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Table 1.

Long-period Ap stars found by our technique in the TESS Sectors 1–13 data, obtained in the first year of mission operations and covering the southern ecliptic hemisphere.

Specrtral TESS
HD TIC type V Teff log g roAp Bzrms/B0/Q0 Refs. Prot Refs. Lines (a) Refs. notes Sectors
(mag) (K) (cm s−2) (kG) (d)
12932 268751602 Ap SrCrEu 10.17 7319 roAp 1.0/–/– 3 s 8/C BN Cet; Nd III 6145 strong S3
18610 280051011 A2p CrEuSr 8.17 7994 3.76 –/5.7/– 1 r 1 S2,13
19918 348717688 Ap SrEuCr 9.35 7793 4.06 roAp 0.8/–/– 3, 4 vs 8/C BT Hyi; Nd III 6145 strong S1,12-13
27472 38586127 Ap Sr 9.96 7309 3.93 b 8/F S1-5,8-12
29578 220399820 A4p SrEuCr 8.52 7520 3.80 0.8/3.1/3.8 1 > 5 yr 1 r 1 S5,9
33629 77743907 Ap SrCr(Eu) 9.03 7266 3.90 –/4.8/– 1 r 1 S5
42075 37354067 Ap EuCrSr 8.98 7225 3.82 –/8.5/– 1 r 1 S6
44226 38000192 A3p SrCrEu 9.46 7707 3.86 –/5.0/– 1 r 1 S6
44979 124988213 Ap Si 6.53 12 593 Possible Prot = 3.3 d; A = 17 μmag S6,7
50169 282101454 A3p SrCrEu 8.99 9556 3.75 1.3/5.1/6.4 1, 2 10 600 7 r 1 S6
50345 237564008 Ap EuCr 9.70 10 026 4.22 One δ Sct peak; ν = 13.5469 d−1 S6
51684 156913148 F0p SrEuCr 7.96 8747 1.4/6.0/6.6 1 371 7 r 1 S6-7
52280 167751145 Ap SrCrEu 9.82 7621 3.80 vb 8/F S1-8,10-13
52847 80283159 Ap CrEu(Sr) 8.13 8126 3.71 –/4.4/– 1 r 1 S7
53722 177813458 Ap EuCr(Sr) 9.02 7658 4.04 S7
59071 49927077 Ap Si 9.55 10 127 4.13 S7
59435 6176523 A6IIIp Sr 7.97 6599 –/3.0/– 1 1360 7 r 1 SB2 S7
61468 110709971 A3p EuCr 9.85 9413 4.10 1.9/6.8/6.4 1 322 7 r 1 S7
62261 280577153 Ap Si 9.74 10 488 4.05 S7
62746 333819119 A0V (+ApSi) 9.11 9427 S7
66821 341550034 Ap Si 9.99 10 092 4.27 154.9 7 S7-9
67337 133771486 Ap Si 10.10 S7-8
67658 80486647 Ap Si 9.76 12 018 S7,9
69013 125297016 A2p SrEu 9.56 7013 3.98 roAp –/4.8/– 1 r 1 S7
69578 307031171 F6III Sr 9.56 S1-2,5-6,8-12
69638 218710779 Ap EuCr 9.43 8154 4.24 vb 8/F S7-8
71376 50753571 A Si 9.71 11 191 4.11 S7
76021 355850109 A Si 10.34 11 474 S9-11
76460 356088697 A3p Sr 9.80 7111 3.52 roAp –/3.6/– 1 r 1 δ Sct? ν = 55.87 d−1; A = 57 μmag S9-11
77438 401242170 Ap EuCrSr 10.07 9944 4.14 s 8/F S9
85284 444094235 Ap EuCr(Sr) 9.82 13640 s 8/F S9-10
85564 131725540 Ap (SiCrSr) 9.54 7667 4.10 vb 8/F S9-10
85766 48330947 Ap (SiCr) 9.98 7428 4.09 δ Sct, 31–35 d−1; three peaks S9
88241 72802368 F0p SrEu 8.60 7038 3.69 –/3.6/– 1 r 1 Possible roAp; 5σ 104.8 d−1 S9
89075 168274937 A (pEu) 8.53 10 584 3.85 vb 8/F Maybe Am S9
90131 73765625 Ap EuCr(Sr) 9.49 8387 3.65 S9
92499 146715928 A2p SrEuCr 8.93 7732 3.98 roAp 1.1/8.3/– 1 > 5 yr? 1 r 1 S9-10
93507 398501076 Ap SiCr pec 8.46 9760 4.01 2.2/7.2/7.7 1 556 7 r 1 S10-11
95811 461161123 Ap SrCrEu 9.56 6925 3.77 S9
97132 81554659 Ap SrCrEu 9.84 9257 3.83 S10
106322 334505323 Ap EuCr 9.39 7683 3.65 S10
119027 49332521 Ap SrEu(Cr) 9.92 6936 3.98 roAp 0.5/3.2/3.7 1 r 1 LZ Hya S11
133792 454802988 Ap SrCrEu 6.25 9700 3.61 –/–/1.1 1 vs 8/C Some g modes? S12
135396 455599747 Ap (SrCr) 7.99 6820 3.44 s 8/C S12
139850 65313788 Ap Si 10.27 8187 S12
141668 281965562 Ap Si 9.61 S12
147516 223456276 Ap Si 10.09 9446 3.71 S12
150562 44827786 A/F (pEu) 9.91 7348 4.08 roAp 1.2/4.9/5.7 1 r 1 νrot = 0.19 d−1? S12
151860 170419024 Ap SrEu(Cr) 9.01 6625 3.75 roAp s 8/F S12
156808 196639668 Ap EuCr 8.65 5816 b 8/F Peak at 3.465 d−1; g mode? S12
163231 260084368 Ap Si 9.63 12 369 νrot = 0.306 d−1? S13
171420 291561579 Ap Si 10.67 6793 4.33 S13
176196 387132889 Ap EuCr(Sr) 7.51 11 711 4.27 0.2/–/– 3 vs 8/C S13
185204 369871758 Ap SrEuCr 9.53 7666 3.85 –/5.6/– 1 r 1 νrot = 0.080 d−1? S13
209364 206461701 Ap SrCrEu 10.03 7188 3.57 S1
213637 69855370 F1p EuSr 9.65 6607 4.08 roAp 0.2/5.2/5.4 1 r 1 MM Aqr S2
217522 139191168 Ap SrSi: 7.54 6918 4.02 roAp 0.8/–/2.0 3, 4, 5, 6 vs 8/C BP Gru; Nd III 6145 strong S1
217704 12968953 Ap Sr 10.17 7883 3.94 roAp mr 8/C S2
225234 266905315 A3V 8.87 8084 4.27 S1,13
J0651 (b) 167695608 F0p SrEu(Cr) 11.51 7185 4.05 roAp s 8/H S1-4,6-13

