Table 1
Observations log of the RR Lyr spectra around the maximum luminosity.
Night | Obs. | N | Texp | Ψ | φemi | S/N | Vshock | I(%) | I(%) |
---|---|---|---|---|---|---|---|---|---|
(yyyy-mm-dd) | (s) | Blazhko | pulsation | (km s−1) | Hα | HeI D3 | |||
1994-08-03 | OHP | 26 | 450–480 (480) | 0.44 | 0.956 | 55 | 111 | 20 | 4 |
1994-08-04 | OHP | 35 | 420–600 (480) | 0.47 | 0.931 | 36 | – | [18] | [0] |
1995-08-07 | OHP | 18 | 300–480 (360) | 0.86 | 0.890 | 22 | 131 | – | 0 |
1995-08-08 | OHP | 32 | 300–540 (540) | 0.89 | 0.877 | 37 | – | 4 | 0 |
1995-09-05 | OHP | 48 | 180–600 (360) | 1.60 | 0.915 | 27 | – | 7 | 6 |
1995-10-17 | OHP | 38 | 300 | 2.67 | 0.890 | 32 | 128 | 22 | 0 |
1996-06-24 | OHP | 30 | 300–500 (500) | 0.12 | 0.882 | 34 | 122 | 27 | (2) |
1996-06-25 | OHP | 34 | 240–540 (420) | 0.15 | 0.873 | 48 | 119 | 18 | 0 |
1996-08-01 | OHP | 56 | 180–360 (300) | 1.10 | 0.876 | 31 | 143 | 33 | 3 |
1996-08-02 | OHP | 20 | 420–600 (600) | 1.12 | 0.870 | 24 | 131 | 28 | 3 |
1996-08-11 | OHP | 36 | 420–600 (480) | 1.36 | 0.907 | 33 | 120 | 29 | 5 |
1997-05-30 | OHP | 28 | 300–600 (420) | 0.95 | 0.877 | 11 | 135 | – | 0 |
1997-06-11 | OHP | 38 | 180–300 (180) | 1.26 | 0.887 | 24 | 129 | 33 | 1 |
1997-08-05 | OHP | 37 | 300–480 (300) | 2.66 | 0.896 | 39 | 139 | 40 | 8 |
1997-08-06 | OHP | 58 | 300 | 2.69 | 0.898 | 29 | 134 | 40 | 8 |
1997-08-09 | OHP | 48 | 300–480 (300) | 2.76 | 0.883 | 26 | 149 | 25 | 4 |
1997-08-10 | OHP | 38 | 300–600 (300) | 2.79 | 0.885 | 15 | 146 | 24 | 0 |
1997-08-30 | OHP | 65 | 300 | 3.30 | 0.884 | 36 | 124 | 21 | 5 |
1997-08-31 | OHP | 60 | 180–300 (240) | 3.33 | 0.881 | 29 | 121 | 27 | 0 |
2013-10-12 | Ouka | 40 | 300 | 0.16 | 0.922 | 13 | 117 | 43 | 7 |
2015-10-29 | Ouka | 58 | 300 | 0.33 | 0.921 | 19 | – | 34 | 3 |
2015-11-06 | Ouka | 23 | 300 | 0.53 | 0.917 | 26 | 119 | 31 | 3 |
2015-11-10 | Ouka | 43 | 300 | 0.63 | 0.919 | 17 | – | 32 | 7 |
2015-11-11 | Ouka | 32 | 300 | 0.66 | 0.915 | 5 | – | 27 | 3 |
2015-11-14 | Ouka | 48 | 300 | 0.74 | 0.920 | 6 | – | 44 | (2) |
2015-11-19 | Ou8a | 49 | 300 | 0.86 | 0.922 | 9 | – | 44 | 5 |
2015-11-27 | Ouka | 40 | 300 | 1.07 | 0.919 | 6 | – | 38 | 0 |
2015-12-01 | Ouka | 39 | 300 | 1.17 | 0.920 | 8 | – | 41 | (3) |
2015-12-14 | Ouka | 23 | 300 | 1.50 | 0.921 | 5 | – | 34 | (2) |
2015-12-18 | Ouka | 22 | 300 | 1.61 | 0.920 | 11 | 126 | 37 | (3) |
Notes. When the quality of the data allowed to determine the shock velocity, the nights are marked in bold. Columns provide the date of the night, the observatory (Obs.), the number, N, of observed spectra, the exposure time, Texp, or the range of exposure time used during the night. The value in parenthesis is the exposure time corresponding to the spectrum of the maximum of Hα. Then, the corresponding Blazhko phase, Ψ, of the night, the pulsation phase φemi of the maximum of the emission of Hα called “the first apparition”, the estimated S/N per pixel with 2σ around 6557 Å over 2.5 Å, the maximum shock velocity (km s−1) near φ ≃ 0.9 and the maximum intensity of the Hα and He I D3 emission components with respect to the continuum. When the intensity number is in parenthesis, it means that the presence of the emission is doubtful in terms of the noise level or continuum; when it is equal to zero, no emission was observed. When I is in square brackets, it means that the spectrum on which their measurements are made is either the first or the last of the night and therefore may not match at the maximum value.
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