2013MNRAS.434.1387L


Query : 2013MNRAS.434.1387L

2013MNRAS.434.1387L - Mon. Not. R. Astron. Soc., 434, 1387-1397 (2013/September-2)

The high time resolution universe pulsar survey -VIII. The galactic millisecond pulsar population.

LEVIN L., BAILES M., BARSDELL B.R., BATES S.D., BHAT N.D.R., BURGAY M., BURKE-SPOLAOR S., CHAMPION D.J., COSTER P., D'AMICO N., JAMESON A., JOHNSTON S., KEITH M.J., KRAMER M., MILIA S., NG C., POSSENTI A., STAPPERS B., THORNTON D. and VAN STRATEN W.

Abstract (from CDS):

We have used millisecond pulsars (MSPs) from the southern High Time Resolution Universe (HTRU) intermediate latitude survey area to simulate the distribution and total population of MSPs in the Galaxy. Our model makes use of the scalefactor method, which estimates the ratio of the total number of MSPs in the Galaxy to the known sample. Using our best-fitting value for the z-height, z = 500pc, we find an underlying population of MSPs of 8.3(±4.2)x104 sources down to a limiting luminosity of Lmin = 0.1mJykpc2 and a luminosity distribution with a steep slope of dlogN/dlogL = -1.45±0.14. However, at the low end of the luminosity distribution, the uncertainties introduced by small number statistics are large. By omitting very low luminosity pulsars, we find a Galactic population above Lmin = 0.2mJykpc2 of only 3.0(±0.7)x104 MSPs. We have also simulated pulsars with periods shorter than any known MSP, and estimate the maximum number of sub-MSPs in the Galaxy to be 7.8(±5.0)x104 pulsars at L = 0.1mJykpc2. In addition, we estimate that the high and low latitude parts of the southern HTRU survey will detect 68 and 42 MSPs, respectively, including 78 new discoveries. Pulsar luminosity, and hence flux density, is an important input parameter in the model. Some of the published flux densities for the pulsars in our sample do not agree with the observed flux densities from our data set, and we have instead calculated average luminosities from archival data from the Parkes Telescope. We found many luminosities to be very different than their catalogue values, leading to very different population estimates. Large variations in flux density highlight the importance of including scintillation effects in MSP population studies.

Abstract Copyright: © 2013 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society (2013)

