2022A&A...660A..70M


Query : 2022A&A...660A..70M

2022A&A...660A..70M - Astronomy and Astrophysics, volume 660A, 70-70 (2022/4-1)

Long-period Ap stars discovered with TESS data: The northern ecliptic hemisphere.

MATHYS G., KURTZ D.W. and HOLDSWORTH D.L.

Abstract (from CDS):

The rotation periods of the magnetic Ap stars span five to six orders of magnitude. While it is well established that period differentiation must have taken place at the pre-main sequence stage, the physical processes that lead to it remain elusive. The existence of Ap stars that have rotation periods of tens to hundreds of years is particularly intriguing, and their study represents a promising avenue to gain additional insight into the origin and evolution of rotation in Ap stars. Historically, almost all the longest period Ap stars known have been found to be strongly magnetic; very few weakly magnetic Ap stars with very long periods have been identified and studied. To remedy that, we showed how a systematic search based on the analysis of TESS photometric data could be performed to identify super-slowly rotating Ap (ssrAp) stars independently of the strengths of their magnetic fields, with the intention to characterise the distribution of the longest Ap star rotation periods in an unbiased manner. We successfully applied this method to the analysis of the TESS 2-min cadence observations of Ap stars of the southern ecliptic hemisphere. For our present study, we applied the same approach to the analysis of the TESS 2-min cadence observations of Ap stars of the northern ecliptic hemisphere. We confirm that the technique leads to the reliable identification of ssrAp star candidates in an unbiased manner. We find 67 Ap stars with no rotational variability in the northern ecliptic hemisphere TESS data. Among them, 46 are newly identified ssrAp star candidates, which is double the number found in the southern ecliptic hemisphere. We confirm that super-slow rotation tends to occur less frequently in weakly magnetic Ap stars than in strongly magnetic stars. We present new evidence of the existence of a gap between ∼2 kG and ∼3 kG in the distribution of the magnetic field strengths of long period Ap stars. We also confirm that the incidence of roAp stars is higher than average in slowly rotating Ap stars. We report the unexpected discovery of nine definite and five candidate δ Sct stars, and of two eclipsing binaries. This work paves the way for a systematic, unbiased study of the longest period Ap stars, with a view to characterise the correlations between their rotational, magnetic, and pulsational properties.

Abstract Copyright: © ESO 2022

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

VizieR on-line data: <Available at CDS (J/A+A/660/A70): tablea1.dat>

Status at CDS : All or part of tables of objects could be ingested in SIMBAD with priority 2.

