Table 3: Frequencies $\nu$ , periods $\nu ^{-1}$ , maximum Power $P_{\rm max}$ , significance levels p, latitudes $\vartheta$ (where the power exceeds the given significance level) and cycles (when the corresponding oscillations occurred) for the labeled regions in Figs. 7a and 7b. The error $\Delta \nu=0.6~{\rm nHz}$ is half the frequency resolution.
$\nu$ (nHz) $\nu ^{-1}$ (d) $P_{\rm max}$ p (%) $\vartheta$ Cycle

${\rm N}$ 400.0 28.9 1.1 99.99 $27\hbox{$^\circ$ }{\rm S}$ - $58\hbox{$^\circ$ }{\rm S}$ 23

${\rm O}$ 401.1 28.9 0.4 99.99 $34\hbox{$^\circ$ }{\rm S}$ - $54\hbox{$^\circ$ }{\rm S}$ 21, 22, 23

${\rm P}$ 406.6 28.5 0.6 99.99 $28\hbox{$^\circ$ }{\rm S}$ - $54\hbox{$^\circ$ }{\rm S}$ 23

${\rm Q}$ 406.6 28.5 1.2 99.99 $26\hbox{$^\circ$ }{\rm N}$ - $57\hbox{$^\circ$ }{\rm N}$ 22

${\rm R}$ 411.0 28.2 1.1 99.99 $19\hbox{$^\circ$ }{\rm S}$ - $57\hbox{$^\circ$ }{\rm S}$ 21, 22

414.4 27.9 1.0 99.99 $22\hbox{$^\circ$ }{\rm S}$ - $23\hbox{$^\circ$ }{\rm S}$ 21, 22

${\rm S}_2$ 429.9 26.9 1.1 99.99 $16\hbox{$^\circ$ }{\rm S}$ 22

429.9 26.9 0.7 99.90 $19\hbox{$^\circ$ }{\rm S}$ - $21\hbox{$^\circ$ }{\rm S}$ 23

${\rm S}_3$ 434.3 26.7 1.2 99.99 $10\hbox{$^\circ$ }{\rm S}$ - $12\hbox{$^\circ$ }{\rm S}$ 23

437.6 26.5 0.6 99.90 $11\hbox{$^\circ$ }{\rm S}$ 23

${\rm T}_1$ 426.6 27.1 1.1 99.99 $23\hbox{$^\circ$ }{\rm N}$ - $25\hbox{$^\circ$ }{\rm N}$ 22

429.9 26.9 0.8 99.99 $11\hbox{$^\circ$ }{\rm N}$ - $12\hbox{$^\circ$ }{\rm N}$ 21, 22

429.9 26.9 0.9 99.90 $16\hbox{$^\circ$ }{\rm N}$ - $20\hbox{$^\circ$ }{\rm N}$ 21, 22

${\rm T}_2$ 433.2 26.7 0.6 99.99 $6\hbox{$^\circ$ }{\rm N}$ - $8\hbox{$^\circ$ }{\rm N}$ 21, 22

433.2 26.7 0.9 99.99 $11\hbox{$^\circ$ }{\rm N}$ - $12\hbox{$^\circ$ }{\rm N}$ 21, 22

${\rm T}_3$ 435.4 26.6 0.9 99.90 $14\hbox{$^\circ$ }{\rm N}$ - $15\hbox{$^\circ$ }{\rm N}$ 23

437.6 26.4 1.0 99.99 $16\hbox{$^\circ$ }{\rm N}$ 21, 22, 23

${\rm U}$ 463.1 25.0 0.5 99.00 $14\hbox{$^\circ$ }{\rm S}$ 22

${\rm M'}$ 398.9 29.0 2.3 99.90 $16\hbox{$^\circ$ }{\rm N}$ - $18\hbox{$^\circ$ }{\rm N}$ 22

${\rm R}'$ 409.9 28.2 7.1 99.99 $13\hbox{$^\circ$ }{\rm S}$ - $19\hbox{$^\circ$ }{\rm S}$ 21, 22

413.3 28.0 6.9 99.99 $13\hbox{$^\circ$ }{\rm S}$ - $18\hbox{$^\circ$ }{\rm S}$ 21, 22

${\rm S}'_{1}$ 423.2 27.3 2.8 99.99 $9\hbox{$^\circ$ }{\rm S}$ - $12\hbox{$^\circ$ }{\rm S}$ 21, 23

