cr) 11 0
48 HD 174356 a2* 18 51 08.6099619144 -24 23 14.527174524   9.37 9.18     ApSi 15 0
49 HD 174648 * 18 51 41.0002474368 -01 45 35.238378132   8.90 8.81     B9.5V 21 0
50 HD 176330 * 19 00 26.9045603040 -18 05 44.150363088   10.54 10.39     ApSi 13 0
51 HD 177013 * 19 03 27.0016848312 -17 18 36.035419176   9.34 9.04     ApEu 14 0
52 HD 177016 * 19 03 40.5683341872 -20 34 36.923429208   9.67 9.34     ApEuSrCr 17 0
53 HD 177562 * 19 06 19.2446469120 -27 17 13.508785824   7.39 7.38     ApSi 21 0
54 HD 177765 * 19 07 09.7793979672 -26 19 54.506413128   9.60 9.15     ApSrEuCr 40 0
55 HD 178786 * 19 10 58.8361871928 -25 40 19.719047064   10.20 10.24     ApSi(Cr) 15 0
56 HD 180303 ** 19 16 46.8292128048 -20 46 35.299735428   9.50 9.48     ApSi 16 0
57 HD 181004 Pe* 19 19 23.4141832248 -16 57 16.389434124   9.54 9.64     B8III(pSi) 16 0
58 V* V694 Lyr a2* 19 20 30.7975117080 +37 50 55.028672988     14.210   13.830 ~ 8 0
59 HD 181810 * 19 22 43.5663936528 -21 25 27.516523476   10.65 10.66     ApEuCrSr 8 0
60 HD 182459 * 19 25 40.1552775408 -23 08 12.172354260   9.52 9.59     ApSi 10 0
61 HD 184343 * 19 34 51.5492866128 -23 22 29.392923036   10.10 9.74     FpSrCrEu 8 0
62 HD 188774 dS* 19 55 10.0375808184 +41 17 10.271172480   9.05 8.81     A9IV 43 0
63 HD 200405 SB* 21 01 38.2998330624 +47 54 47.270657412   8.98 8.90     A0pSrCr 39 0
64 * bet Cep bC* 21 28 39.5968513 +70 33 38.574681 2.05 3.01 3.23 3.33 3.55 B0.5IIIs 756 0
65 * e Aqr * 22 10 37.4825833145 -11 33 53.779140933   5.299 5.422     B5III 100 0
66 * rho Aqr SB* 22 20 11.9165745768 -07 49 15.966995808 4.94 5.286 5.339     B8III 88 0
67 V* GL Lac a2* 22 44 07.5047456400 +55 35 21.211012248   8.85 8.82     kB9hB7HeB8pSi 293 0
68 * tau01 Aqr * 22 47 42.7694661672 -14 03 23.141291904   5.650 5.681   5.67 B9V 66 0
69 HD 219831 * 23 19 01.4384081496 -09 03 35.048296152   10.20 9.99     ApSr(Cr) 18 0
70 HD 220556 * 23 24 44.2648148712 -06 00 43.045437816   10.198 9.850     ApSrEuCr 13 0

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