Simbad objects: 82

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Number of rows : 82
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 BD+65 1981 * 00 00 51.1502482224 +66 38 20.823956196   10.41 10.09     A0 6 0
2 HD 236298 * 00 05 35.8946687256 +55 16 10.774056288   9.44 9.45     ~ 7 0
3 V* GR And a2* 00 28 28.5694460472 +32 26 15.875756412   6.99 6.91     A5VpSiSrCr 145 0
4 V* V551 Cas a2* 01 00 33.4346947944 +60 26 40.930591668   8.68 8.5     B8 101 0
5 HD 7410 * 01 14 40.4129513880 +33 00 04.798103940   9.35 9.07     ~ 9 0
6 V* HN And a2* 01 24 18.6765786624 +43 08 31.629475248   6.704 6.676     A4VpSrSi 144 0
7 V* GY And a2* 01 38 31.8255225672 +45 23 58.935650100   6.343 6.380     A2:VpSiSrCrEu 258 0
8 HD 11187 * 01 51 26.6179346232 +54 55 28.849176732   8.20 7.94     A0p 64 0
9 HD 12288 a2* 02 03 30.5070540192 +69 34 56.268492384   7.83 7.74     A0pCrSi 105 0
10 V* V436 And a2* 02 21 02.6744002704 +42 56 38.228602596   7.24 7.27     B9pSrCrEu 68 0
11 BD+46 570 * 02 26 59.7142616928 +46 49 18.202874160   10.11 9.63     ~ 11 0
12 HD 17330 * 02 47 38.6052085032 +29 40 42.700349568   7.12 7.11     ~ 26 0
13 HD 18078 a2* 02 56 32.0098959576 +56 10 41.434633848   8.50 8.27     A0pSrCr 92 0
14 HD 22860 * 03 41 18.3925659000 +28 42 09.929390472   6.86 6.86     ~ 23 0
15 TYC 3729-816-1 * 03 55 47.5573016064 +59 16 10.886028780   11.85 11.35     ~ 3 0
16 HD 276625 * 04 35 29.9083214688 +41 08 10.578388128   10.33 9.94     ~ 8 0
17 HD 242800 * 05 21 38.2035408528 +32 45 31.582915992   10.75 10.55     ~ 6 0
18 HD 243007 * 05 23 08.4374663712 +30 13 27.930588240   10.47 10.2     ~ 7 0
19 BD+32 976 Pe* 05 25 17.0522046504 +32 40 41.251303452   10.59 10.28     kA3hA7mA9SiEu 7 0
20 HD 243321 * 05 25 17.8384723200 +32 36 59.111038584   9.71 9.61     ~ 5 0
21 HD 35436 * 05 26 08.6417739816 +32 48 17.638395984   9.78 9.55     ~ 5 0
22 HD 278204 Pe* 05 28 11.9950106328 +41 50 06.454382136   10.34 10.45     B9IVSi 8 0
23 HD 244545 * 05 32 41.5292051640 +32 46 16.625971524   10.67 10.37     ~ 4 0
24 HD 244640 * 05 33 35.1922854672 +33 43 28.567477308   10.09 9.94     ~ 6 0
25 HD 245416 * 05 37 32.2084636224 +31 46 41.915046468   10.03 9.71     ~ 7 0
26 HD 245726 * 05 39 07.8362790432 +32 13 31.435989924   11.0 10.8     ~ 4 0
27 TYC 2413-476-1 * 05 44 40.3305861336 +34 21 17.015726304   11.00 10.82     ~ 3 0
28 HD 247591 * 05 47 55.7964911400 +29 29 28.113305604   10.63 10.47     ~ 7 0
29 HD 247628 Pe* 05 48 19.7677903680 +33 35 16.982751768   10.85 10.59     kA3hA6mA8SiEu 11 0
30 HD 248727 * 05 53 45.8750268768 +33 17 13.712138664   10.41 10.34     ~ 6 0
31 HD 249401 * 05 57 02.0460663648 +29 32 45.601348668   11.17 10.83     ~ 5 0
32 HD 249931 * 05 59 49.0444593000 +30 56 59.813802204   10.72 10.62     ~ 6 0
33 HD 62658 EB* 07 43 47.8389980376 -32 07 21.086005548   9.23 9.29     ApSi 17 0
34 V* V414 Pup a2* 08 01 24.6419553720 -12 47 35.744707032   8.76 8.81     ApSi 33 0
35 HD 83368 a2* 09 36 25.40686 -48 45 04.2549   6.480 6.232     A8VSrCrEu+F9V 267 0
36 HD 89069 a2* 10 21 16.0361505960 +78 45 51.457200984   8.46 8.42     ~ 52 0
37 * 39 UMa PM* 10 43 43.3264670520 +57 11 57.118841016   5.744 5.782     A0III 64 0
38 HD 96003 * 11 04 33.3400626096 +12 40 01.140685752   6.89 6.87     A3p 30 0
39 HD 97127 * 11 10 53.9167670928 +17 03 47.530406160   9.83 9.43     G0 9 0
40 HD 96571 * 11 14 30.3796872744 +85 38 24.448281360   7.544 7.310     ~ 25 0
41 HD 99458 dS* 11 26 36.2793342840 +01 03 18.844480476   8.38 8.16 8.82   A4IV 14 0
