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Table A.1.

Measurements of the spectra of the ssrAp star candidates.

TIC Other ID V HJD Instr S/N Teff vr σ(vr) B σ(⟨B⟩) Ng Bq σ(⟨Bq⟩) Nl (v sin i)max σ(v sin i)
(2, 400, 000.+) (K) (km s−1) (km s−1) (G) (G) (G) (G) (km s−1) (km s−1)
32259138 HD 138777 9.73 60432.570 S 150 7352 -43.72 0.12 4698 100 3 5600 300 46
88202438 HD 192686 8.88 60540.457 N 85 11670 -10.30 0.05 3573 50 2 4730 230 64
93522454 HD 143487 9.43 54140.822 F 170 7114 4216 100 3 3940 780 21 5.8 0.8
54173.913 U 180 -23.36 0.69 4153 60 3 2630 920 17 7.5 1.4
54535.850 U 135 -14.00 0.79 4111 60 3 2890 750 17 7.5 1.4
54536.815 U 225 -14.24 0.71 4111 60 3 3280 630 17 7.5 1.4
55374.730 U 325 -25.20 0.99 4195 60 3 3330 760 14 7.5 1.4
55609.836 H 50 -22.27 0.47 4006 100 3 19 6.9 1.3
60032.483 S 220 -18.11 0.41 4467 100 3 4330 1350 18 5.8 1.3
163801263 HD 203922 8.50 60539.473 N 75 7602 -23.92 0.05 3503 30 2 3830 120 78 2.9 0.2
170419024 HD 151860 9.01 55326.858 U 390 6625 3.45 0.07 2265 40 2 2580 170 26 4.2 0.3
238659021 HD 8441 6.68 60686.361 N 160 9205 3.68 0.03 64 3.1 0.2
251976407 HD 221568 7.55 60686.313 N 125 9472 -8.33 0.12 2433 30 2 2790 250 38
301918605 HD 17330 7.11 60686.421 N 240 10250 -12.42 0.03 1130 180 72 1.4 0.1
341616734 HD 89069 8.42 60663.707 N 100 9546 -9.23 0.10 3380 120 83 4.3 0.2
60686.678 N 100 -9.17 0.05 3200 90 78 4.8 0.1
352787151 BD+35 5094 9.08 60686.350 N 85 6900 -6.81 0.05 85 2.0 0.2
356088697 HD 76460 9.80 55227.707 F 270 7110 3607 40 2 3890 260 64 4.0 0.3
60038.395 S 210 2.20 0.11 3586 50 2 3350 340 60 3.9 0.4
369969602 HD 128472 9.87 60484.425 S 210 7259 -16.94 0.15 1840 570 46 3.3 0.4
380607580 HD 119794 9.00 60704.562 S 145 9347 -21.49 0.16 5369 40 2 4800 400 47 6.1 0.5
403625657 HD 11187 7.94 60539.704 N 65 10750 5.73 0.06 49 15.3 0.1
405516045 HD 110274 9.47 54138.884 F 180 7766 3775 40 3 3580 440 39 2.5 0.5
54141.828 F 100 -1.43 0.10 3754 40 3 3350 370 42 4.1 0.4
54172.906 U 150 -7.75 0.08 5034 30 2 6320 150 33
54523.854 U 115 -2.97 0.08 4698 30 2 6000 170 33
54535.815 U 170 -4.94 0.09 4425 30 2 5670 200 33 1.5 0.5
60032.587 S 250 -1.49 0.14 5243 40 2 5850 260 38 3.2 0.4
419916333 HD 117290 9.25 54139.763 F 160 7271 6439 40 2 7320 330 21
54141.866 F 130 -27.57 0.23 6313 40 2 7540 310 22
54171.921 U 120 -26.97 0.16 6334 30 2 7650 260 27
54515.870 U 250 -4.47 0.15 4509 30 2 6550 270 27
60036.350 S 260 -36.87 0.20 3020 40 2 2630 630 34 2.2 0.7
430355895 BD+52 3124 10.12 60540.656 N 50 9066 -10.94 0.07 4237 50 2 4920 170 55 2.3 0.4
470837956 BD+61 2565 9.9 60555.089 N 200 8178 -17.89 0.06 1680 140 111 2.4 0.2

Notes. The stars are listed in order of increasing TIC (TESS Input Catalogue) number (Col. 1), with another ID (preferably the HD number) given in Col. 2 and the V magnitude in Col. 3. The Heliocentric Julian Date (HJD) of mid-observation, the instrument with which it was obtained (F = FEROS; H = HARPS; N = HARPS-N; S = SALT-HRS; U = UVES), and the resulting S/N appear in Cols. 4 to 6. The values of Teff in Col. 7 are from the TIC (they are listed as published there even though effective temperatures cannot be determined with 1 K precision). The following columns contain the results of our measurements: the stellar radial velocity vr and its uncertainty σ(vr) (Cols. 8 and 9; the entries were left blank when these values could not be determined); the mean magnetic field modulus ⟨B⟩, its uncertainty σ(⟨B⟩), and the number Ng of Gaussians fitted to the Fe II λ 6149.2 Å line for its determination (Cols. 10 to 12); the mean quadratic magnetic field ⟨Bq⟩, its formal uncertainty σ(⟨Bq⟩), and the number Nl of diagnostic lines from which it was derived (Cols. 13 to 15); the upper limit (v sin i)max of the projected equatorial velocity and the formal uncertainty σ(v sin i) of the v sin i determination (Cols. 16 and 17). The values of the radial velocity and of the projected equatorial velocity are derived from analysis of the same sample of Nl lines as used for the ⟨Bq⟩ determination. For spectra in which the Fe II λ 6149.2 Å line is not resolved into its magnetically split components, the entries in Cols. 8 to 10 are left blank; a dash (‘–’) in Col. 11 identifies those spectra in which the mean quadratic magnetic field is below the detection threshold, and in Col. 14, those spectra in which the rotational Doppler broadening is below the detection threshold. (For TIC 93522454, the ⟨Bq⟩ value derived from the first UVES spectrum was given as it is only marginally below the formal detection threshold and as significant values of similar order were determined from the other UVES observations of this star.)

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