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Table 1.

Known ssrAp stars.

HD/HDE Other ID Spectral type Prot (d) Reference B0 (kG) roAp

Stars with accurately determined periods
50169 BD−1 1414 A3p SrCrEu 10600 Mathys et al. (2019a) 5.1
9996 HR 465 B9p CrEuSi 7937 Metlova et al. (2014) 4.7
965 BD−0 21 A8p SrEuCr 6030 Mathys et al. (2019b) 4.3
166473 CoD−37 12303 A5p SrEuCr 3836 Mathys et al. (2020a) 7.1 roAp
94660 HR 4263 A0p EuCrSi 2800 Mathys (2017) 6.2
187474 HR 7552 A0p EuCrSi 2345 Mathys (1991) 5.4
(a) CPD−62 2717 B8 (b) 1765 Chojnowski et al. (2023) 9.9
59435 BD−8 1937 A4p SrCrEu 1360 Wade et al. (1999) 3.0
18078 BD+55 726 A0p SrCr 1358 Mathys et al. (2016) 3.4
93507 CPD−67 1494 A0p SiCr 556 Mathys et al. (1997) 7.2
2453 BD+31 59 A1p SrEuCr 518.2 Pyper & Adelman (2017) 3.7
51684 CoD−40 2796 F0p SrEuCr 371 Mathys (2017) 6.0
61468 CoD−27 4341 A3p EuCr 322 Mathys (2017) 6.8
110274 CoD−58 4688 A0p EuCr 265.3 Freyhammer et al. (2008) 4.0
69544 CD −50 3225 B8p Si 236.5 Bernhard et al. (2015a)
188041 HR 7575 A6p SrCrEu 223.78 Mathys (2017) 3.7
221568 BD+57 2758 A1p SrCrEu 159.10 Pyper & Adelman (2017)
66821 CPD−54 1483 A0p Si 154.9 Bernhard et al. (2015a)
116458 HR 5049 A0p EuCr 148.39 Mathys (2017) 4.7
126515 BD+1 2927 A2p CrSrEu 129.95 Mathys et al. (1997) 12.7
340577 BD+25 4289 A3p SrCrEu 116.7 Hümmerich et al. (2016)
263361 BD+19 1468 B9p Si 88.9 Bernhard et al. (2015a)
149766 CD−51 10384 B8p Si 87.3 Bernhard et al. (2015a)
(c) BD−7 1884 SrCrEu 75.97 Hümmerich et al. (2016)
158919 CPD−65 3465 B9p Si 75.72 Bernhard et al. (2015a)
102797 CPD−75 757 B9p Si 75.02 Koen & Eyer (2002)
8441 BD+42 293 A2p Sr 69.51 Pyper & Adelman (2017)
5797 BD+59 163 A0p CrEuSr 68.05 Dukes & Adelman (2018)
123335 HR 5292 Bp He wk SrTi 55.215 Hensberge et al. (2007)
103844 CPD−75 767 A0p Si 52.95 Bernhard et al. (2015a)
200311 BD+43 3786 B9p SiCrHg 52.0084 Wade et al. (1997) 8.4
256476 TYC 736-1842-1 A2p Si 51.23 Hümmerich et al. (2016)
184471 BD+32 3471 A9p SrCrEu 50.8 Kudryavtsev & Romanyuk (2012)
87528 CPD−62 1415 B8/9 III (d) 50.35 Bernhard et al. (2015a)

Stars with well-established period lower limits

201601 γ Equ A9p SrEu ≳35 500 Bychkov et al. (2016) 3.9 roAp
213258 BD+35 4815 B9p ≳18 000 Mathys et al. (2023) 3.8 roAp
116114 BD−17 3829 F0p SrCrEu > 17 700 Giarrusso et al. (2022) 6.0 roAp
101065 CD−46 7232 F3p Ho > 15 700 (e) Hubrig et al. (2018) roAp
55719 HR 2727 A3p SrCrEu > 14 000 Giarrusso et al. (2022) 6.3
177765 CD−26 13816 A5p SrEuCr > 13 500 Giarrusso et al. (2022) 3.4 roAp
137949 33 Lib F0p SrEuCr ≫10 000 Giarrusso et al. (2022) 4.7 roAp
165474 BD+12 3382B A7p SrCrEu > 9900 Giarrusso et al. (2022) 6.6
176232 10 Aql A6p Sr ≫4400 Sikora et al. (2019) roAp
29578 CD−54 902 A4p SrEuCr ≳4000 (f) Giarrusso et al. (2022) 3.1

Notes. Column 1 gives the HD number of the stars (when available) and Col. 2 another identification. The spectral types listed in Col. 3 are from Renson & Manfroid (2009), except when otherwise mentioned in a footnote. Columns 4 and 5 contain the value of the period, when it has been accurately determined, or its lower limit, and the corresponding literature source. For those stars whose spectral lines are resolved into their magnetically split components, the phase-averaged value B0 of the mean magnetic field modulus ⟨B⟩ (the line intensity weighted average over the visible stellar hemishphere of the modulus of the magnetic vector) appears in Col. 6. For stars for which the available ⟨B⟩ measurements sample the full rotation cycle well, B0 is the average of ⟨B⟩ over the rotation period; otherwise, it is an average over the observed phases. Most entries in Col. 6 are from Tables 13 and 14 of Mathys (2017); for a few stars, they are complemented by more recent data from Mathys et al. (2019a,b, 2020a, 2023), Giarrusso et al. (2022), and Chojnowski et al. (2023). Rapidly oscillating Ap (roAp) stars are identified in Col. 7.

(a)

TYC 8979-339-1.

(b)

Spectral type from Loden et al. (1976).

(c)

TYC 5395-1139-1.

(d)

Spectral type from Houk & Cowley (1975).

(e)

We adopted the time base covered by the ⟨Bz⟩ measurements as lower limit, not the heavily extrapolated value of 188 yr proposed by Hubrig et al. (2018).

(f)

See text.

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