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Table 2.

Coefficients cℓm for the LCT covariance-based data.

m cmm cm + 2,  m cm + 4,  m cm + 6,  m
3 (+0.026, +0.417)  ±  (0.018, 0.105) (−0.155, +0.089)  ±  (0.032, 0.103) (+0.118, −0.108)  ±  (0.075, 0.074) (−0.117, +0.004)  ±  (0.015, 0.029)
4 (+0.457, +0.136)  ±  (0.016, 0.060) (−0.097, +0.061)  ±  (0.027, 0.017) (−0.010, −0.066)  ±  (0.036, 0.030) (−0.071, +0.019)  ±  (0.014, 0.026)
5 (+0.478, +0.037)  ±  (0.031, 0.070) (−0.263, −0.021)  ±  (0.086, 0.067) (−0.059, −0.106)  ±  (0.052, 0.112) (+0.041, −0.011)  ±  (0.045, 0.040)
6 (+0.411, +0.021)  ±  (0.055, 0.019) (−0.202, −0.050)  ±  (0.025, 0.057) (−0.005, −0.118)  ±  (0.040, 0.032) (−0.006, +0.059)  ±  (0.007, 0.018)
7 (+0.473, +0.026)  ±  (0.024, 0.028) (−0.183, −0.055)  ±  (0.015, 0.024) (−0.012, −0.073)  ±  (0.012, 0.023) (+0.043, +0.018)  ±  (0.006, 0.012)
8 (+0.441, −0.013)  ±  (0.015, 0.022) (−0.231, −0.038)  ±  (0.021, 0.027) (−0.047, −0.009)  ±  (0.031, 0.068) (+0.038, +0.001)  ±  (0.017, 0.027)
9 (+0.434, +0.028)  ±  (0.013, 0.042) (−0.162, −0.032)  ±  (0.023, 0.014) (−0.010, −0.053)  ±  (0.018, 0.044) (+0.025, +0.022)  ±  (0.005, 0.030)
10 (+0.423, +0.008)  ±  (0.024, 0.012) (−0.139, −0.057)  ±  (0.017, 0.041) (+0.011, −0.076)  ±  (0.034, 0.028) (+0.020, −0.013)  ±  (0.001, 0.010)
11 (+0.400, −0.010)  ±  (0.027, 0.003) (−0.173, −0.117)  ±  (0.049, 0.043) (−0.043, −0.064)  ±  (0.027, 0.058) (+0.002, +0.024)  ±  (0.018, 0.024)
12 (+0.419, −0.040)  ±  (0.029, 0.023) (−0.117, −0.078)  ±  (0.006, 0.011) (−0.016, −0.021)  ±  (0.010, 0.032) (−0.027, −0.007)  ±  (0.042, 0.030)
13 (+0.345, −0.016)  ±  (0.036, 0.023) (−0.195, −0.112)  ±  (0.018, 0.020) (−0.048, −0.028)  ±  (0.029, 0.011) (−0.071, +0.026)  ±  (0.013, 0.023)
14 (+0.380, −0.057)  ±  (0.026, 0.025) (−0.128, −0.102)  ±  (0.038, 0.044) (−0.007, +0.006)  ±  (0.027, 0.022) (−0.019, +0.001)  ±  (0.015, 0.017)
15 (+0.431, −0.074)  ±  (0.017, 0.013) (−0.085, −0.151)  ±  (0.054, 0.029) (−0.072, −0.041)  ±  (0.020, 0.057) (−0.053, −0.012)  ±  (0.036, 0.020)

Notes. Each bracketed pair of numbers refers to the real and imaginary parts of cℓm. The numbers in italics are not significantly different from zero (zero within 1σ).

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