2023MNRAS.526L..83H


Query : 2023MNRAS.526L..83H

2023MNRAS.526L..83H - Mon. Not. R. Astron. Soc., 526, L83-L87 (2023/November-3)

Searching for magnetic fields in pulsating A-type stars: the discovery of a strong field in the probable δ Sct star HD 340577 and a null result for the γ Dor star HR 8799.

HUBRIG S., JARVINEN S.P., ALVARADO-GOMEZ J.D., ILYIN I. and SCHOLLER M.

Abstract (from CDS):

Numerous δ Sct and γ Dor pulsators are identified in the region of the Hertzsprung-Russell diagram that is occupied by chemically peculiar magnetic Ap stars. The connection between δ Sct and γ Dor pulsations and the magnetic field in Ap stars is however not clear: theory suggests for magnetic Ap stars some critical field strengths for pulsation mode suppression by computing the magnetic damping effect for selected p and g modes. To test these theoretical considerations, we obtained PEPSI spectropolarimetric snapshots of the typical Ap star HD 340577, for which δ Sct-like pulsations were recently detected in Transiting Exoplanet Survey Satellite data, and the γ Dor pulsator HR 8799, which is a remarkable system with multiple planets and two debris discs. Our measurements reveal the presence of a magnetic field with a strength of several hundred Gauss in HD 340577. The measured mean longitudinal field would be the strongest field measured so far in a δ Sct star if the pulsational character of HD 340577 is confirmed spectroscopically. No magnetic field is detected in HR 8799.

Abstract Copyright: © 2023 The Author(s) Published by Oxford University Press on behalf of Royal Astronomical Society

Journal keyword(s): techniques: polarimetric - techniques: spectroscopic - stars: chemically peculiar - stars: individual: HD 340577, HR 8799 - stars: magnetic field - stars: oscillations

Simbad objects: 14

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Number of rows : 14
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 HD 965 Pe* 00 14 04.0648431696 -00 02 00.098903652   8.94 8.57     A1III-IVSrSiEu 81 0
2 V* CP Oct dS* 03 09 53.7500021592 -83 31 53.581689012   8.01 7.61     F2/3Ib/II 66 0
3 * E Pup SB* 07 12 15.8070021456 -40 29 55.755380940   5.38 5.31     A1/2V:+ApSrEu 112 0
4 HD 116114 PM* 13 21 46.3079033856 -18 44 31.563482928   7.34 7.02     F0VpSrCrEu 145 0
5 HD 133792 * 15 09 25.5217838448 -63 38 34.549433448   6.298 6.247     ApSrCrEu 82 0
6 * bet CrB a2* 15 27 49.7540595700 +29 06 20.494640434 4.08 3.97 3.68 3.50 3.45 F2VpSrCrEuSi 703 0
7 HD 177765 * 19 07 09.7793979672 -26 19 54.506413128   9.60 9.15     ApSrEuCr 40 0
8 KOI-6237 dS* 19 26 17.5548700656 +49 05 51.881760456   12.03 11.67     F0V 17 0
9 HD 184471 SB* 19 33 20.4267326904 +32 34 37.124341284   9.31 9.00     A8SrCrEu 53 0
10 HD 191742 a2* 20 09 47.0414403552 +42 32 28.814787780   8.36 8.16     A7p 79 0
11 HD 340577 a2* 20 34 40.8259625472 +26 29 07.645780140   9.29 9.09     ~ 19 0
12 TYC 1718-851-1 * 23 07 24.5842410000 +21 08 01.068712476   11.5 9.75     G0 4 0
13 SDSS J230725.90+210459.0 HB* 23 07 25.9082363496 +21 04 59.093467428           A0 4 0
14 HD 218396 El* 23 07 28.7157209544 +21 08 03.310767492   6.21 5.953     F0+VkA5mA5 1285 0

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