Table 3.

Fit parameters of the NSs plotted in Figs 3 and 4. The solutions with low and high asymptotic fields are listed, and solutions that recover the parameters of Ho (2015) are marked with an asterisk.

Fit parameters
PSRαϵτmBGP0t
(kyr)(1013 G)(s)(kyr)
SGR 0526−660.1000.1001.64256.0353.2464.786
0.9000.0010.438240.0003.6894.779
SGR 1627−410.1000.1001.26122.4880.0903.677
0.9000.0013.201240.0000.4774.981
HBP J1734−33330.1000.1001.1935.2311.0123.477
*0.6330.0020.0856.5001.0602.070
0.9000.00110.00075.2360.8389.939
HBP J1846−0258 A0.1000.0010.0744.9320.2470.433
0.9000.1006.71843.2730.0070.810
HBP J1846−0258 B0.1000.1000.2864.8800.1870.833
0.9000.1003.10243.1870.2250.430
PSR J0537−69100.1000.1000.3720.0940.0151.007
*0.5250.0530.9210.1700.0151.950
0.9000.00110.0002.9420.0143.564
PSR B0833−450.1000.1002.2540.3380.0736.570
*0.5410.0052.7090.5500.06510.200
0.9000.00110.0003.5860.05815.738
RX J0822.0−43000.1000.1001.7830.0980.1115.200
0.9000.00110.0003.0100.1123.702
1E 1207.4−52000.1000.0016.8600.0170.42020.000
0.9000.00110.0000.8800.4242.004
CXOU J185238.6+0040200.1000.1002.5720.0030.1057.500
0.9000.00110.0000.0690.1055.401
Fit parameters
PSRαϵτmBGP0t
(kyr)(1013 G)(s)(kyr)
SGR 0526−660.1000.1001.64256.0353.2464.786
0.9000.0010.438240.0003.6894.779
SGR 1627−410.1000.1001.26122.4880.0903.677
0.9000.0013.201240.0000.4774.981
HBP J1734−33330.1000.1001.1935.2311.0123.477
*0.6330.0020.0856.5001.0602.070
0.9000.00110.00075.2360.8389.939
HBP J1846−0258 A0.1000.0010.0744.9320.2470.433
0.9000.1006.71843.2730.0070.810
HBP J1846−0258 B0.1000.1000.2864.8800.1870.833
0.9000.1003.10243.1870.2250.430
PSR J0537−69100.1000.1000.3720.0940.0151.007
*0.5250.0530.9210.1700.0151.950
0.9000.00110.0002.9420.0143.564
PSR B0833−450.1000.1002.2540.3380.0736.570
*0.5410.0052.7090.5500.06510.200
0.9000.00110.0003.5860.05815.738
RX J0822.0−43000.1000.1001.7830.0980.1115.200
0.9000.00110.0003.0100.1123.702
1E 1207.4−52000.1000.0016.8600.0170.42020.000
0.9000.00110.0000.8800.4242.004
CXOU J185238.6+0040200.1000.1002.5720.0030.1057.500
0.9000.00110.0000.0690.1055.401
Table 3.

Fit parameters of the NSs plotted in Figs 3 and 4. The solutions with low and high asymptotic fields are listed, and solutions that recover the parameters of Ho (2015) are marked with an asterisk.

Fit parameters
PSRαϵτmBGP0t
(kyr)(1013 G)(s)(kyr)
SGR 0526−660.1000.1001.64256.0353.2464.786
0.9000.0010.438240.0003.6894.779
SGR 1627−410.1000.1001.26122.4880.0903.677
0.9000.0013.201240.0000.4774.981
HBP J1734−33330.1000.1001.1935.2311.0123.477
*0.6330.0020.0856.5001.0602.070
0.9000.00110.00075.2360.8389.939
HBP J1846−0258 A0.1000.0010.0744.9320.2470.433
0.9000.1006.71843.2730.0070.810
HBP J1846−0258 B0.1000.1000.2864.8800.1870.833
0.9000.1003.10243.1870.2250.430
PSR J0537−69100.1000.1000.3720.0940.0151.007
*0.5250.0530.9210.1700.0151.950
0.9000.00110.0002.9420.0143.564
PSR B0833−450.1000.1002.2540.3380.0736.570
*0.5410.0052.7090.5500.06510.200
0.9000.00110.0003.5860.05815.738
RX J0822.0−43000.1000.1001.7830.0980.1115.200
0.9000.00110.0003.0100.1123.702
1E 1207.4−52000.1000.0016.8600.0170.42020.000
0.9000.00110.0000.8800.4242.004
CXOU J185238.6+0040200.1000.1002.5720.0030.1057.500
0.9000.00110.0000.0690.1055.401
Fit parameters
PSRαϵτmBGP0t
(kyr)(1013 G)(s)(kyr)
SGR 0526−660.1000.1001.64256.0353.2464.786
0.9000.0010.438240.0003.6894.779
SGR 1627−410.1000.1001.26122.4880.0903.677
0.9000.0013.201240.0000.4774.981
HBP J1734−33330.1000.1001.1935.2311.0123.477
*0.6330.0020.0856.5001.0602.070
0.9000.00110.00075.2360.8389.939
HBP J1846−0258 A0.1000.0010.0744.9320.2470.433
0.9000.1006.71843.2730.0070.810
HBP J1846−0258 B0.1000.1000.2864.8800.1870.833
0.9000.1003.10243.1870.2250.430
PSR J0537−69100.1000.1000.3720.0940.0151.007
*0.5250.0530.9210.1700.0151.950
0.9000.00110.0002.9420.0143.564
PSR B0833−450.1000.1002.2540.3380.0736.570
*0.5410.0052.7090.5500.06510.200
0.9000.00110.0003.5860.05815.738
RX J0822.0−43000.1000.1001.7830.0980.1115.200
0.9000.00110.0003.0100.1123.702
1E 1207.4−52000.1000.0016.8600.0170.42020.000
0.9000.00110.0000.8800.4242.004
CXOU J185238.6+0040200.1000.1002.5720.0030.1057.500
0.9000.00110.0000.0690.1055.401
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