Journal keyword(s): stars: neutron - pulsars: general

Simbad objects: 55

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Number of rows : 55
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 J0900-3144 Psr 09 00 43.95220 -31 44 30.8722           ~ 68 0
2 PSR J1017-7156 Psr 10 17 51.311783 -71 56 41.57398           ~ 61 1
3 PSR J1045-45 Psr 10 45 50.179671 -45 09 54.05686           ~ 154 1
4 PSR J1056-7117 Psr 10 56 45.8706243384 -71 17 53.766596328           ~ 8 0
5 PSR J1125-58 Psr 11 25 44.352943 -58 25 16.85965           ~ 55 1
6 PSR J1125-6014 Psr 11 25 55.243299 -60 14 06.80942           ~ 61 0
7 PSR J1157-5112 Psr 11 57 08.166 -51 12 56.14           ~ 32 1
8 PSR J1216-6410 Psr 12 16 07.321183 -64 10 09.16656           ~ 23 0
9 PSR J1227-6208 Psr 12 27 00.4413 -62 08 43.789           ~ 16 0
10 PSR B1257+12 Psr 13 00 03.1075 +12 40 55.155           ~ 546 1
11 PSR J1337-6423 Psr 13 37 31.93 -64 23 04.9           ~ 18 2
12 PSR J1406-4656 Psr 14 06.0 -46 56           ~ 2 0
13 PSR J1420-5625 Psr 14 20 03.062 -56 25 55.00           ~ 11 0
14 PSR J1431-5740 Psr 14 31 03.49603 -57 40 11.6601           ~ 15 0
15 PSR J1431-4715 Psr 14 31 44.6313693632 -47 15 27.399549133           ~ 49 0
16 PSR J1435-60 Psr 14 35 20.2733756922 -61 00 57.545079751           ~ 58 1
17 PSR J1439-5501 Psr 14 39 39.7420 -55 01 23.621           ~ 27 1
18 PSR J1446-4701 Psr 14 46 35.709721 -47 01 26.79678           ~ 82 1
19 PSR J1453-58 Psr 14 54 10.908 -58 46 34.74           ~ 31 1
20 PSR J1502-6752 Psr 15 02 18.610 -67 52 16.78           ~ 16 1
21 PSR J1525-5544 Psr 15 25 28.12719 -55 45 49.8854           ~ 19 0
22 PSR J1529-3828 Psr 15 29 15.1066 -38 28 45.850           ~ 10 0
23 PSR J1543-5149 Psr 15 43 44.145289 -51 49 54.71350           ~ 41 1
24 PSR J1545-4550 Psr 15 45 55.945403 -45 50 37.50813           ~ 34 0
25 PSR J1604-72 Psr 16 03 35.670781 -72 02 32.82328           ~ 142 0
26 PSR J1618-3919 Psr 16 18 18.82500 -39 21 01.8320           ~ 32 0
27 PSR J1622-6617 Psr 16 22 03.667 -66 17 16.98           ~ 13 1
28 PSR J1629-6902 Psr 16 29 08.744211 -69 02 45.46922           ~ 22 0
29 PSR J1708-35 Psr 17 08 17.616678 -35 06 22.65950           ~ 29 1
30 PSR J1719-14 Psr 17 19 10.076221 -14 38 01.00200           ~ 92 2
31 PSR J1721-2457 Psr 17 21 05.50008 -24 57 06.2260           ~ 37 0
32 PSR J1729-2117 Psr 17 29 10.808 -21 17 28.00           ~ 8 0
33 PSR J1730-2304 Psr 17 30 21.68471 -23 04 31.2590           ~ 194 1
34 PSR J1731-1845 Psr 17 31.0 -18 45           ~ 1 0
35 PSR J1732-5049 Psr 17 32 47.766068 -50 49 00.31465           ~ 87 0
36 PSR J1744-1134 Psr 17 44 29.4220844 -11 34 54.801320           ~ 323 1
37 PSR J1745-0952 Psr 17 45 09.1400 -09 52 39.670           ~ 28 0
38 PSR J1748-2446ad Psr 17 48 04.9 -24 46 04           ~ 141 1
39 Cl Terzan 5 Cl* 17 48 05.00 -24 46 48.0           ~ 948 1
40 PSR J1751-2857 Psr 17 51 32.686848 -28 57 46.57130           ~ 65 1
41 PSR J1755-3715 Psr 17 55 35.3975810472 -37 16 10.012600704           ~ 8 0
42 PSR J1756-2251 Psr 17 56 46.63 -22 51 59.4           ~ 153 1
43 PSR J1756-5322 Psr 17 57 15.154960 -53 22 26.59604           ~ 56 0
44 PSR J1801-32 Psr 18 01 25.8890 -32 10 53.720           ~ 22 1
45 PSR J1801-1417 Psr 18 01 51.064902 -14 17 34.54980           ~ 45 0
46 PSR J1802-2124 Psr 18 02 05.334393 -21 24 03.67600           ~ 101 1
47 PSR J1804-27 Psr 18 04 21.13307 -27 17 31.3370           ~ 87 1
48 PSR J1810-2005 Psr 18 10 58.988 -20 05 08.30           ~ 33 0
49 PSR J1811-2405 Psr 18 11 19.854352 -24 05 18.42800           ~ 56 1
50 PSR J1825-0319 Psr 18 25 55.954707 -03 19 57.58370           ~ 19 0
51 PSR J1843-1113 Psr 18 43 41.260405 -11 13 31.10310           ~ 86 0
52 PSR B1855+09 Psr 18 57 36.390620 +09 43 17.20712           DA 569 1
53 PSR J1911-11 Psr 19 11 49.2927 -11 14 22.330           ~ 87 1
54 PSR J1918-0642 Psr 19 18 48.027685 -06 42 34.95735           ~ 146 0
55 PSR B1937+21.4 Psr 19 39 38.560096 +21 34 59.13552           ~ 1142 0

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