Notes. Since all but one of the stars have an HD number, and these stars are known in the literature by their HD numbers, we have chosen to order the table by those in Col. 1. Column 2 gives the TESS Input Catalogue (TIC) number. Column 3 gives spectral classifications; all of those are some type of Ap star, since that was a selection criterion. Columns 4–6 give V, Teff, and log g where there are estimates of those available. The uncertainties of Teff and log g are likely to be 100s K and up to 0.3 dex, respectively; we have not rounded the values taken from the compilations to reflect these uncertainties. The data in Cols. 3–6 were taken from the TIC (version 8.0) or SIMBAD compilations. Column 7 indicates whether a star is a known roAp star. Column 8 gives information about the measured magnetic field strengths. All three values correspond to the mean over a rotation period (if known) or over the existing observations (otherwise) of the range spanned by each of the following magnetic field moments: ⟨Bzrms is the root-mean-square longitudinal field, as defined by Bohlender et al. (1993). It is essentially the quadratic mean of the mean longitudinal magnetic field. Since the latter is a signed quantity, and may reverse its sign over a rotation cycle, taking the quadratic mean is the way to avoid cancellation and to define a parameter that characterises the actual strength of the longitudinal field. We denote by B0 the average value over a rotation cycle of the mean magnetic field modulus ⟨B⟩; this is the same quantity as listed in Col. 3 of Table 13 of Mathys (2017). The notation Q0 refers to the average value over a rotation cycle of the mean quadratic magnetic field ⟨Bq⟩; this is the same quantity as listed in Col. 10 of Table 13 of Mathys (2017). Column 10 gives measurements for the stellar rotation periods, with the following column giving the references for those; the references are for compilations, where the original source reference can be found. Column 12 gives a comment on the width and the magnetic resolution of the spectral lines, from the source identified in Col. 13 (see text). Column 14, the penultimate column, gives various notes, including variable star names, primarily for the roAp stars, since the stars studied here, by definition, do not show rotational variation and hence are not α2 CVn stars; that column also notes that some of these stars show δ Sct variations. The final column indicates in which TESS 27 d sectors the star was observed.

(a)

r = resolved; mr = marginally resolved; s = sharp; vs = very sharp; b = broad; vb = very broad.

(b)

J0651 = J06514218−6325495.

References. (1) Mathys (2017); (2) Mathys et al. (2019a); (3) Bagnulo et al. (2015); (4) Mathys & Hubrig (1997); (5) Medupe et al. (2015); (6) Hubrig et al. (2002); (7) Mathys (2019); (8) this paper (8/C: based on ESO-CES spectra; 8/F: based on ESO-FEROS spectra; 8/H: based on SALT-HRS spectrum).

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