Table 4: Frequencies $\nu$ , periods $\nu ^{-1}$ , maximum power $P_{\rm max}$ , significance levels p, and latitudes $\vartheta$ (where the power exceeds the given significance level) for the labeled regions in Figs. 8a-8d (cycle 21). The columns on the left give the values for the net magnetic flux, the columns on the right the values for the total magnetic flux. The error $\Delta \nu=1.5~{\rm nHz}$ is half the frequency resolution. The time intervals were determined using the $99.0\%$ significance contours of Morlet wavelets with nondimensional frequency 18 (cf. Sect. 2.2).
$\nu$ (nHz) $\nu ^{-1}$ (d) $P_{\rm max}$ p (%) $\vartheta$ Time $\nu$ (nHz) $\nu ^{-1}$ (d) $P_{\rm max}$ p (%) $\vartheta$ Time

${\rm N}_{21}$ 399.7 29.0 0.2 99.9 $40\hbox{$^\circ$ }{\rm S}$ - $55\hbox{$^\circ$ }{\rm S}$ 78.9-80.3 ${\rm n}'_{21}$ 399.7 29.0 0.3 99.9 $37\hbox{$^\circ$ }{\rm S}$ - $50\hbox{$^\circ$ }{\rm S}$ 82.0-82.8

${\rm O}_{21}$ 399.7 29.0 0.4 99.9 $40\hbox{$^\circ$ }{\rm N}$ - $53\hbox{$^\circ$ }{\rm N}$ 78.3-79.5 ${\rm o}'_{21}$ 399.7 29.0 0.03 99.9 $57\hbox{$^\circ$ }{\rm N}$ - $59\hbox{$^\circ$ }{\rm N}$ 82.0-83.3

82.4-83.5

${\rm R}_{21}$ 412.0 28.1 2.3 99.9 $18\hbox{$^\circ$ }{\rm S}$ - $72\hbox{$^\circ$ }{\rm S}$ 78.5-82.4 ${\rm R}'_{21}$ 412.0 28.1 10.0 99.9 $12\hbox{$^\circ$ }{\rm S}$ - $20\hbox{$^\circ$ }{\rm S}$ 81.0-82.3

${\rm S}'_{1,21}$ 421.3 27.5 8.9 99.9 $10\hbox{$^\circ$ }{\rm S}$ - $13\hbox{$^\circ$ }{\rm S}$ 80.4-81.4

84.0-84.6

${\rm T}_{2,21}$ 430.5 26.9 1.9 99.9 $12\hbox{$^\circ$ }{\rm N}$ 79.6-81.0 ${\rm T}'_{2,21}$ 430.5 26.9 9.2 99.9 $5\hbox{$^\circ$ }{\rm S}$ - $27\hbox{$^\circ$ }{\rm N}$ 82.0-83.0

430.5 26.9 2.0 99.0 $16\hbox{$^\circ$ }{\rm N}$ - $18\hbox{$^\circ$ }{\rm N}$ 80.4-81.2 83.9-84.5

433.6 26.7 3.2 99.9 $0\hbox{$^\circ$ }{\rm N}$ - $4\hbox{$^\circ$ }{\rm N}$ 79.1-80.3

80.7-81.7

85.6-86.4

${\rm U}'_{2,21}$ 461.2 25.1 5.0 99.0 $14\hbox{$^\circ$ }{\rm S}$ - $19\hbox{$^\circ$ }{\rm S}$ 80.8-81.7

${\rm v}'_{21}$ 415.1 27.9 6.0 99.9 $13\hbox{$^\circ$ }{\rm N}$ - $14\hbox{$^\circ$ }{\rm N}$ 81.9-82.6

${\rm T}^{*}_{2,21}$ 861.0 13.44 4.4 99.9 $14\hbox{$^\circ$ }{\rm N}$ - $18\hbox{$^\circ$ }{\rm N}$ 79.2-79.9 ${\rm T'}^{*}_{2,21}$ 867.1 13.35 15.8 99.9 $4\hbox{$^\circ$ }{\rm S}$ - $17\hbox{$^\circ$ }{\rm N}$ 79.2-79.9

80.4-80.7 81.2-82.8

867.1 13.35 2.9 99.9 $5\hbox{$^\circ$ }{\rm N}$ - $13\hbox{$^\circ$ }{\rm N}$ 80.9-81.7 84.0-84.3

