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 . | |||||||
---|---|---|---|---|---|---|---|
PSR . | P . | |$\dot{P}$| . | n . | τPSR . | SNR . | τSNR − . | τSNR + . |
. | (s) . | (10−11ss−1) . | . | (kyr) . | . | (kyr) . | (kyr) . |
AXP 1E 1841−045 | 11.783 | 3.930 | 4.750 | G27.4+0.0 (Kes 73) | 0.750 | 2.100 [1] | |
AXP 1E 2259+586 | 6.979 | 4.843e − 2 | 228.317 | G109.1−01.0 (CTB 109) | 10.000 | 16.000 [2] | |
CXOU J171405.7−381031 | 3.825 | 6.400 | 0.947 | G348.7+00.3 | 0.350 | 3.150 [3] | |
SGR 0526−66 | 8.054 | 3.800 | 3.358 | N49 | − | 4.800 [4] | |
SGR 1627−41 | 2.595 | 1.900 | 2.164 | G337.3−0.1 | − | 5.000 [5] | |
HBP J1119−6127 | 0.408 | 0.400 | 2.684 ± 0.002 [14] | 1.616 | G292.2−0.5 | 4.200 | 7.100 [6] |
HBP J1734−3333 | 1.170 | 0.228 | 0.9 ± 0.2 [15] | 8.131 | G354.8−0.8 | 1.300 | − [7] |
HBP J1846−0258 A | 0.325 | 0.709 | 2.64 ± 0.01 [16] | 0.726 | G029.7−0.3 (Kes 75) | 0.900 | 4.300 [8] |
HBP J1846−0258 B | 0.327 | 0.711 | 2.16 ± 0.13 [17] | 0.728 | |||
PSR J0537−6910 | 0.016 | 0.518 | −1.5 ± 0.1 [18] | 4.925 | N157B | 1.000 | 5.000 [9] |
PSR B0833−45 | 0.089 | 1.250 | 1.4 ± 0.2 [19] | 11.319 | G263.9−03.3 (Vela) | 5.400 | 16.000 [10] |
RX J0822.0−4300 | 0.112 | 8.300e − 4 | 213.799 | G260.4−3.4 (Puppis A) | 3.700 | 5.200 [11] | |
1E 1207.4−5209 | 0.424 | 6.600e − 6 | 1.018e5 | G296.5 +10.0 (PKS 1209−51/52) | 2.000 | 20.000 [12] | |
CXOU J185238.6+004020 | 0.105 | 8.680e − 7 | 1.917e5 | G033.6+00.1 (Kes 79) | 5.400 | 7.500 [13] |
Observed properties of NSs . | |||||||
---|---|---|---|---|---|---|---|
PSR . | P . | |$\dot{P}$| . | n . | τPSR . | SNR . | τSNR − . | τSNR + . |
. | (s) . | (10−11ss−1) . | . | (kyr) . | . | (kyr) . | (kyr) . |
AXP 1E 1841−045 | 11.783 | 3.930 | 4.750 | G27.4+0.0 (Kes 73) | 0.750 | 2.100 [1] | |
AXP 1E 2259+586 | 6.979 | 4.843e − 2 | 228.317 | G109.1−01.0 (CTB 109) | 10.000 | 16.000 [2] | |
CXOU J171405.7−381031 | 3.825 | 6.400 | 0.947 | G348.7+00.3 | 0.350 | 3.150 [3] | |
SGR 0526−66 | 8.054 | 3.800 | 3.358 | N49 | − | 4.800 [4] | |
SGR 1627−41 | 2.595 | 1.900 | 2.164 | G337.3−0.1 | − | 5.000 [5] | |
HBP J1119−6127 | 0.408 | 0.400 | 2.684 ± 0.002 [14] | 1.616 | G292.2−0.5 | 4.200 | 7.100 [6] |
HBP J1734−3333 | 1.170 | 0.228 | 0.9 ± 0.2 [15] | 8.131 | G354.8−0.8 | 1.300 | − [7] |
HBP J1846−0258 A | 0.325 | 0.709 | 2.64 ± 0.01 [16] | 0.726 | G029.7−0.3 (Kes 75) | 0.900 | 4.300 [8] |
HBP J1846−0258 B | 0.327 | 0.711 | 2.16 ± 0.13 [17] | 0.728 | |||
PSR J0537−6910 | 0.016 | 0.518 | −1.5 ± 0.1 [18] | 4.925 | N157B | 1.000 | 5.000 [9] |
PSR B0833−45 | 0.089 | 1.250 | 1.4 ± 0.2 [19] | 11.319 | G263.9−03.3 (Vela) | 5.400 | 16.000 [10] |
RX J0822.0−4300 | 0.112 | 8.300e − 4 | 213.799 | G260.4−3.4 (Puppis A) | 3.700 | 5.200 [11] | |
1E 1207.4−5209 | 0.424 | 6.600e − 6 | 1.018e5 | G296.5 +10.0 (PKS 1209−51/52) | 2.000 | 20.000 [12] | |
CXOU J185238.6+004020 | 0.105 | 8.680e − 7 | 1.917e5 | G033.6+00.1 (Kes 79) | 5.400 | 7.500 [13] |