425.5 27.2 2.6 99.90 $8\hbox{$^\circ$ }{\rm S}$ - $13\hbox{$^\circ$ }{\rm S}$ 23

${\rm S}'_{2}$ 428.8 27.0 2.7 99.99 $9\hbox{$^\circ$ }{\rm S}$ - $10\hbox{$^\circ$ }{\rm S}$ 22

432.1 26.8 3.0 99.99 $11\hbox{$^\circ$ }{\rm S}$ - $12\hbox{$^\circ$ }{\rm S}$ 22

${\rm S}'_{3}$ 435.4 26.6 3.6 99.99 $11\hbox{$^\circ$ }{\rm S}$ - $13\hbox{$^\circ$ }{\rm S}$ 23

${\rm S}'_{4}$ 441.0 26.2 3.0 99.99 $16\hbox{$^\circ$ }{\rm S}$ - $17\hbox{$^\circ$ }{\rm S}$ 22

${\rm T}'_{1}$ 425.5 27.2 1.2 99.90 $26\hbox{$^\circ$ }{\rm N}$ - $41\hbox{$^\circ$ }{\rm N}$ 22

427.7 27.1 2.6 99.99 $18\hbox{$^\circ$ }{\rm N}$ - $20\hbox{$^\circ$ }{\rm N}$ 22

429.9 27.1 2.0 99.99 $23\hbox{$^\circ$ }{\rm N}$ - $25\hbox{$^\circ$ }{\rm N}$ 21

${\rm T}'_{2}$ 433.2 26.7 3.8 99.99 $15\hbox{$^\circ$ }{\rm N}$ - $25\hbox{$^\circ$ }{\rm N}$ 21

${\rm T}'_{3}$ 436.5 26.5 3.5 99.99 $13\hbox{$^\circ$ }{\rm N}$ - $18\hbox{$^\circ$ }{\rm N}$ 23

${\rm U}'_{1}$ 455.4 25.4 2.6 99.90 $13\hbox{$^\circ$ }{\rm S}$ - $16\hbox{$^\circ$ }{\rm S}$ 22

${\rm U'}_2$ 462.0 25.1 3.3 99.99 $16\hbox{$^\circ$ }{\rm S}$ - $17\hbox{$^\circ$ }{\rm S}$ 21, 23

