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Table 2 Satellite and observatory data weight parameters, residual means and rms

From: Parent magnetic field models for the IGRF-12GFZ-candidates

 

Nb

σ

k

a

μ

rms

  

A

B

C

    

Satellite

        

X SM

122,286

3.4

3.2

3.2

1.0

0.55

0.01

2.76

Y SM

122,286

3.3

3.4

3.3

1.0

0.55

0.00

2.87

Z SM

122,286

5.4

5.4

5.5

1.0

0.55

−1.04

4.75

X HL

276,916

10.0

10.0

11.0

0.7

0.30

0.56

25.77

Y HL

276,916

11.3

12.2

6.5

0.7

0.30

0.13

28.14

Z HL

276,916

11.0

11.0

7.0

0.7

0.30

0.04

13.76

X SM,Euler only

89,461

3.4

3.2

3.2

1.0

0.55

−0.02

2.94

Y SM,Euler only

89,461

3.3

3.4

3.3

1.0

0.55

0.01

2.76

Z SM,Euler only

89,461

5.4

5.4

5.5

1.0

0.55

0.77

5.46

Observatories

        

X SM

31,614

4.5

1.0

0.40

0.27

4.03

Y SM

31,614

4.2

1.0

0.40

−0.22

3.95

Z SM

31,614

7.0

1.0

0.40

−0.36

5.43

X HL

8,007

14.0

0.9

0.30

−4.34

24.59

Y HL

8,007

7.0

0.9

0.30

1.19

15.56

Z HL

8,007

18.0

0.9

0.30

0.40

24.12

  1. The first three rows for satellite and observatory data are mid- and low-latitude data, whereas the next three are for high-latitude data. The ‘ SM,Euler only’ data are used exclusively for calculating the Euler angles. Nb is the number of data values, σ is the prior standard deviation in nT, k and a are the weight parameters defined in Equation 12, and finally μ and rms are the data residuals mean and rms values, respectively (both in nT).