Table 2.

For a given PSR, P is the period, |$\dot{P}$| the period derivative. The characteristic age is τPSR and the lower and upper SNR age limits are τSNR− and τSNR +, respectively, from the McGill magnetar catalogue (http://www.physics.mcgill.ca/∼pulsar/magnetar/main.html). The SNR ages have been compiled in the U. of Manitoba's High-Energy SNR Catalogue (SNRcat, http://www.physics.umanitoba.ca/snr/SNRcat/). References to SNR ages in this table are [1]: Kumar et al. (2014), [2]: Nakano et al. (2015), [3]: Nakamura et al. (2009), [4]: Park et al. (2012), [5]: Corbel et al. (1999), [6]: Kumar et al. (2012), [7]: Ho & Anderson (2012), [8]: Gotthelf et al. (2000), [9]: Wang & Gotthelf (1998), [10]: Page et al. (2009), [11]: Becker et al. (2012), [12]: Zavlin et al. (2000), [13]: Sun et al. (2004). References to the braking indices included here are [14]: Weltevrede et al. (2011), [15]: Espinoza et al. (2011), [16]: Livingstone et al. (2006), [17]: Livingstone et al. (2011), [18]: Middleditch et al. (2006), [19]: Lyne et al. (1996), [20]: Olausen & Kaspi (2014).

Observed properties of NSs
PSRP|$\dot{P}$|nτPSRSNRτSNR −τSNR +
(s)(10−11ss−1)(kyr)(kyr)(kyr)
AXP 1E 1841−04511.7833.9304.750G27.4+0.0 (Kes 73)0.7502.100 [1]
AXP 1E 2259+5866.9794.843e − 2228.317G109.1−01.0 (CTB 109)10.00016.000 [2]
CXOU J171405.7−3810313.8256.4000.947G348.7+00.30.3503.150 [3]
SGR 0526−668.0543.8003.358N494.800 [4]
SGR 1627−412.5951.9002.164G337.3−0.15.000 [5]
HBP J1119−61270.4080.4002.684 ± 0.002 [14]1.616G292.2−0.54.2007.100 [6]
HBP J1734−33331.1700.2280.9 ± 0.2 [15]8.131G354.8−0.81.300− [7]
HBP J1846−0258 A0.3250.7092.64 ± 0.01 [16]0.726G029.7−0.3 (Kes 75)0.9004.300 [8]
HBP J1846−0258 B0.3270.7112.16 ± 0.13 [17]0.728
PSR J0537−69100.0160.518−1.5 ± 0.1 [18]4.925N157B1.0005.000 [9]
PSR B0833−450.0891.2501.4 ± 0.2 [19]11.319G263.9−03.3 (Vela)5.40016.000 [10]
RX J0822.0−43000.1128.300e − 4213.799G260.4−3.4 (Puppis A)3.7005.200 [11]
1E 1207.4−52090.4246.600e − 61.018e5G296.5 +10.0 (PKS 1209−51/52)2.00020.000 [12]
CXOU J185238.6+0040200.1058.680e − 71.917e5G033.6+00.1 (Kes 79)5.4007.500 [13]
Observed properties of NSs
PSRP|$\dot{P}$|nτPSRSNRτSNR −τSNR +
(s)(10−11ss−1)(kyr)(kyr)(kyr)
AXP 1E 1841−04511.7833.9304.750G27.4+0.0 (Kes 73)0.7502.100 [1]
AXP 1E 2259+5866.9794.843e − 2228.317G109.1−01.0 (CTB 109)10.00016.000 [2]
CXOU J171405.7−3810313.8256.4000.947G348.7+00.30.3503.150 [3]
SGR 0526−668.0543.8003.358N494.800 [4]
SGR 1627−412.5951.9002.164G337.3−0.15.000 [5]
HBP J1119−61270.4080.4002.684 ± 0.002 [14]1.616G292.2−0.54.2007.100 [6]
HBP J1734−33331.1700.2280.9 ± 0.2 [15]8.131G354.8−0.81.300− [7]
HBP J1846−0258 A0.3250.7092.64 ± 0.01 [16]0.726G029.7−0.3 (Kes 75)0.9004.300 [8]
HBP J1846−0258 B0.3270.7112.16 ± 0.13 [17]0.728
PSR J0537−69100.0160.518−1.5 ± 0.1 [18]4.925N157B1.0005.000 [9]
PSR B0833−450.0891.2501.4 ± 0.2 [19]11.319G263.9−03.3 (Vela)5.40016.000 [10]
RX J0822.0−43000.1128.300e − 4213.799G260.4−3.4 (Puppis A)3.7005.200 [11]
1E 1207.4−52090.4246.600e − 61.018e5G296.5 +10.0 (PKS 1209−51/52)2.00020.000 [12]
CXOU J185238.6+0040200.1058.680e − 71.917e5G033.6+00.1 (Kes 79)5.4007.500 [13]
Table 2.

