141 results on '"Hobbs, G."'
Search Results
2. Limitations in timing precision due to single-pulse shape variability in millisecond pulsars
- Author
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Shannon, RM, Osłowski, S, Dai, S, Bailes, M, Hobbs, G, Manchester, RN, van Straten, W, Raithel, CA, Ravi, V, Toomey, L, Bhat, NDR, Burke-Spolaor, S, Coles, WA, Keith, MJ, Kerr, M, Levin, Y, Sarkissian, JM, Wang, J-B, Wen, L, and Zhu, X-J
- Subjects
methods: data analysis ,stars: neutron ,pulsars: general ,Astronomical and Space Sciences ,Astronomy & Astrophysics - Abstract
High-sensitivity radio-frequency observations of millisecond pulsars usually show stochastic, broad-band, pulse-shape variations intrinsic to the pulsar emission process. These variations induce jitter noise in pulsar timing observations; understanding the properties of this noise is of particular importance for the effort to detect gravitational waves with pulsar timing arrays. We assess the short-term profile and timing stability of 22 millisecond pulsars that are part of the Parkes Pulsar Timing Array sample by examining intraobservation arrival time variability and single-pulse phenomenology. In 7 of the 22 pulsars, in the band centred at approximately 1400 MHz, we find that the brightest observations are limited by intrinsic jitter. We find consistent results, either detections or upper limits, for jitter noise in other frequency bands. PSR J1909-3744 shows the lowest levels of jitter noise, which we estimate to contribute ~10 ns root mean square error to the arrival times for hour-duration observations. Larger levels of jitter noise are found in pulsars with wider pulses and distributions of pulse intensities. The jitter noise in PSR J0437-4715 decorrelates over a bandwidth of ∼2 GHz. We show that the uncertainties associated with timing pulsar models can be improved by including physically motivated jitter uncertainties. Pulse-shape variations will limit the timing precision at future, more sensitive, telescopes; it is imperative to account for this noise when designing instrumentation and timing campaigns for these facilities. © 2014 The Authors. Published by Oxford University Press on behalf of the Royal Astronomical Society.
- Published
- 2014
3. The Parkes pulsar timing array second data release: timing analysis.
- Author
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Reardon, D J, Shannon, R M, Cameron, A D, Goncharov, B, Hobbs, G B, Middleton, H, Shamohammadi, M, Thyagarajan, N, Bailes, M, Bhat, N D R, Dai, S, Kerr, M, Manchester, R N, Russell, C J, Spiewak, R, Wang, J B, and Zhu, X J
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BINARY pulsars ,PULSARS ,NEUTRON stars ,INTERSTELLAR medium ,STELLAR mass ,GRAVITATIONAL waves - Abstract
The main goal of pulsar timing array experiments is to detect correlated signals such as nanohertz-frequency gravitational waves. Pulsar timing data collected in dense monitoring campaigns can also be used to study the stars themselves, their binary companions, and the intervening ionized interstellar medium. Timing observations are extraordinarily sensitive to changes in path-length between the pulsar and the Earth, enabling precise measurements of the pulsar positions, distances and velocities, and the shapes of their orbits. Here we present a timing analysis of 25 pulsars observed as part of the Parkes Pulsar Timing Array (PPTA) project over time spans of up to 24 yr. The data are from the second data release of the PPTA, which we have extended by including legacy data. We make the first detection of Shapiro delay in four Southern pulsars (PSRs J1017−7156, J1125−6014, J1545−4550, and J1732−5049), and of parallax in six pulsars. The prominent Shapiro delay of PSR J1125−6014 implies a neutron star mass of M
