Table 2.
Periods found in the observational intervals: sequentially TESS-21a, TESS-21b, Kazan-22, TESS-23a, and TESS-23b. The periods in different intervals are divided by double lines.
Period, day | Frequency (d−1) | Aa (mag) | Interpretation |
---|---|---|---|
0.13756(5) | 7.269(3) | 0.006 | ≈νorb |
0.132919(6) | 7.5234(3) | 0.046 | ν− |
0.15114(4) | 6.616(2) | 0.009 | ν+ |
1.1045(6) | 0.9054(5) | 0.028 | ν− − ν+ |
3.99 | 0.250 | 0.01 | ≈νpr− |
0.13755(6) | 7.270(3) | 0.006 | ≈νorb |
0.132903(6) | 7.5243(4) | 0.049 | ν− |
0.15107(3) | 6.620(1) | 0.012 | ν+ |
1.1085(8) | 0.9021(7) | 0.023 | ν− − ν+ |
4.32 | 0.2315 | 0.017 | ≈νpr− |
1.83 | 0.545 | 0.015 | ν1 |
2.75 | 0.364 | 0.017 | ν2 |
0.132740(6) | 7.5335(3) | 0.065 | ν− |
0.15232(2) | 6.5651(10) | 0.033 | ν+ |
1.83 | 0.547 | 0.02 | ν1 |
2.95 | 0.339 | 0.03 | ν2 |
1.03 | 0.968 | 0.017 | ν− − ν+ |
0.13374(1) | 7.4771(6) | 0.019 | ν− |
4.10 | 0.244 | 0.074 | ≈νpr− |
0.13380(6) | 7.4741(32) | 0.009 | ν− |
4.10 | 0.244 | 0.045 | ≈νpr− |
1.88 | 0.531 | 0.053 | ν1 |
2.73 | 0.366 | 0.062 | ν2 |
2.08 | 0.482 | 0.051 | ν3 |
Notes:νorb is the orbital frequency and corresponding period found earlier spectroscopically (Cowley et al. 1975); νpr− is the frequency corresponding to the nodal precession period; ν− is the frequency of the negative superhumps; ν+ is the frequency of the positive superhumps. Here, a is amplitude of the sinusoid that best fits the folded light curve.
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