**Table 3:** Frequencies $\nu$ , periods $\nu ^{-1}$ , maximum Power $P_{\rm max}$ , significance levels p, latitudes $\vartheta$ (where the power exceeds the given significance level) and cycles (when the corresponding oscillations occurred) for the labeled regions in Figs. 7a and 7b. The error $\Delta \nu=0.6~{\rm nHz}$ is half the frequency resolution.
	$\nu$ (nHz)	$\nu ^{-1}$ (d)	$P_{\rm max}$	p (%)	$\vartheta$	Cycle
${\rm N}$	400.0	28.9	1.1	99.99	$27\hbox{$^\circ$ }{\rm S}$ - $58\hbox{$^\circ$ }{\rm S}$	23
${\rm O}$	401.1	28.9	0.4	99.99	$34\hbox{$^\circ$ }{\rm S}$ - $54\hbox{$^\circ$ }{\rm S}$	21, 22, 23
${\rm P}$	406.6	28.5	0.6	99.99	$28\hbox{$^\circ$ }{\rm S}$ - $54\hbox{$^\circ$ }{\rm S}$	23
${\rm Q}$	406.6	28.5	1.2	99.99	$26\hbox{$^\circ$ }{\rm N}$ - $57\hbox{$^\circ$ }{\rm N}$	22
${\rm R}$	411.0	28.2	1.1	99.99	$19\hbox{$^\circ$ }{\rm S}$ - $57\hbox{$^\circ$ }{\rm S}$	21, 22
	414.4	27.9	1.0	99.99	$22\hbox{$^\circ$ }{\rm S}$ - $23\hbox{$^\circ$ }{\rm S}$	21, 22
${\rm S}_2$	429.9	26.9	1.1	99.99	$16\hbox{$^\circ$ }{\rm S}$	22
	429.9	26.9	0.7	99.90	$19\hbox{$^\circ$ }{\rm S}$ - $21\hbox{$^\circ$ }{\rm S}$	23
${\rm S}_3$	434.3	26.7	1.2	99.99	$10\hbox{$^\circ$ }{\rm S}$ - $12\hbox{$^\circ$ }{\rm S}$	23
	437.6	26.5	0.6	99.90	$11\hbox{$^\circ$ }{\rm S}$	23
${\rm T}_1$	426.6	27.1	1.1	99.99	$23\hbox{$^\circ$ }{\rm N}$ - $25\hbox{$^\circ$ }{\rm N}$	22
	429.9	26.9	0.8	99.99	$11\hbox{$^\circ$ }{\rm N}$ - $12\hbox{$^\circ$ }{\rm N}$	21, 22
	429.9	26.9	0.9	99.90	$16\hbox{$^\circ$ }{\rm N}$ - $20\hbox{$^\circ$ }{\rm N}$	21, 22
${\rm T}_2$	433.2	26.7	0.6	99.99	$6\hbox{$^\circ$ }{\rm N}$ - $8\hbox{$^\circ$ }{\rm N}$	21, 22
	433.2	26.7	0.9	99.99	$11\hbox{$^\circ$ }{\rm N}$ - $12\hbox{$^\circ$ }{\rm N}$	21, 22
${\rm T}_3$	435.4	26.6	0.9	99.90	$14\hbox{$^\circ$ }{\rm N}$ - $15\hbox{$^\circ$ }{\rm N}$	23
	437.6	26.4	1.0	99.99	$16\hbox{$^\circ$ }{\rm N}$	21, 22, 23
${\rm U}$	463.1	25.0	0.5	99.00	$14\hbox{$^\circ$ }{\rm S}$	22
${\rm M'}$	398.9	29.0	2.3	99.90	$16\hbox{$^\circ$ }{\rm N}$ - $18\hbox{$^\circ$ }{\rm N}$	22
${\rm R}'$	409.9	28.2	7.1	99.99	$13\hbox{$^\circ$ }{\rm S}$ - $19\hbox{$^\circ$ }{\rm S}$	21, 22
	413.3	28.0	6.9	99.99	$13\hbox{$^\circ$ }{\rm S}$ - $18\hbox{$^\circ$ }{\rm S}$	21, 22
${\rm S}'_{1}$	423.2	27.3	2.8	99.99	$9\hbox{$^\circ$ }{\rm S}$ - $12\hbox{$^\circ$ }{\rm S}$	21, 23
	425.5	27.2	2.6	99.90	$8\hbox{$^\circ$ }{\rm S}$ - $13\hbox{$^\circ$ }{\rm S}$	23
${\rm S}'_{2}$	428.8	27.0	2.7	99.99	$9\hbox{$^\circ$ }{\rm S}$ - $10\hbox{$^\circ$ }{\rm S}$	22
	432.1	26.8	3.0	99.99	$11\hbox{$^\circ$ }{\rm S}$ - $12\hbox{$^\circ$ }{\rm S}$	22
${\rm S}'_{3}$	435.4	26.6	3.6	99.99	$11\hbox{$^\circ$ }{\rm S}$ - $13\hbox{$^\circ$ }{\rm S}$	23
${\rm S}'_{4}$	441.0	26.2	3.0	99.99	$16\hbox{$^\circ$ }{\rm S}$ - $17\hbox{$^\circ$ }{\rm S}$	22
${\rm T}'_{1}$	425.5	27.2	1.2	99.90	$26\hbox{$^\circ$ }{\rm N}$ - $41\hbox{$^\circ$ }{\rm N}$	22
	427.7	27.1	2.6	99.99	$18\hbox{$^\circ$ }{\rm N}$ - $20\hbox{$^\circ$ }{\rm N}$	22
	429.9	27.1	2.0	99.99	$23\hbox{$^\circ$ }{\rm N}$ - $25\hbox{$^\circ$ }{\rm N}$	21
${\rm T}'_{2}$	433.2	26.7	3.8	99.99	$15\hbox{$^\circ$ }{\rm N}$ - $25\hbox{$^\circ$ }{\rm N}$	21
${\rm T}'_{3}$	436.5	26.5	3.5	99.99	$13\hbox{$^\circ$ }{\rm N}$ - $18\hbox{$^\circ$ }{\rm N}$	23
${\rm U}'_{1}$	455.4	25.4	2.6	99.90	$13\hbox{$^\circ$ }{\rm S}$ - $16\hbox{$^\circ$ }{\rm S}$	22
${\rm U'}_2$	462.0	25.1	3.3	99.99	$16\hbox{$^\circ$ }{\rm S}$ - $17\hbox{$^\circ$ }{\rm S}$	21, 23

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