p = 1.5 ± 0.2 M⊙ (68 per cent credibility interval). Measurements of both Shapiro delay and relativistic periastron advance in PSR J1600−3053 yield a large but uncertain pulsar mass of |$M_p = 2.06^{+0.44}_{-0.41}$| M⊙ (68 per cent credibility interval). We measure the distance to PSR J1909−3744 to a precision of 10 lyr, indicating that for gravitational wave periods over a decade, the pulsar provides a coherent baseline for pulsar timing array experiments. [ABSTRACT FROM AUTHOR]- Published
- 2021
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4. The Vela Pulsar: Results from the First Year of Fermi LAT Observations
- Author
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Abdo, A.A., Ackermann, M., Ajello, M., Allafort, A., Atwood, W.B., Baldini, L., Ballet, J., Barbiellini, G., Baring, M.G., Bastieri, D., Baughman, B.M., Bechtol, K., Bellazzini, R., Berenji, B., Blandford, R.D., Bloom, E.D., Bonamente, E., Borgland, A.W., Bouvier, A., Bregeon, J., Brez, A., Brigida, M., Bruel, P., Burnett, T.H., Buson, S., Caliandro, G. A., Cameron, R.A., Caraveo, P. A., Carrigan, S., Casandjian, J. M., Cecchi, C., Celik, O., Chekhtman, A., Cheung, C. C., Chiang, J., Ciprini, S., Claus, R., Cohen-Tanugi, J., Conrad, J., Dermer, C. D., de, Luca A., de, Palma F., Dormody, M., do, Couto e Silva E., Drell, P. S., Dubois, R., Dumora, D., Farnier, C., Favuzzi, C., Fegan, S. J., Focke, W. B., Fortin, P., Frailis, M., Funk, S., Fusco, P., Gargano, F., Gasparrini, D., Gehrels, N., Germani, S., Giavitto, G., Giebels, B., Giglietto, N., Giordano, F., Glanzman, T., Godfrey, G., Grenier, I. A., Grondin, M.-H., Grove, J. E., Guillemot, L., Guiriec, S., Hadasch, D., Harding, A. K., Hays, E., Hobbs, G., Horan, D., Hughes, R. E., Jackson, M. S., Johannesson, G., Johnson, A. S., Johnson, T. J., Johnson, W. N., Kerr, M., Knodlseder, J., Kuss, M., Lande, J., Latronico, L., Lee, S.-H., Lemoine-Goumard, M., Llena, Garde M., Longo, F., Loparco, F., Lott, B., Lovellette, M. N., Lubrano, P., Makeev, A., Manchester, R. N., Marelli, M., Mazziotta, M. N., McConville, W., McEnery, J. E., McGlynn, S., Meurer, C., Michelson, P. F., Mitthumsiri, W., Moiseev, A. A., Monte, C., Monzani, M. E., Morselli, A., Moskalenko, I. V., Murgia, S., Nolan, P. L., Norris, J. P., Noutsos, A., Nuss, E., Omodei, N., Orlando, E., Ormes, J. F., Paneque, D., Panetta, J. H., Parent, D., Pelassa, V., Pepe, M., Pesce-Rollins, M., Pierbattista, M., Piron, F., Porter, T. A., Raino, S., Rando, R., Ray, P. S., Razzano, M., Reimer, A., Reimer, O., Reposeur, T., Ritz, S., Rochester, L. S., Rodriguez, A. Y., Romani, R. W., Roth, M., Ryde, F., Sadrozinski, H. F.-W., Sander, A., Saz, Parkinson P. M., Sgro, C., Siskind, E. J., Smith, D. A., Smith, P. D., Spandre, G., Spinelli, P., Starck, J.