683 research outputs found

    Spin frequency evolution and pulse profile variations of the recently re-activated radio magnetar XTE J1810-197

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    After spending almost a decade in a radio-quiet state, the Anomalous X-ray Pulsar XTE J1810-197 turned back on in early December 2018. We have observed this radio magnetar at 1.5 GHz with ~daily cadence since the first detection of radio re-activation on 8 December 2018. In this paper, we report on the current timing properties of XTE J1810-197 and find that the magnitude of the spin frequency derivative has increased by a factor of 2.6 over our 48-day data set. We compare our results with the spin-down evolution reported during its previous active phase in the radio band. We also present total intensity pulse profiles at five different observing frequencies between 1.5 and 8.4 GHz, collected with the Lovell and the Effelsberg telescopes. The profile evolution in our data set is less erratic than what was reported during the previous active phase, and can be seen varying smoothly between observations. Profiles observed immediately after the outburst show the presence of at least five cycles of a very stable ~50-ms periodicity in the main pulse component that lasts for at least tens of days. This remarkable structure is seen across the full range of observing frequencies.Comment: 9 pages, 7 figures, updated with additional analysis of the 50-ms oscillation, accepted for publication in MNRA

    Precision timing of PSR J1012+5307 and strong-field GR tests

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    We report on the high precision timing analysis of the pulsar-white dwarf binary PSR J1012+5307. Using 15 years of multi-telescope data from the European Pulsar Timing Array (EPTA) network, a significant measurement of the variation of the orbital period is obtained. Using this ideal strong-field gravity laboratory we derive theory independent limits for both the dipole radiation and the variation of the gravitational constant.Comment: 3 pages, Proceedings of the 12th Marcel Grossmann Meeting on General Relativity (MG 12

    The INPOP10a planetary ephemeris and its applications in fundamental physics

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    International audienceCompared to the previous INPOP versions, the INPOP10a planetary and lunar ephemeris has several improvements. For the planets of our solar system, no big change was brought in the dynamics but improvements were implemented in the fitting process, the data sets used in the fit and in the selection of fitted parameters. We report here the main characteristics of the planetary part of INPOP10a like the fit of the product of the Solar mass with the gravitational constant (GM⊙_{\odot}) instead of the astronomical unit. Determinations of PPN parameters as well as adjustments of the Sun J2 and of asteroid masses are also presented. New advances of nodes and perihelia of planets were also estimated and are given here. As for INPOP08, INPOP10a provides to the user, positions and velocities of the planets, the moon, the rotation angles of the Earth and the Moon as well as TT-TDB chebychev polynomials at http://www.imcce.fr/inpo

    The Discovery of Six Recycled Pulsars from the Arecibo 327-MHz Drift-Scan Pulsar Survey

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    Recycled pulsars are old (≳108\gtrsim10^{8} yr) neutron stars that are descendants from close, interacting stellar systems. In order to understand their evolution and population, we must find and study the largest number possible of recycled pulsars in a way that is as unbiased as possible. In this work, we present the discovery and timing solutions of five recycled pulsars in binary systems (PSRs J0509++0856, J0709++0458, J0732++2314, J0824++0028, J2204++2700) and one isolated millisecond pulsar (PSR J0154++1833). These were found in data from the Arecibo 327-MHz Drift-Scan Pulsar Survey (AO327). All these pulsars have a low dispersion measure (DM) (≲45 pc cm−3\lesssim 45 \, \rm{pc}\, cm^{-3}), and have a DM-determined distance of ≲\lesssim 3 kpc. Their timing solutions, have data spans ranging from 1 to ∼\sim 7 years, include precise estimates of their spin and astrometric parameters, and for the binaries, precise estimates of their Keplerian binary parameters. Their orbital periods range from about 4 to 815 days and the minimum companion masses (assuming a pulsar mass of 1.4 M⊙\rm{M_{\odot}}) range from ∼\sim 0.06--1.11 M⊙\rm{M_{\odot}}. For two of the binaries we detect post-Keplerian parameters; in the case of PSR~J0709++0458 we measure the component masses but with a low precision, in the not too distant future the measurement of the rate of advance of periastron and the Shapiro delay will allow very precise mass measurements for this system. Like several other systems found in the AO327 data, PSRs J0509++0854, J0709++0458 and J0732++2314 are now part of the NANOGrav timing array for gravitational wave detection

    Placing limits on the stochastic gravitational-wave background using European Pulsar Timing Array data

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    Direct detection of low-frequency gravitational waves (10−9−10−810^{-9} - 10^{-8} Hz) is the main goal of pulsar timing array (PTA) projects. One of the main targets for the PTAs is to measure the stochastic background of gravitational waves (GWB) whose characteristic strain is expected to approximately follow a power-law of the form hc(f)=A(f/yr−1)αh_c(f)=A (f/\hbox{yr}^{-1})^{\alpha}, where ff is the gravitational-wave frequency. In this paper we use the current data from the European PTA to determine an upper limit on the GWB amplitude AA as a function of the unknown spectral slope α\alpha with a Bayesian algorithm, by modelling the GWB as a random Gaussian process. For the case α=−2/3\alpha=-2/3, which is expected if the GWB is produced by supermassive black-hole binaries, we obtain a 95% confidence upper limit on AA of 6×10−156\times 10^{-15}, which is 1.8 times lower than the 95% confidence GWB limit obtained by the Parkes PTA in 2006. Our approach to the data analysis incorporates the multi-telescope nature of the European PTA and thus can serve as a useful template for future intercontinental PTA collaborations.Comment: 14 pages, 8 figures, 3 tables, mnras accepte
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