Table 6
Parameters from the Fourier decomposition.
| # | A 0 | A 1 | A 2 | A 3 | A 4 | φ 21 | φ 31 | φ 41 | N | D m |
|
|
||||||||||
| RR0 | ||||||||||
|
|
||||||||||
| V1 | 15.121(2) | 0.337(2) | 0.160(2) | 0.110(2) | 0.050(2) | 4.045(12) | 8.498(16) | 6.581(22) | 7 | 2.6 |
| V2a | 15.196(2) | 0.320(2) | 0.134(2) | 0.107(2) | 0.081(2) | 4.005(11) | 8.511(15) | 6.668(16) | 7 | 3.0 |
| V3 | 15.118(2) | 0.319(2) | 0.152(2) | 0.112(2) | 0.059(2) | 3.973(11) | 8.413(13) | 6.468(19) | 7 | 4.9 |
| V15 | 15.067(2) | 0.344(2) | 0.181(2) | 0.122(1) | 0.081(2) | 3.987(7) | 8.274(12) | 6.431(14) | 10 | 2.5 |
|
|
||||||||||
| RR1 | ||||||||||
|
|
||||||||||
| V14 | 15.176(2) | 0.214(3) | 0.030(3) | 0.012(2) | 0.010(2) | 4.773(26) | 2.673(137) | 2.338(104) | 6 | − |
Notes.A good decomposition could not be obtained for V19, due to poor phase coverage; the Fourier fit to V2 was also poor, and V16 is excluded because it shows signs of amplitude and period modulation due to Blazhko effects or non-radial pulsation. Numbers in parentheses are the 1-σ uncertainties on the last decimal place.
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