-L., Strickman, M. S., Suson, D. J., Fukazawa, Y., Kamae, T., Katagiri, H., Kataoka, J., Kawai, N., Mizuno, T., Nakamori, T., Ohsugi, T., Ozaki, Masanobu, Takahashi, H., Takahashi, Tadayuki, Astrophysique Interprétation Modélisation (AIM (UMR7158 / UMR_E_9005 / UM_112)), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut national des sciences de l'Univers (INSU - CNRS)-Université Paris Diderot - Paris 7 (UPD7)-Centre National de la Recherche Scientifique (CNRS), Centre d'Etudes Nucléaires de Bordeaux Gradignan (CENBG), Université Sciences et Technologies - Bordeaux 1 (UB)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Laboratoire Leprince-Ringuet (LLR), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-École polytechnique (X)-Centre National de la Recherche Scientifique (CNRS), Laboratoire de Physique Théorique et Astroparticules (LPTA), Université Montpellier 2 - Sciences et Techniques (UM2)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Centre d'étude spatiale des rayonnements (CESR), Université Toulouse III - Paul Sabatier (UT3), Université de Toulouse (UT)-Université de Toulouse (UT)-Institut national des sciences de l'Univers (INSU - CNRS)-Observatoire Midi-Pyrénées (OMP), Institut de Recherche pour le Développement (IRD)-Université Toulouse III - Paul Sabatier (UT3), Université de Toulouse (UT)-Université de Toulouse (UT)-Institut national des sciences de l'Univers (INSU - CNRS)-Centre National d'Études Spatiales [Toulouse] (CNES)-Centre National de la Recherche Scientifique (CNRS)-Météo-France -Institut de Recherche pour le Développement (IRD)-Institut national des sciences de l'Univers (INSU - CNRS)-Centre National d'Études Spatiales [Toulouse] (CNES)-Centre National de la Recherche Scientifique (CNRS)-Météo-France -Centre National de la Recherche Scientifique (CNRS), Fermi-LAT, Abdo, A. A., Ackermann, M., Ajello, M., Allafort, A., Atwood, W. B., Baldini, L., Ballet, J., Barbiellini, G., Baring, M. G., Bastieri, D., Baughman, B. M., Bechtol, K., Bellazzini, R., Berenji, B., Blandford, D., Bloom, E. D., Bonamente, E., Borgland, A. W., Bouvier, A., Bregeon, J., Brez, A., Brigida, M., Bruel, P., Burnett, T. H., Buson, S., Caliandro, G. A., Cameron, R. A., Caraveo, P. A., Carrigan, S., Casandjian, J. M., Cecchi, C., Celik, O., Chekhtman, A., Cheung, C. C., Chiang, J., Ciprini, S., Claus, R., Cohen Tanugi, J., Conrad, J., Dermer, C. D., Luca, A. d., Palma, F. d., Dormody, M., Silva, E. D. E., Drell, P. S., Dubois, R., Dumora, D., Farnier, C., Favuzzi, C., Fegan, S. J., Focke, W. B., Fortin, P., Frailis, M., Fukazawa, Y., Funk, S., Fusco, P., Gargano, F., Gasparrini, D., Gehrels, N., Germani, S., Giavitto, G., Giebels, B., Giglietto, N., Giordano, F., Glanzman, T., Godfrey, G., Grenier, I. A., Grondin, M. H., Grove, J. E., Guillemot, L., Guiriec, S., Hadasch, D., Harding, A. K., Hays, E., Hobbs, G., Horan, D., Hughes, R. E., Jackson, M. S., Johannesson, G., Johnson, A. S., Johnson, T. J., Johnson, W. N., Kamae, T., Katagiri, H., Kataoka, J., Kawai, N., Kerr, M., Knodlseder, J., Kuss, M., Lande, J., Latronico, L., Lee, S. H., Lemoine Goumard, M., Garde, M. L., Longo, Francesco, Loparco, F., Lott, B., Lovellette, M. N., Lubrano, P., Makeev, A., Manchester, R. N., Marelli, M., Mazziotta, M. N., Mcconville, W., Mcenery, J. E., Mcglynn, S., Meurer, C., Michelson, P. F., Mitthumsiri, W., Mizuno, T., Moiseev, A. A., Monte, C., Monzani, M. E., Morselli, A., Moskalenko, I. V., Murgia, S., Nakamori, T., Nolan, P. L., Norris, J. P., Noutsos, A., Nuss, E., Ohsugi, T., Omodei, N., Orlando, E., Ormes, J. F., Ozaki, M., Paneque, D., Panetta, J. H., Parent, D., Pelassa, V., Pepe, M., Pesce