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 . | |||||||
---|---|---|---|---|---|---|---|
PSR . | P . | |$\dot{P}$| . | n . | τPSR . | SNR . | τSNR − . | τSNR + . |
. | (s) . | (10−11ss−1) . | . | (kyr) . | . | (kyr) . | (kyr) . |
AXP 1E 1841−045 | 11.783 | 3.930 | 4.750 | G27.4+0.0 (Kes 73) | 0.750 | 2.100 [1] | |
AXP 1E 2259+586 | 6.979 | 4.843e − 2 | 228.317 | G109.1−01.0 (CTB 109) | 10.000 | 16.000 [2] | |
CXOU J171405.7−381031 | 3.825 | 6.400 | 0.947 | G348.7+00.3 | 0.350 | 3.150 [3] | |
SGR 0526−66 | 8.054 | 3.800 | 3.358 | N49 | − | 4.800 [4] | |
SGR 1627−41 | 2.595 | 1.900 | 2.164 | G337.3−0.1 | − | 5.000 [5] | |
HBP J1119−6127 | 0.408 | 0.400 | 2.684 ± 0.002 [14] | 1.616 | G292.2−0.5 | 4.200 | 7.100 [6] |
HBP J1734−3333 | 1.170 | 0.228 | 0.9 ± 0.2 [15] | 8.131 | G354.8−0.8 | 1.300 | − [7] |
HBP J1846−0258 A | 0.325 | 0.709 | 2.64 ± 0.01 [16] | 0.726 | G029.7−0.3 (Kes 75) | 0.900 | 4.300 [8] |
HBP J1846−0258 B | 0.327 | 0.711 | 2.16 ± 0.13 [17] | 0.728 | |||
PSR J0537−6910 | 0.016 | 0.518 | −1.5 ± 0.1 [18] | 4.925 | N157B | 1.000 | 5.000 [9] |
PSR B0833−45 | 0.089 | 1.250 | 1.4 ± 0.2 [19] | 11.319 | G263.9−03.3 (Vela) | 5.400 | 16.000 [10] |
RX J0822.0−4300 | 0.112 | 8.300e − 4 | 213.799 | G260.4−3.4 (Puppis A) | 3.700 | 5.200 [11] | |
1E 1207.4−5209 | 0.424 | 6.600e − 6 | 1.018e5 | G296.5 +10.0 (PKS 1209−51/52) | 2.000 | 20.000 [12] | |
CXOU J185238.6+004020 | 0.105 | 8.680e − 7 | 1.917e5 | G033.6+00.1 (Kes 79) | 5.400 | 7.500 [13] |
Observed properties of NSs . | |||||||
---|---|---|---|---|---|---|---|
PSR . | P . | |$\dot{P}$| . | n . | τPSR . | SNR . | τSNR − . | τSNR + . |
. | (s) . | (10−11ss−1) . | . | (kyr) . | . | (kyr) . | (kyr) . |
AXP 1E 1841−045 | 11.783 | 3.930 | 4.750 | G27.4+0.0 (Kes 73) | 0.750 | 2.100 [1] | |
AXP 1E 2259+586 | 6.979 | 4.843e − 2 | 228.317 | G109.1−01.0 (CTB 109) | 10.000 | 16.000 [2] | |
CXOU J171405.7−381031 | 3.825 | 6.400 | 0.947 | G348.7+00.3 | 0.350 | 3.150 [3] | |
SGR 0526−66 | 8.054 | 3.800 | 3.358 | N49 | − | 4.800 [4] | |
SGR 1627−41 | 2.595 | 1.900 | 2.164 | G337.3−0.1 | − | 5.000 [5] | |
HBP J1119−6127 | 0.408 | 0.400 | 2.684 ± 0.002 [14] | 1.616 | G292.2−0.5 | 4.200 | 7.100 [6] |
HBP J1734−3333 | 1.170 | 0.228 | 0.9 ± 0.2 [15] | 8.131 | G354.8−0.8 | 1.300 | − [7] |
HBP J1846−0258 A | 0.325 | 0.709 | 2.64 ± 0.01 [16] | 0.726 | G029.7−0.3 (Kes 75) | 0.900 | 4.300 [8] |
HBP J1846−0258 B | 0.327 | 0.711 | 2.16 ± 0.13 [17] | 0.728 | |||
PSR J0537−6910 | 0.016 | 0.518 | −1.5 ± 0.1 [18] | 4.925 | N157B | 1.000 | 5.000 [9] |
PSR B0833−45 | 0.089 | 1.250 | 1.4 ± 0.2 [19] | 11.319 | G263.9−03.3 (Vela) | 5.400 | 16.000 [10] |
RX J0822.0−4300 | 0.112 | 8.300e − 4 | 213.799 | G260.4−3.4 (Puppis A) | 3.700 | 5.200 [11] | |
1E 1207.4−5209 | 0.424 | 6.600e − 6 | 1.018e5 | G296.5 +10.0 (PKS 1209−51/52) | 2.000 | 20.000 [12] | |
CXOU J185238.6+004020 | 0.105 | 8.680e − 7 | 1.917e5 | G033.6+00.1 (Kes 79) | 5.400 | 7.500 [13] |
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