2021MNRAS.500.3281G


Query : 2021MNRAS.500.3281G

2021MNRAS.500.3281G - Mon. Not. R. Astron. Soc., 500, 3281-3289 (2021/January-3)

On the long-term evolution of rotating radio transients.

GENCALI A.A. and ERTAN U.

Abstract (from CDS):

Investigation of the long-term evolution of rotating radio transients (RRATs) is important to understand the evolutionary connections between the isolated neutron star populations in a single picture. The X-ray luminosities of RRATs (except one source) are not known. In the fallback disc model, we have developed a method to estimate the dipole field strengths of RRATs without X-ray information. We have found that RRATs could have dipole field strengths, B0, at the poles ranging from ∼7 x 109 to ∼6 x 1011 G which fill the gap between the B0 ranges of central compact objects (CCOs) and dim isolated neutron stars (XDINs) estimated in the same model. In our model, most of RRATs are evolving at ages (∼2-6) x 105 yr, much smaller than their characteristic ages, such that, cooling luminosities of a large fraction of relatively nearby RRATs could be detected by the eROSITA all-sky survey. Many RRATs are located above the upper border of the pulsar death valley with the fields inferred from the dipole-torque formula, while they do not show strong, continuous radio pulses. The B0 values estimated in our model, place all RRATs either into the death valley or below the death line. We have tentatively proposed that RRATs could be the sources below their individual death points, and their short radio bursts could be ignited by the disc-field interaction occasionally enhancing the flux of open field lines through the magnetic poles. We have also discussed the evolutionary links between CCOs, RRATs, and XDINs.

Abstract Copyright: © 2020 The Author(s) Published by Oxford University Press on behalf of the Royal Astronomical Society

Journal keyword(s): accretion, accretion discs - methods: numerical - stars: neutron - pulsars: general

Simbad objects: 36

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Number of rows : 36
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 PSR J0139+3336 Psr 01 39 57.23 +33 36 59.7           ~ 24 0
2 PSR J0146+6145 Psr 01 46 22.21 +61 45 03.8   28.100 25.620     ~ 613 0
3 PSR J0201+7005 Psr 02 01 41.344 +70 05 18.11           ~ 7 0
4 PSR J0628+09 Psr 06 28 36 +09 09.2           ~ 28 0
5 PSR J0735-62 Psr 07 35 05.0 -63 02 00           ~ 12 0
6 PSR J0847-4316 Psr 08 47 57.33 -43 16 56.8           ~ 25 0
7 PSR J0912-3851 Psr 09 12 42.70 -38 51 03.0           ~ 11 0
8 PSR J1048-5838 Psr 10 48 12.570 -58 38 18.58           ~ 8 0
9 PSR J1226-3223 Psr 12 26 45.9 -32 23 14           ~ 8 0
10 PSR J1317-5759 Psr 13 17 46.31 -57 59 30.2           ~ 32 0
11 PSR J1443-60 Psr 14 44 06.02 -60 26 09.4           ~ 14 0
12 PSR J1514-59 Psr 15 13 44.78 -59 46 31.9           ~ 9 0
13 PSR J1538+2345 Psr 15 38 06.07 +23 45 04.0           ~ 20 0
14 PSR J1554-5209 Psr 15 54 27.15 -52 09 38.3           ~ 12 0
15 PSR J1623-0841 Psr 16 23 42.701 -08 41 36.40           ~ 9 0
16 PSR J1647-3607 Psr 16 47 46.51 -36 07 04.0           ~ 9 0
17 PSR J1652-4406 Psr 16 52.0 -44 06           ~ 6 0
18 PSR J1707-44 Psr 17 07 41.41 -44 17 19.0           ~ 10 0
19 PSR J1739-2521 Psr 17 39 32.83 -25 21 02.0           ~ 9 0
20 PSR J1754-3014 Psr 17 54 30.08 -30 14 42.0           ~ 5 0
21 PSR J1807-25 Psr 18 07 13.66 -25 57 20.0           ~ 6 0
22 PSR J1819-1458 Psr 18 19 34.173 -14 58 03.57           ~ 136 0
23 PSR J1826-14 Psr 18 26 42.391 -14 19 21.60           ~ 20 0
24 PSR J1839-0141 Psr 18 39 07.03 -01 41 56.0           ~ 10 0
25 PSR J1840-1417 Psr 18 41.0 -14 18           ~ 22 0
26 PSR J1846-02 Psr 18 46 15.49 -02 57 36.0           ~ 34 0
27 PSR J1848-1243 Psr 18 48 17.980 -12 43 26.60           ~ 6 0
28 PSR J1854+0306 Psr 18 54.0 +03 06           ~ 20 0
29 PSR J1854-15 Psr 18 54 53.6 -15 57 47           ~ 10 0
30 PSR J1909+0641 Psr 19 09 29 +06 41.4           ~ 6 0
31 PSR J1913+1333 Psr 19 13 17.975 +13 30 32.80           ~ 44 0
32 PSR J1919+1745 Psr 19 19 43 +17 45.0           ~ 8 0
33 PSR J2033+0042 Psr 20 33 31.12000 +00 42 24.1000           ~ 11 0
34 PSR J2105+6223 Psr 21 05 12.93 +62 23 05.5           ~ 4 0
35 2E 4673 HXB 23 01 08.14 +58 52 44.5           ~ 673 1
36 PSR J2325-0530 Psr 23 25 15.3 -05 30 39           ~ 15 0

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