Rollins, M., Pierbattista, M., Piron, F., Porter, T. A., Raino, S., Rando, R., Ray, P. S., Razzano, M., Reimer, A., Reimer, O., Reposeur, T., Ritz, S., Rochester, L. S., Rodriguez, A. Y., Romani, R. W., Roth, M., Ryde, F., Sadrozinski, H. F. W., Sander, A., Parkinson, P. M. S., Sgro, C., Siskind, E. J., Smith, D. A., Smith, P. D., Spandre, G., Spinelli, P., Starck, J. L., Strickman, M. S., Suson, D. J., Takahashi, H., Takahashi, T., Tanaka, T., Thayer, J. B., Thayer, J. G., Thompson, D. J., Tibaldo, L., Torres, D. F., Tosti, G., Tramacere, A., Usher, T. L., Etten, A. V., Vasileiou, V., Venter, C., Vilchez, N., Vitale, V., Waite, A. P., Wang, P., Watters, K., Weltevrede, P., Winer, B. L., Wood, K. S., Ylinen, T., Ziegler, M., Astrophysique Interprétation Modélisation (AIM (UMR_7158 / UMR_E_9005 / UM_112)), Centre National de la Recherche Scientifique (CNRS)-Institut national des sciences de l'Univers (INSU - CNRS)-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris Diderot - Paris 7 (UPD7), Université Sciences et Technologies - Bordeaux 1-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Université Fédérale Toulouse Midi-Pyrénées-Université Fédérale Toulouse Midi-Pyrénées-Institut national des sciences de l'Univers (INSU - CNRS)-Observatoire Midi-Pyrénées (OMP), Université Fédérale Toulouse Midi-Pyrénées-Centre National de la Recherche Scientifique (CNRS), 12006653 - Venter, Christo, Centre National de la Recherche Scientifique (CNRS)-École polytechnique (X)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), Observatoire Midi-Pyrénées (OMP), Météo France-Centre National d'Études Spatiales [Toulouse] (CNES)-Université Fédérale Toulouse Midi-Pyrénées-Centre National de la Recherche Scientifique (CNRS)-Institut de Recherche pour le Développement (IRD)-Météo France-Centre National d'Études Spatiales [Toulouse] (CNES)-Université Fédérale Toulouse Midi-Pyrénées-Centre National de la Recherche Scientifique (CNRS)-Institut de Recherche pour le Développement (IRD)-Centre National de la Recherche Scientifique (CNRS)-Institut national des sciences de l'Univers (INSU - CNRS)-Université Toulouse III - Paul Sabatier (UT3), and Université Fédérale Toulouse Midi-Pyrénées
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[PHYS.ASTR.HE]Physics [physics]/Astrophysics [astro-ph]/High Energy Astrophysical Phenomena [astro-ph.HE] ,Astrophysics::High Energy Astrophysical Phenomena ,general [Pulsars] ,Magnetosphere ,FOS: Physical sciences ,Fermi satellite ,Astrophysics ,Vela ,01 natural sciences ,Spectral line ,High Energy Gamma-ray Astronomy ,stars: neutron ,Spitzer Space Telescope ,Pulsar ,pulsars: general ,0103 physical sciences ,010303 astronomy & astrophysics ,Pulsars ,Physics ,High Energy Astrophysical Phenomena (astro-ph.HE) ,010308 nuclear & particles physics ,[SDU.ASTR.HE]Sciences of the Universe [physics]/Astrophysics [astro-ph]/High Energy Astrophysical Phenomena [astro-ph.HE] ,neutron [Stars] ,Astronomy and Astrophysics ,Light curve ,Astrophysics - Astrophysics of Galaxies ,Particle acceleration ,Pulsars: general ,[PHYS.ASTR.GA]Physics [physics]/Astrophysics [astro-ph]/Galactic Astrophysics [astro-ph.GA] ,13. Climate action ,Space and Planetary Science ,Astrophysics of Galaxies (astro-ph.GA) ,[SDU.ASTR.GA]Sciences of the Universe [physics]/Astrophysics [astro-ph]/Galactic Astrophysics [astro-ph.GA] ,Astrophysics - High Energy Astrophysical Phenomena ,Fermi Gamma-ray Space Telescope - Abstract