82.7-83.2 85.7-86.0

**Table 4:** Frequencies $\nu$ , periods $\nu ^{-1}$ , maximum power $P_{\rm max}$ , significance levels p, and latitudes $\vartheta$ (where the power exceeds the given significance level) for the labeled regions in Figs. 8a-8d (cycle 21). The columns on the left give the values for the net magnetic flux, the columns on the right the values for the total magnetic flux. The error $\Delta \nu=1.5~{\rm nHz}$ is half the frequency resolution. The time intervals were determined using the $99.0\%$ significance contours of Morlet wavelets with nondimensional frequency 18 (cf. Sect. 2.2).
	$\nu$ (nHz)	$\nu ^{-1}$ (d)	$P_{\rm max}$	p (%)	$\vartheta$	Time		$\nu$ (nHz)	$\nu ^{-1}$ (d)	$P_{\rm max}$	p (%)	$\vartheta$	Time
${\rm N}_{21}$	399.7	29.0	0.2	99.9	$40\hbox{$^\circ$ }{\rm S}$ - $55\hbox{$^\circ$ }{\rm S}$	78.9-80.3	${\rm n}'_{21}$	399.7	29.0	0.3	99.9	$37\hbox{$^\circ$ }{\rm S}$ - $50\hbox{$^\circ$ }{\rm S}$	82.0-82.8
${\rm O}_{21}$	399.7	29.0	0.4	99.9	$40\hbox{$^\circ$ }{\rm N}$ - $53\hbox{$^\circ$ }{\rm N}$	78.3-79.5	${\rm o}'_{21}$	399.7	29.0	0.03	99.9	$57\hbox{$^\circ$ }{\rm N}$ - $59\hbox{$^\circ$ }{\rm N}$	82.0-83.3
						82.4-83.5
${\rm R}_{21}$	412.0	28.1	2.3	99.9	$18\hbox{$^\circ$ }{\rm S}$ - $72\hbox{$^\circ$ }{\rm S}$	78.5-82.4	${\rm R}'_{21}$	412.0	28.1	10.0	99.9	$12\hbox{$^\circ$ }{\rm S}$ - $20\hbox{$^\circ$ }{\rm S}$	81.0-82.3
							${\rm S}'_{1,21}$	421.3	27.5	8.9	99.9	$10\hbox{$^\circ$ }{\rm S}$ - $13\hbox{$^\circ$ }{\rm S}$	80.4-81.4
													84.0-84.6
${\rm T}_{2,21}$	430.5	26.9	1.9	99.9	$12\hbox{$^\circ$ }{\rm N}$	79.6-81.0	${\rm T}'_{2,21}$	430.5	26.9	9.2	99.9	$5\hbox{$^\circ$ }{\rm S}$ - $27\hbox{$^\circ$ }{\rm N}$	82.0-83.0
	430.5	26.9	2.0	99.0	$16\hbox{$^\circ$ }{\rm N}$ - $18\hbox{$^\circ$ }{\rm N}$	80.4-81.2							83.9-84.5
								433.6	26.7	3.2	99.9	$0\hbox{$^\circ$ }{\rm N}$ - $4\hbox{$^\circ$ }{\rm N}$	79.1-80.3
													80.7-81.7
													85.6-86.4
							${\rm U}'_{2,21}$	461.2	25.1	5.0	99.0	$14\hbox{$^\circ$ }{\rm S}$ - $19\hbox{$^\circ$ }{\rm S}$	80.8-81.7
							${\rm v}'_{21}$	415.1	27.9	6.0	99.9	$13\hbox{$^\circ$ }{\rm N}$ - $14\hbox{$^\circ$ }{\rm N}$	81.9-82.6
${\rm T}^{*}_{2,21}$	861.0	13.44	4.4	99.9	$14\hbox{$^\circ$ }{\rm N}$ - $18\hbox{$^\circ$ }{\rm N}$	79.2-79.9	${\rm T'}^{*}_{2,21}$	867.1	13.35	15.8	99.9	$4\hbox{$^\circ$ }{\rm S}$ - $17\hbox{$^\circ$ }{\rm N}$	79.2-79.9
						80.4-80.7							81.2-82.8
	867.1	13.35	2.9	99.9	$5\hbox{$^\circ$ }{\rm N}$ - $13\hbox{$^\circ$ }{\rm N}$	80.9-81.7							84.0-84.3
						82.7-83.2							85.7-86.0

Source LaTeX | All tables | In the text

	1 Introduction
	2 Data and reduction procedure
	3 The low frequency range 1 nHz ${\le \nu \le }$ 30 nHz
	4 The intermediate frequency range 30 nHz ${\le \nu \le }$ 120 nHz
	5 The high frequency range 390 nHz ${\le \nu \le }$ 470 nHz
	6 Possible r-mode signatures in the magnetic flux
	7 Conclusions
	References
	Online Material