42 V* DV Cha EB* 11 49 30.5806351848 -76 09 31.497840828   10.295 10.044 10.153   ApSi 22 1
43 V* AX CVn a2* 12 39 16.8606994152 +35 57 07.050433068   6.466 6.385     A0pSrCrEuKsn 175 0
44 V* V883 Cen SB* 14 08 56.2530021000 -59 16 36.154960536 5.89 6.352 6.339     B3V+B8V 67 0
45 HD 127304 * 14 29 49.6705817016 +31 47 28.278712392   6.034 6.050     A0Vs(Si) 85 0
46 TYC 2553-480-1 * 14 30 49.6431091200 +31 47 55.051464408   11.70 11.56     ~ 4 0
47 * alf Cir a2* 14 42 30.4206520931 -64 58 30.478845491 3.55 3.43 3.19 2.96 2.86 A7VpSrCrEu 364 0
48 * bet CrB a2* 15 27 49.7540595700 +29 06 20.494640434 4.08 3.97 3.68 3.50 3.45 F2VpSrCrEuSi 686 0
49 V* DQ Dra a2* 16 24 25.3384367736 +55 12 18.346742676   5.736 5.734     A2pSi 99 0
50 HD 158919 a2* 17 31 48.1093514256 +01 50 34.519669512   9.30 9.21     ApSi 12 0
51 HD 174016 SB* 18 44 21.1829894376 +61 56 19.352248908   7.90 7.45     ~ 28 0
52 BD+29 3427 * 18 59 18.4036757232 +29 48 14.893543836   9.90 9.66     F0p 9 0
53 BD+29 3448 Pu* 19 01 49.4294378472 +30 01 34.585552956   9.82 9.54     F0pSr 13 0
54 2MASS J19052003+4232382 V* 19 05 20.0392316832 +42 32 38.188591008           ~ 4 0
55 BD+44 3063 gD* 19 06 27.5519195736 +44 50 33.430309584   10.60 10.19     A9V 29 0
56 HD 179709B * 19 12 23.0783175264 +30 20 59.182864368   9.09 9.08     ~ 5 0
57 KOI-6237 dS* 19 26 17.5548700656 +49 05 51.881760456   12.03 11.67     F0V 12 0
58 TYC 3560-2018-1 dS* 19 31 26.4556229784 +48 30 03.432188916   13.03 12.50     F2IV 4 0
59 HD 184471 SB* 19 33 20.4267326904 +32 34 37.124341284   9.31 9.00     A8SrCrEu 49 0
60 HD 187400 * 19 49 06.7214754456 +20 19 02.217802512   8.70 8.63     ~ 7 0
61 V* V1291 Aql a2* 19 53 18.7357174440 -03 06 52.063556976   5.837 5.619     F0VpSrCrEu 277 0
62 HD 191742 a2* 20 09 47.0414403552 +42 32 28.814787780   8.36 8.16     A7p 76 0
63 HD 332312 * 20 29 18.7116637464 +31 41 14.671280328   10.07 9.72 9.70   A2 7 0
64 HD 340577 a2* 20 34 40.8259625472 +26 29 07.645780140   9.29 9.09     ~ 16 0
65 HD 335238 * 20 50 43.6655493504 +29 48 12.042715104   9.30 9.26     A2 43 0
66 BD+47 3253 * 21 00 54.9941085744 +48 00 22.822140852   9.69 9.55     A1IV 8 0
67 V* V2200 Cyg a2* 21 01 14.3203959696 +43 43 18.402894444   7.60 7.68     B9p 128 0
68 BD+39 4435 ** 21 06 06.32 +40 00 36.9     9.3     ~ 6 0
69 * gam Equ a2* 21 10 20.5000721160 +10 07 53.691967776 5.03 4.94 4.68 4.43 4.32 A9VpSrCrEu 552 0
70 BD+35 4488 Pe* 21 20 25.9123354680 +36 25 31.332306036   9.97 9.83     ~ 5 0
71 HD 203922 * 21 24 12.7419082800 +35 01 35.291909460   8.83 8.50     ~ 13 0
72 HD 206977 Pe* 21 44 54.4592545056 +36 11 26.441434176   9.20 8.98     A2IVSrSi 11 0
73 BD+46 3543 * 22 02 12.7264523232 +47 05 25.255324860   9.97 9.75     ~ 7 0
74 UCAC4 686-113414 * 22 02 15.4293535158 +47 05 16.593430718   13.513 12.997 13.019   ~ 1 0
75 BD+52 3124 Pe* 22 09 16.4409592536 +52 43 14.772558180   10.22 10.12     ~ 5 0
76 BD+54 2730 * 22 17 45.9688034136 +55 38 01.154673744   10.72 10.46     ~ 8 0
77 BD+57 2636 SB* 22 53 56.5847080752 +58 15 44.242099488   9.96 9.55     Ap 7 0
78 HD 240242 Pe* 23 16 25.7769721080 +58 19 16.428580680   10.71 10.15     ~ 6 0
79 V* V436 Cas a2* 23 32 47.6484957000 +57 54 20.112470496   7.72 7.55     A0p 115 0
80 HD 222416 * 23 40 12.1541949096 +45 04 25.134585024   7.77 7.73     ~ 20 0
81 BD+35 5094 Pe* 23 46 36.7182649536 +36 06 51.452946396   9.50 9.08     F2VFe-0.6Sr 8 0
82 BD+61 2565 Pe* 23 54 55.6814554224 +62 04 22.262228940   10.27 9.9     ApSrCrEu 9 0

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