We report on analysis of timing and spectroscopy of the Vela pulsar using eleven months of observations with the Large Area Telescope on the Fermi Gamma-Ray Space Telescope. The intrinsic brightness of Vela at GeV energies combined with the angular resolution and sensitivity of the LAT allow us to make the most detailed study to date of the energy-dependent light curves and phase-resolved spectra, using a LAT-derived timing model. The light curve consists of two peaks (P1 and P2) connected by bridge emission containing a third peak (P3). We have confirmed the strong decrease of the P1/P2 ratio with increasing energy seen with EGRET and previous Fermi LAT data, and observe that P1 disappears above 20 GeV. The increase with energy of the mean phase of the P3 component can be followed with much greater detail, showing that P3 and P2 are present up to the highest energies of pulsation. We find significant pulsed emission at phases outside the main profile, indicating that magnetospheric emission exists over 80% of the pulsar period. With increased high-energy counts the phase-averaged spectrum is seen to depart from a power- law with simple exponential cutoff, and is better fit with a more gradual cutoff. The spectra in fixed-count phase bins are well fit with power-laws with exponential cutoffs, revealing a strong and complex phase dependence of the cutoff energy, especially in the peaks. By combining these results with predictions of the outer magnetosphere models that map emission characteristics to phase, it will be possible to probe the particle acceleration and the structure of the pulsar magnetosphere with unprecedented detail., Comment: 35 pages, 12 figures, accepted for publication in Astrophysical Journal
- Published
- 2010
5. Search for a radio pulsar in the remnant of supernova 1987A.
- Author
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Zhang, S-B, Dai, S, Hobbs, G, Staveley-Smith, L, Manchester, R N, Russell, C J, Zanardo, G, and Wu, X-F
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SUPERNOVA remnants ,PULSARS ,LARGE magellanic cloud ,RADIO telescopes ,ACTINIC flux - Abstract
We have observed the remnant of supernova SN 1987A (SNR 1987A), located in the Large Magellanic Cloud (LMC) to search for periodic and/or transient radio emission with the Parkes 64 m-diameter radio telescope. We found no evidence of a radio pulsar in our periodicity search and derived 8σ upper bounds on the flux density of any such source of $31\,\mu$ Jy at 1.4 GHz and $21\,\mu$ Jy at 3 GHz. Four candidate transient events were detected with greater than 7σ significance, with dispersion measures (DMs) in the range 150–840 cm
−3 pc. For two of them, we found a second pulse at slightly lower significance. However, we cannot at present conclude that any of these are associated with a pulsar in SNR 1987A. As a check on the system, we also observed PSR B0540−69, a young pulsar that also lies in the LMC. We found eight giant pulses at the DM of this pulsar. We discuss the implications of these results for models of the supernova remnant, neutron star formation, and pulsar evolution. [ABSTRACT FROM AUTHOR]- Published
- 2018
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6. HIGH-PRECISION TIMING OF FIVE MILLISECOND PULSARS: SPACE VELOCITIES, BINARY EVOLUTION, AND EQUIVALENCE PRINCIPLES.
- Author
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Gonzalez, M. E., Stairs, I. H., Ferdman, R. D., Freire, P. C. C., Nice, D. J., Demorest, P. B., Ransom, S. M., Kramer, M., Camilo, F., Hobbs, G., Manchester, R. N., and Lyne, A. G.
