2010ApJ...715..230O


Query : 2010ApJ...715..230O

2010ApJ...715..230O - Astrophys. J., 715, 230-241 (2010/May-3)

Pulsar binary birthrates with spin-opening angle correlations.

O'SHAUGHNESSY R. and KIM C.

Abstract (from CDS):

One ingredient in an empirical birthrate estimate for pulsar binaries is the fraction of sky subtended by the pulsar beam: the pulsar beaming fraction. This fraction depends on both the pulsar's opening angle and the misalignment angle between its spin and magnetic axes. The current estimates for pulsar binary birthrates are based on an average value of beaming fractions for only two pulsars, i.e., PSRs B1913+16 and B1534+12. In this paper, we revisit the observed pulsar binaries to examine the sensitivity of birthrate predictions to different assumptions regarding opening angle and alignment. Based on empirical estimates for the relative likelihood of different beam half-opening angles and misalignment angles between the pulsar rotation and magnetic axes, we calculate an effective beaming correction factor, fb,eff, whose reciprocal is equivalent to the average fraction of all randomly selected pulsars that point toward us. For those pulsars without any direct beam geometry constraints, we find that fb,eff is likely to be smaller than 6, a canonically adopted value when calculating birthrates of Galactic pulsar binaries. We calculate fb,eff for PSRs J0737-3039A and J1141-6545, applying the currently available constraints for their beam geometry. As in previous estimates of the posterior probability density function P({R}) for pulsar binary birthrates {R}, PSRs J0737-3039A and J1141-6545 still significantly contribute to, if not dominate, the Galactic birthrate of tight pulsar-neutron star (NS) and pulsar-white dwarf (WD) binaries, respectively. Our median posterior present-day birthrate predictions for tight PSR-NS binaries, wide PSR-NS binaries, and tight PSR-WD binaries given a preferred pulsar population model and beaming geometry are 89 Myr–1, 0.5 Myr–1, and 34 Myr–1, respectively. For long-lived PSR-NS binaries, these estimates include a weak (x1.6) correction for slowly decaying star formation in the galactic disk. For pulsars with spin period between 10 ms and 100 ms, where few measurements of misalignment and opening angle provide a sound basis for extrapolation, we marginalized our posterior birthrate distribution P({R}) over a range of plausible beaming correction factors. We explore several alternative beaming geometry distributions, demonstrating that our predictions are robust except in (untestable) scenarios with many highly aligned recycled pulsars. Finally, in addition to exploring alternative beam geometries, we also briefly summarize how uncertainties in each pulsar binary's lifetime and in the pulsar luminosity distribution can be propagated into P({R)}.

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Journal keyword(s): binaries: close - pulsars: general - stars: neutron - white dwarfs

Simbad objects: 15

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Number of rows : 15
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 J0737-3039A Psr 07 37 51.24669 -30 39 40.6895           ~ 317 1
2 PSR J0737-3039 Psr 07 37 51.248 -30 39 40.83           ~ 445 1
3 PSR J0737-3039B Psr 07 37 51.24927 -30 39 40.7195           ~ 222 1
4 PSR J0751+1807 Psr 07 51 09.1539 +18 07 38.335           ~ 316 1
5 PSR J1141-6545 Psr 11 41 07.00060 -65 45 19.0500     25.08 24.38   ~ 207 1
6 PSR J1518+4904 Psr 15 18 16.832 +49 04 34.19           ~ 201 1
7 PSR B1534+11 Psr 15 37 09.9603 +11 55 55.554           ~ 453 1
8 PSR J1738+0333 Psr 17 38 53.966386 +03 33 10.87200           ~ 191 1
9 PSR J1753-2240 Psr 17 53 39.847 -22 40 42.00           ~ 53 1
10 PSR J1756-2251 Psr 17 56 46.63 -22 51 59.4           ~ 153 1
11 PSR J1756-5322 Psr 17 57 15.154960 -53 22 26.59604           ~ 56 0
12 PSR B1809-17.6 Psr 18 11 55.034 -17 36 37.70           ~ 114 1
13 PSR J1829+2456 Psr 18 29 34.6668 +24 56 18.193           ~ 89 1
14 PSR J1906+0749 Psr 19 06 48.67 +07 46 28.6           ~ 172 1
15 PSR J1915+1606 Psr 19 15 27.99999 +16 06 27.4034     22.5     ~ 1032 1

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