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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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