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PULSARS ,BINARY systems (Astronomy) ,RELATIVISTIC astrophysics ,ASTROPHYSICS ,NEUTRON stars - Abstract
We present high-precision timing of five millisecond pulsars (MSPs) carried out for more than seven years; four pulsars are in binary systems and one is isolated. We are able to measure the pulsars' proper motions and derive an estimate for their space velocities. The measured two-dimensional velocities are in the range 70-210 km s
-1 , consistent with those measured for other MSPs. We also use all the available proper motion information for isolated and binary MSPs to update the known velocity distribution for these populations. As found by earlier works, we find that the velocity distribution of binary and isolated MSPs are indistinguishable with the current data. Four of the pulsars in our observing program are highly recycled with low-mass white dwarf companions and we are able to derive accurate binary parameters for these systems. For three of these binary systems, we are able to place initial constraints on the pulsar masses with best-fit values in the range 1.0-1.6 M⊙ . The implications of the results presented here to our understanding of binary pulsar evolution are discussed. The updated parameters for the binary systems studied here, together with recently discovered similar systems, allowed us to update previous limits on the violation of the strong equivalence principle through the parameter |Δ| to 4.6 x 10-3 (95% confidence) and the violation of Lorentz invariance/momentum conservation through the parameter |α̂ to 5.5 x 10-20 (95% confidence). [ABSTRACT FROM AUTHOR]- Published
- 2011
- Full Text
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7. Characterizing the rotational irregularities of the Vela pulsar from 21 yr of phase-coherent timing.
- Author
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Shannon, R. M., Lentati, L. T., Kerr, M., Johnston, S., Hobbs, G., and Manchester, R. N.
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PULSARS ,NEUTRON stars ,MAGNETOSPHERE ,BAYESIAN analysis ,ASTRONOMICAL observations - Abstract
Pulsars show two classes of rotational irregularities that can be used to understand neutron-star interiors and magnetospheres: glitches and timing noise. Here we present an analysis of the Vela pulsar spanning nearly 21 yr of observation and including eight glitches. We identify the relative pulse number of all of the observations between glitches, with the only pulse-number ambiguities existing over glitch events. We use the phase coherence of the timing solution to simultaneously model the timing noise and glitches in a Bayesian framework, allowing us to select preferred models for both. We find the glitches can be described using only permanent and transient changes in spin frequency, i.e. no step changes in frequency derivative. For all of the glitches, we only need two exponentially decaying changes in spin frequency to model the transient components. In contrast to previous studies, we find that the dominant transient components decay on a common ≈1300 d time-scale, and that a larger fraction (≳25 per cent) of glitch amplitudes are associated with these transient components. We also detect shorterduration transient components of ≈25 d, as previously observed, but are limited in sensitivity to events with shorter durations by the cadence of our observations. The timing noise is well described by a steep power-law process that is independent of the glitches and subdominant to the glitch recovery. The braking index is constrained to be <8 with 95 per cent confidence. This methodology can be used to robustly measure the properties of glitches and timing noise in other pulsars. [ABSTRACT FROM AUTHOR]
- Published
- 2016
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8. Detection of 107 glitches in 36 southern pulsars.
- Author
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Yu, M., Manchester, R. N., Hobbs, G., Johnston, S., Kaspi, V. M., Keith, M., Lyne, A. G., Qiao, G. J., Ravi, V., Sarkissian, J. M., Shannon, R., and Xu, R. X.
