Table 3: Radial heliocentric velocities and equivalent widths for $\lambda \lambda$ 6196 and 6283 ( $1\sigma$ rms-error in parenthesis). 3 $\sigma$ (=3.0 FWHM $\sigma _{\rm noise}$ ) upper limits for $\lambda \lambda$ 6379 and 6613. Uncertainties in $\lambda$ 6283 central velocity are of the order of 10 to 20 km $\ensuremath {\rm {s}^{-1}}$ .
6196 6283 6379 6613

Phase v w v w 3 $\sigma$ 3 $\sigma$

(days) (km $\ensuremath {\rm {s}^{-1}}$ ) (mÅ) (km $\ensuremath {\rm {s}^{-1}}$ ) (mÅ) (mÅ) (mÅ)

-2 1647 (1) 12 (2) $\sim$ 1677 160 (15) <13 <31

+14 1650 (1) 13 (2) $\sim$ 1656 180 (15) <11 <29

+61 1649 (1) 16 (3) $\sim$ 1639 190 (20) <25 <55

**Table 3:** Radial heliocentric velocities and equivalent widths for $\lambda \lambda$ 6196 and 6283 ( $1\sigma$ rms-error in parenthesis). 3 $\sigma$ (=3.0 *FWHM* $\sigma _{\rm noise}$ ) upper limits for $\lambda \lambda$ 6379 and 6613. Uncertainties in $\lambda$ 6283 central velocity are of the order of 10 to 20 km $\ensuremath {\rm {s}^{-1}}$ .
	6196	6283	6379	6613
Phase	v	w	v	w	3 $\sigma$	3 $\sigma$
(days)	(km $\ensuremath {\rm {s}^{-1}}$ )	(mÅ)	(km $\ensuremath {\rm {s}^{-1}}$ )	(mÅ)	(mÅ)	(mÅ)
-2	1647 (1)	12 (2)	$\sim$ 1677	160 (15)	<13	<31
+14	1650 (1)	13 (2)	$\sim$ 1656	180 (15)	<11	<29
+61	1649 (1)	16 (3)	$\sim$ 1639	190 (20)	<25	<55

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