Table 7: Frequency estimates for r-modes (Eqs. (3) and (4)) and equatorially trapped Rossby waves (Eq. (5)), calculated with $\nu_{{\rm S}}=455~{\rm nHz}$ .
l m $\nu_{l,m,{\rm syn}}$ $\nu_{l,m,{\rm rot}}$ m $\nu_{m,{\rm rot}}$ m $\nu_{m,{\rm rot}}$

1 1 -31.7 455 1 448 20 45.4

2 1 272 152 2 362 21 43.2

2 2 543 303 3 272 22 41.3

3 1 347 75.8 4 214 23 39.5

3 3 1042 228 5 175 24 37.8

4 1 378 45.5 6 147 25 36.3

4 4 1511 182 7 127 26 34.9

5 1 393 30.3 8 112 27 33.7

5 5 1965 152 9 100 28 32.5

6 1 402 21.7 10 90.1 29 31.3

6 6 2410 130 11 82.0 30 30.3

7 1 407 16.3 12 75.3 31 29.3

7 7 2849 114 13 69.6 32 28.4

8 1 411 12.6 14 64.7 33 27.5

8 8 3285 101 15 60.4 34 26.7

9 1 413 10.1 16 56.6 35 26.0

9 9 3718 91. 17 53.3 36 25.3

10 1 415 8.27 18 50.4 37 24.6

10 10 4150 82.7 19 47.8 38 23.9

**Table 7:** Frequency estimates for r-modes (Eqs. (3) and (4)) and equatorially trapped Rossby waves (Eq. (5)), calculated with $\nu_{{\rm S}}=455~{\rm nHz}$ .
l	m	$\nu_{l,m,{\rm syn}}$	$\nu_{l,m,{\rm rot}}$	m	$\nu_{m,{\rm rot}}$	m	$\nu_{m,{\rm rot}}$
1	1	-31.7	455	1	448	20	45.4
2	1	272	152	2	362	21	43.2
2	2	543	303	3	272	22	41.3
3	1	347	75.8	4	214	23	39.5
3	3	1042	228	5	175	24	37.8
4	1	378	45.5	6	147	25	36.3
4	4	1511	182	7	127	26	34.9
5	1	393	30.3	8	112	27	33.7
5	5	1965	152	9	100	28	32.5
6	1	402	21.7	10	90.1	29	31.3
6	6	2410	130	11	82.0	30	30.3
7	1	407	16.3	12	75.3	31	29.3
7	7	2849	114	13	69.6	32	28.4
8	1	411	12.6	14	64.7	33	27.5
8	8	3285	101	15	60.4	34	26.7
9	1	413	10.1	16	56.6	35	26.0
9	9	3718	91.	17	53.3	36	25.3
10	1	415	8.27	18	50.4	37	24.6
10	10	4150	82.7	19	47.8	38	23.9

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