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PULSAR detection ,RADIO telescopes ,RADIO frequency ,LINEAR systems ,PLANETARY magnetospheres ,PREDICTION models ,NEUTRONS - Abstract
Timing observations from the Parkes 64-m radio telescope for 165 pulsars between 1990 and 2011 have been searched for period glitches. Data spans for each pulsar ranged between 5.3 and 20.8 yr. From the total of 1911 yr of pulsar rotational history, 107 glitches were identified in 36 pulsars. Out of these glitches, 61 have previously been reported whereas 46 are new discoveries. Glitch parameters, both for the previously known and the new glitch detections, were measured by fitting the timing residual data. Observed relative glitch sizes Δνg/ν range between 10−10 and 10−5, where ν = 1/P is the pulse frequency. We confirm that the distribution of Δνg/ν is bimodal with peaks at approximately 10−9 and 10−6. Glitches are mostly observed in pulsars with characteristic ages between 103 and 105 yr, with large glitches mostly occurring in the younger pulsars. Exponential post-glitch recoveries were observed for 27 large glitches in 18 pulsars. The fraction Q of the glitch that recovers exponentially also has a bimodal distribution. Large glitches generally have low Q, typically just a few per cent, but large Q values are observed in both large and small glitches. Observed time constants for exponential recoveries ranged between 10 and 300 d with some tendency for longer time-scales in older pulsars. Shorter time-scale recoveries may exist but were not revealed by our data which typically have observation intervals of 2–4 weeks. For most of the 36 pulsars with observed glitches, there is a persistent linear increase in $\dot{\nu }$ (i.e. decrease in the slow-down rate $|\dot{\nu }|$) in the interglitch interval. Where an exponential recovery is also observed, the effects of this are superimposed on the linear increase in $\dot{\nu }$. In some but not all cases, the slope of the linear recovery changes at the time of a glitch. The $\ddot{\nu }$ values characterizing the linear changes in $\dot{\nu }$ are almost always positive and, after subtracting the magnetospheric component of the braking, are approximately proportional to the ratio of $|\dot{\nu }|$ and the interglitch interval, as predicted by vortex-creep models. [ABSTRACT FROM AUTHOR]
- Published
- 2013
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9. PSR J1910–5959A: A rare gravitational laboratory for testing white dwarf models.
- Author
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Corongiu, A., Venkatraman Krishnan, V., Freire, P. C. C., Kramer, M., Possenti, A., Geyer, M., Ridolfi, A., Abbate, F., Bailes, M., Barr, E. D., Balakrishnan, V., Buchner, S., Champion, D. J., Chen, W., Hugo, B. V., Karastergiou, A., Lyne, A. G., Manchester, R. N., Padmanabh, P. V., and Parthasarathy, A.
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BINARY pulsars ,STELLAR mass ,SPIN-orbit interactions ,TESTING laboratories ,GLOBULAR clusters ,PULSARS - Abstract
Context. PSR J1910−5959A is a binary millisecond pulsar in a 0.837 day circular orbit around a helium white dwarf (HeWD) companion. The position of this pulsar is 6.3 arcmin (∼74 core radii) away from the optical centre of the globular cluster (GC) NGC 6752. Given the large offset, the association of the pulsar with the GC has been debated. Aims. We aim to obtain precise measurements of the masses of the stars in the system along with secular orbital parameters, which will help identify if the system belongs to the GC. Methods. We have made use of archival Parkes 64 m 'Murriyang' telescope data and carried out observations with the MeerKAT telescope with different backends and receivers over the last two decades. Pulse times of arrival were obtained from these using standard pulsar data reduction techniques and analysed using state-of-the-art Bayesian pulsar timing techniques. We also performed an analysis of the pulsar's total intensity and polarisation profile to understand the interstellar scattering along the line of sight, and we determined the pulsar's geometry by fitting the rotating vector model to the polarisation data. Results. We obtain precise measurements of several post-Keplerian parameters: the range, r = 0.202(6) T
⊙ , and shape, s = 0.999823(4), of the Shapiro delay, from which we infer: the orbital inclination to be 88.9−0.14 +0.15 deg; the masses of the pulsar and the companion to be 1.55(7) M⊙ and 0.202(6) M⊙ , respectively; a secular change in the orbital period Ṗb = −53−6.0 +7.4 × 10−15 s s−1 that proves the GC association; and a secular change in the projected semi-major axis of the pulsar, ẋ = −40.7−8.2 +7.3 × 10−16 s s−1 , likely caused by the spin–orbit interaction from a misaligned HeWD spin, at odds with the likely isolated binary evolution of the system. We also discuss some theoretical models for the structure and evolution of white dwarfs in neutron star–white dwarf binaries, using PSR J1910−5959A's companion as a test bed. Conclusions. PSR J1910−5959A is a rare system for which several parameters of both the pulsar and the HeWD companion can be accurately measured. As such, it is a test bed for discriminating between alternative models of HeWD structure and cooling. [ABSTRACT FROM AUTHOR]- Published
- 2023
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10. Observations of six glitches in PSR B1737−30.
