Table 3: Results of the Fourier analysis performed on the 1993 and 1995 data. The frequencies f_i are in d^-1, the amplitude K_i in km s^-1 and the phases $\varphi _i$ in fractions of a day. The zero points are HJD 2 449 201.4558 for the 1993 data and HJD 2 449 969.3337 in 1995. The residuals are respectively 0.47 and 0.40 km s^-1.
1993 1995

f_i K_i $\varphi _i$ f_i K_i $\varphi _i$

f₁ 6.591 3.57 0.896 6.589 3.31 0.059

$\pm3$ $\pm11$ $\pm5$ $\pm1$ $\pm9$ $\pm4$

f₂ 0.659 1.60 0.452 0.670 1.37 0.231

$\pm6$ $\pm11$ $\pm11$ $\pm3$ $\pm9$ $\pm10$

f₃ 0.840 0.80 0.213 0.872 1.57 0.704

$\pm11$ $\pm11$ $\pm22$ $\pm3$ $\pm9$ $\pm9$

f₄ 5.993 0.41 0.331 6.019 0.47 0.584

$\pm21$ $\pm11$ $\pm44$ $\pm8$ $\pm9$ $\pm29$

**Table 3:** Results of the Fourier analysis performed on the 1993 and 1995 data. The frequencies f_i are in d^-1, the amplitude K_i in km s^-1 and the phases $\varphi _i$ in fractions of a day. The zero points are HJD 2 449 201.4558 for the 1993 data and HJD 2 449 969.3337 in 1995. The residuals are respectively 0.47 and 0.40 km s^-1.
	1993	1995
	f_i	K_i	$\varphi _i$	f_i	K_i	$\varphi _i$
f₁	6.591	3.57	0.896	6.589	3.31	0.059
	$\pm3$	$\pm11$	$\pm5$	$\pm1$	$\pm9$	$\pm4$
f₂	0.659	1.60	0.452	0.670	1.37	0.231
	$\pm6$	$\pm11$	$\pm11$	$\pm3$	$\pm9$	$\pm10$
f₃	0.840	0.80	0.213	0.872	1.57	0.704
	$\pm11$	$\pm11$	$\pm22$	$\pm3$	$\pm9$	$\pm9$
f₄	5.993	0.41	0.331	6.019	0.47	0.584
	$\pm21$	$\pm11$	$\pm44$	$\pm8$	$\pm9$	$\pm29$

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