Table 3.
Identified frequencies using superposition of linear modes and their corresponding amplitudes and phases.
Designation | f | A | ϕ | f − iforb |
---|---|---|---|---|
(d−1) | (ppm) |
![]() |
(d−1) | |
F1 | 11.070396(6) | 1671(14) | 0.881(6) | 0.291161(6) |
F2 | 11.624913(6) | 1644(14) | 0.951(7) | 0.246831(6) |
F3 | 12.795260(7) | 1450(14) | 0.898(10) | 0.219486(7) |
F4 | 20.122555(10) | 909(14) | 0.671(12) | 0.238223(10) |
F5 = F4 − 2forb | 18.924924(11) | 852(14) | 0.654(12) | 0.238161(11) |
F6 = F2 + 2forb | 12.822585(13) | 751(14) | 0.955(16) | 0.246810(13) |
F7 = F2 − 2forb | 10.427359(13) | 689(14) | 0.416(16) | 0.246970(13) |
F8 | 25.636172(16) | 586(14) | 0.923(18) | 0.114224(16) |
F9 | 0.384953(17) | 526(14) | 0.911(20) | 0.213894(17) |
F10 | 1.20499(9) | 355(6) | 0.93(15) | 0.00730(9) |
F11 = F2 + F9 | 12.004905(29) | 353(14) | 0.14(4) | 0.027977(29) |
F12 | 21.064357(27) | 336(14) | 0.96(3) | 0.104732(27) |
F13 | 24.231017(27) | 333(14) | 0.84(3) | 0.277161(27) |
F14 = F2−forb | 11.025846(28) | 331(14) | 0.17(3) | 0.246610(28) |
F15 | 26.474933(29) | 320(14) | 0.46(3) | 0.125691(29) |
F16 = 2F3 | 25.58853(3) | 307(14) | 0.43(4) | 0.16187(3) |
F17 | 26.02396(3) | 304(14) | 0.26(4) | 0.27357(3) |
F18 = F13 − 2forb | 23.03406(3) | 302(14) | 0.70(4) | 0.27790(3) |
F19 | 21.15642(3) | 296(14) | 0.86(4) | 0.19680(3) |
F20 | 18.79018(3) | 283(14) | 0.45(4) | 0.22594(3) |
F21 | 26.30992(3) | 278(14) | 0.58(4) | 0.03932(3) |
F22 | 25.36344(3) | 276(14) | 0.93(4) | 0.21189(3) |
F23 = F17 + 2forb | 27.22191(4) | 267(14) | 0.76(4) | 0.27382(4) |
F24 = 2F13 − F19 | 27.30487(4) | 265(14) | 0.75(4) | 0.24206(4) |
F25 = F15 − 2forb | 25.27759(4) | 261(14) | 0.48(4) | 0.12604(4) |
F26 = F8 − 2forb | 24.43814(4) | 259(14) | 0.56(4) | 0.11456(4) |
F27 = 2F20 − F8 | 11.94680(4) | 255(14) | 0.99(4) | 0.03013(4) |
F28 | 19.80501(4) | 235(14) | 0.59(4) | 0.04308(4) |
F29 = 2F10 | 2.40437(15) | 228(10) | 0.53(25) | 0.00899(15) |
F30 = F1 + 3forb | 12.86744(4) | 226(14) | 0.68(5) | 0.29167(4) |
F31 = F10 + 2F30 | 26.93439(4) | 213(14) | 0.69(5) | 0.01370(4) |
F32 | 30.10391(5) | 203(14) | 0.89(6) | 0.16159(5) |
F33 = F26 − F27 | 12.49486(5) | 195(14) | 0.84(5) | 0.08091(5) |
F34 = F33−forb | 11.89432(5) | 193(14) | 0.79(6) | 0.08261(5) |
F35 = F24 − 2forb | 26.10775(5) | 190(14) | 0.90(6) | 0.24149(5) |
F36 | 25.79572(5) | 188(14) | 0.45(6) | 0.04533(5) |
F37 = F3 − 2F9 | 12.01945(6) | 184(14) | 0.41(7) | 0.04252(6) |
F38 | 29.67863(6) | 184(14) | 0.11(8) | 0.26369(6) |
F39 = 2F8 − F24 | 23.96734(5) | 182(14) | 0.62(6) | 0.01348(5) |
F40 = 2F3 + 2F9 | 26.36555(5) | 182(14) | 0.31(6) | 0.01631(5) |
F41 = F36 − 2forb | 24.59721(5) | 180(14) | 0.41(6) | 0.04451(5) |
F42 = F26 − 2F2 | 1.19073(9) | 179(18) | 0.75(14) | 0.00696(9) |
F43 = 2F29 + F25 | 30.09140(6) | 178(14) | 0.69(7) | 0.14908(6) |
F44 = 2F6 − F26 | 1.21202(16) | 175(6) | 0.81(25) | 0.01433(16) |
F45 = F8 − 2F7 | 4.78401(5) | 167(14) | 0.45(6) | 0.00676(5) |
Notes. The values in parentheses give the 1σ uncertainty as a combination of the values reported by the least square algorithm and the standard error estimates formulated by Montgomery & O’Donoghue (1999). Here, forb is the orbital frequency. Further possible combinations are: F24 = 2F15 − 2F6; F33 = F22 − F30; F37 = 2F12 − F32; F39 = F27 + F37; F43 = 2F26 − F20; F44 = F29 − F42; F45 = F29 + 2F42.
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