2012MNRAS.422.1294G


Query : 2012MNRAS.422.1294G

2012MNRAS.422.1294G - Mon. Not. R. Astron. Soc., 422, 1294-1305 (2012/May-2)

Discovery of the millisecond pulsar PSR J2043+1711 in a Fermi source with the Nancay Radio Telescope.

GUILLEMOT L., FREIRE P.C.C., COGNARD I., JOHNSON T.J., TAKAHASHI Y., KATAOKA J., DESVIGNES G., CAMILO F., FERRARA E.C., HARDING A.K., JANSSEN G.H., KEITH M., KERR M., KRAMER M., PARENT D., RANSOM S.M., RAY P.S., SAZ PARKINSON P.M., SMITH D.A., STAPPERS B.W. and THEUREAU G.

Abstract (from CDS):

We report the discovery of the millisecond pulsar PSR J2043+1711 in a search of a Fermi Large Area Telescope (LAT) source with no known associations, with the Nanay Radio Telescope. The new pulsar, confirmed with the Green Bank Telescope, has a spin period of 2.38 ms, is relatively nearby ({img} kpc) and is in a 1.48-d orbit around a low-mass companion, probably an He-type white dwarf. Using an ephemeris based on Arecibo, Nanay and Westerbork timing measurements, pulsed gamma-ray emission was detected in the data recorded by the Fermi LAT. The gamma-ray light curve and spectral properties are typical of other gamma-ray millisecond pulsars seen with Fermi. X-ray observations of the pulsar with Suzaku and the Swift X-ray Telescope yielded no detection. At 1.4 GHz, we observe strong flux density variations because of interstellar diffractive scintillation; however, a sharp peak can be observed at this frequency during bright scintillation states. At 327 MHz, the pulsar is detected with a much higher signal-to-noise ratio and its flux density is far more steady. However, at that frequency the Arecibo instrumentation cannot yet fully resolve the pulse profile. Despite that, our pulse time-of-arrival measurements have a post-fit residual rms of 2 {img}s. This and the expected stability of this system have made PSR J2043+1711 one of the first new Fermi-selected millisecond pulsars to be added to pulsar gravitational wave timing arrays. It has also allowed a significant measurement of relativistic delays in the times of arrival of the pulses due to the curvature of space-time near the companion, but not yet with enough precision to derive useful masses for the pulsar and the companion. Nevertheless, a mass for the pulsar between 1.7 and 2.0 M☉ can be derived if a standard millisecond pulsar formation model is assumed. In this paper, we also present a comprehensive summary of pulsar searches in Fermi LAT sources with the Nanay Radio Telescope to date.

Abstract Copyright: 2012 The Authors Monthly Notices of the Royal Astronomical Society2012 RAS

Journal keyword(s): pulsars: general - pulsars: individual: PSR J2043+1711 - gamma-rays: general

Simbad objects: 33

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Number of rows : 33
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 NVSS J003119+072456 BLL 00 31 19.7096957544 +07 24 53.560153296   19.8   18.6   ~ 42 1
2 7C 0059+5808 Bla 01 02 45.76237340 +58 24 11.1366164   20.09 19.22 18.57 17.90 ~ 262 1
3 QSO B0116-219 Bla 01 18 57.26217841 -21 41 30.1402631   19.40 19.0 19.37   ~ 144 1
4 PSO J021.2103-06.4169 BLL 01 24 50.4851504351 -06 25 00.943106646       18.4   ~ 46 1
5 1RXS J012712.6+032250 BLL 01 27 13.9561096712 +03 23 00.587171321           ~ 39 0
6 RX J0131.1+6120 BLL 01 31 07.2257589038 +61 20 33.372505609           ~ 54 0
7 RX J0137.7+5814 BLL 01 37 50.4761854680 +58 14 11.321731860           ~ 66 2
8 1FGL J0224.0+6201c gam 02 24 02 +62 01.0           ~ 22 0
9 RX J0250.7+5629 BLL 02 50 47.5927019856 +56 29 35.424727188           ~ 32 1
10 ICRF J033415.4-372543 BLL 03 34 15.4249837080 -37 25 43.063647672 16.95 16.71 16.56     ~ 80 1
11 2FGL J0434.1-2014 BLL 04 34 07.9139033376 -20 15 17.144331444 18.95 18.45 18.17 19.6   ~ 54 1
12 PSO J080.8044-25.5318 G 05 23 13.0748610986 -25 31 54.492620030           ~ 56 0
13 ICRF J071355.6+193500 Bla 07 13 55.67917496 +19 35 00.4089341       18   ~ 106 3
14 PSR J0734-1559 Psr 07 34 45.693 -15 59 18.43           ~ 29 0
15 2FGL J0928.8-3530 Bla 09 28 49.82929 -35 29 48.8494           ~ 36 1
16 1FGL J1119.9-2205 gam 11 20.0 -22 04           ~ 36 0
17 ICRF J112038.4+070447 QSO 11 20 38.44359842 +07 04 47.1724558           ~ 70 1
18 SDSS J112903.24+375656.7 BLL 11 29 03.2509775616 +37 56 56.742130896           ~ 35 0
19 PSR J1311-3430 Psr 13 11 45.7292612136 -34 30 30.294149760   21.0   18.8   ~ 181 1
20 QSO B1313-333 Bla 13 16 07.98594757 -33 38 59.1726741   18.04 20.0 17.23   ~ 267 1
21 NVSS J134042-041006 BLL 13 40 42.0173568000 -04 10 07.046694084           ~ 46 1
22 1FGL J1407.9-2928 gam 14 07 24.29 -29 48 23.0           ~ 26 0
23 PSR J1614-2230 Psr 16 14 36.50974 -22 30 31.5420           ~ 452 1
24 PSR J1625-0021 Psr 16 25 10.469 -00 21 26.73           ~ 35 0
25 3C 345 Bla 16 42 58.80997043 +39 48 36.9939552   16.81 16.59 16.84   ~ 1808 3
26 PSR J1903+0327 Psr 19 03 05.7937 +03 27 19.222           ~ 187 1
27 MAGIC J2001+435 BLL 20 01 12.8737326408 +43 52 52.840241616   15.6   15   ~ 108 1
28 PSR J2017+0603 Psr 20 17 22.7048 +06 03 05.585           ~ 120 1
29 RX J2030.8+1935 BLL 20 30 57.1340134032 +19 36 12.930528420           ~ 59 2
30 QSO B2032+107 BLL 20 35 22.33330500 +10 56 06.7881888   17.96 16.37 17.4   ~ 218 1
31 PSR J2043+1711 Psr 20 43 20.8828 +17 11 28.941           ~ 129 1
32 PSR J2302+4442 Psr 23 02 46.9789 +44 42 22.102           ~ 124 0
33 PSR J2339-0533 Psr 23 39 38.7412778376 -05 33 05.108592528     18.48     ~ 149 0

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