For a given PSR, P is the period, |$\dot{P}$| the period derivative. The characteristic age is τPSR and the lower and upper SNR age limits are τSNR− and τSNR +, respectively, from the McGill magnetar catalogue (http://www.physics.mcgill.ca/∼pulsar/magnetar/main.html). The SNR ages have been compiled in the U. of Manitoba's High-Energy SNR Catalogue (SNRcat, http://www.physics.umanitoba.ca/snr/SNRcat/). References to SNR ages in this table are [1]: Kumar et al. (2014), [2]: Nakano et al. (2015), [3]: Nakamura et al. (2009), [4]: Park et al. (2012), [5]: Corbel et al. (1999), [6]: Kumar et al. (2012), [7]: Ho & Anderson (2012), [8]: Gotthelf et al. (2000), [9]: Wang & Gotthelf (1998), [10]: Page et al. (2009), [11]: Becker et al. (2012), [12]: Zavlin et al. (2000), [13]: Sun et al. (2004). References to the braking indices included here are [14]: Weltevrede et al. (2011), [15]: Espinoza et al. (2011), [16]: Livingstone et al. (2006), [17]: Livingstone et al. (2011), [18]: Middleditch et al. (2006), [19]: Lyne et al. (1996), [20]: Olausen & Kaspi (2014).

Observed properties of NSs
PSRP|$\dot{P}$|nτPSRSNRτSNR −τSNR +
(s)(10−11ss−1)(kyr)(kyr)(kyr)
AXP 1E 1841−04511.7833.9304.750G27.4+0.0 (Kes 73)0.7502.100 [1]
AXP 1E 2259+5866.9794.843e − 2228.317G109.1−01.0 (CTB 109)10.00016.000 [2]
CXOU J171405.7−3810313.8256.4000.947G348.7+00.30.3503.150 [3]
SGR 0526−668.0543.8003.358N494.800 [4]
SGR 1627−412.5951.9002.164G337.3−0.15.000 [5]
HBP J1119−61270.4080.4002.684 ± 0.002 [14]1.616G292.2−0.54.2007.100 [6]
HBP J1734−33331.1700.2280.9 ± 0.2 [15]8.131G354.8−0.81.300− [7]
HBP J1846−0258 A0.3250.7092.64 ± 0.01 [16]0.726G029.7−0.3 (Kes 75)0.9004.300 [8]
HBP J1846−0258 B0.3270.7112.16 ± 0.13 [17]0.728
PSR J0537−69100.0160.518−1.5 ± 0.1 [18]4.925N157B1.0005.000 [9]
PSR B0833−450.0891.2501.4 ± 0.2 [19]11.319G263.9−03.3 (Vela)5.40016.000 [10]
RX J0822.0−43000.1128.300e − 4213.799G260.4−3.4 (Puppis A)3.7005.200 [11]
1E 1207.4−52090.4246.600e − 61.018e5G296.5 +10.0 (PKS 1209−51/52)2.00020.000 [12]
CXOU J185238.6+0040200.1058.680e − 71.917e5G033.6+00.1 (Kes 79)5.4007.500 [13]
Observed properties of NSs
PSRP|$\dot{P}$|nτPSRSNRτSNR −τSNR +
(s)(10−11ss−1)(kyr)(kyr)(kyr)
AXP 1E 1841−04511.7833.9304.750G27.4+0.0 (Kes 73)0.7502.100 [1]
AXP 1E 2259+5866.9794.843e − 2228.317G109.1−01.0 (CTB 109)10.00016.000 [2]
CXOU J171405.7−3810313.8256.4000.947G348.7+00.30.3503.150 [3]
SGR 0526−668.0543.8003.358N494.800 [4]
SGR 1627−412.5951.9002.164G337.3−0.15.000 [5]
HBP J1119−61270.4080.4002.684 ± 0.002 [14]1.616G292.2−0.54.2007.100 [6]
HBP J1734−33331.1700.2280.9 ± 0.2 [15]8.131G354.8−0.81.300− [7]
HBP J1846−0258 A0.3250.7092.64 ± 0.01 [16]0.726G029.7−0.3 (Kes 75)0.9004.300 [8]
HBP J1846−0258 B0.3270.7112.16 ± 0.13 [17]0.728
PSR J0537−69100.0160.518−1.5 ± 0.1 [18]4.925N157B1.0005.000 [9]
PSR B0833−450.0891.2501.4 ± 0.2 [19]11.319G263.9−03.3 (Vela)5.40016.000 [10]
RX J0822.0−43000.1128.300e − 4213.799G260.4−3.4 (Puppis A)3.7005.200 [11]
1E 1207.4−52090.4246.600e − 61.018e5G296.5 +10.0 (PKS 1209−51/52)2.00020.000 [12]
CXOU J185238.6+0040200.1058.680e − 71.917e5G033.6+00.1 (Kes 79)5.4007.500 [13]
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