- Author
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Zou, W. Z., Wang, N., Manchester, R. N., Urama, J. O., Hobbs, G., Liu, Z. Y., and Yuan, J. P.
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PULSARS ,ASTRONOMICAL observations ,DIPOLE moments ,MAGNETIC dipoles ,STARS - Abstract
Six glitches have been recently observed in the rotational frequency of the young pulsar PSR B1737−30 (J1740−3015) using the 25-m Nanshan telescope of Urumqi Observatory. With a total of 20 glitches in 20 yr, it is one of the most frequently glitching pulsars of the ∼1750 known pulsars. Glitch amplitudes are very variable with fractional increases in rotation rate ranging from 10
−9 to 10−6 . Interglitch intervals are also very variable, but no relationship is observed between interval and the size of the preceding glitch. There is a persistent increase in , opposite in sign to that expected from slowdown with a positive braking index, which may result from changes in the effective magnetic dipole moment of the star during the glitch. [ABSTRACT FROM AUTHOR]- Published
- 2008
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11. The Parkes Multibeam Pulsar Survey – VI. Discovery and timing of 142 pulsars and a Galactic population analysis.
- Author
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Lorimer, D. R., Faulkner, A. J., Lyne, A. G., Manchester, R. N., Kramer, M., McLaughlin, M. A., Hobbs, G., Possenti, A., Stairs, I. H., Camilo, F., Burgay, M., D'Amico, N., Corongiu, A., and Crawford, F.
- Subjects
STATISTICAL astronomy ,NEUTRON stars ,PULSAR detection ,STELLAR populations ,PARAMETERS (Statistics) ,BINARY star orbits - Abstract
We present the discovery and follow-up observations of 142 pulsars found in the Parkes 20-cm multibeam pulsar survey of the Galactic plane. These new discoveries bring the total number of pulsars found by the survey to 742. In addition to tabulating spin and astrometric parameters, along with pulse width and flux density information, we present orbital characteristics for 13 binary pulsars which form part of the new sample. Combining these results from another recent Parkes multibeam survey at high Galactic latitudes, we have a sample of 1008 normal pulsars which we use to carry out a determination of their Galactic distribution and birth rate. We infer a total Galactic population of potentially detectable pulsars (i.e. those beaming towards us) having 1.4-GHz luminosities above 0.1 mJy kpc
2 . Adopting the Tauris & Manchester beaming model, this translates to a total of active radio pulsars in the Galaxy above this luminosity limit. Using a pulsar current analysis, we derive the birth rate of this population to be pulsars per century. An important conclusion from our work is that the inferred radial density function of pulsars depends strongly on the assumed distribution of free electrons in the Galaxy. As a result, any analyses using the most recent electron model of Cordes & Lazio predict a dearth of pulsars in the inner Galaxy. We show that this model can also bias the inferred pulsar scaleheight with respect to the Galactic plane. Combining our results with other Parkes multibeam surveys we find that the population is best described by an exponential distribution with a scaleheight of 330 pc. Surveys underway at Parkes and Arecibo are expected to improve the knowledge of the radial distribution outside the solar circle, and to discover several hundred new pulsars in the inner Galaxy. [ABSTRACT FROM AUTHOR]- Published
- 2006
- Full Text
- View/download PDF
12. Discovery of an extremely intermittent periodic radio source.
- Author
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Surnis, M P, Rajwade, K M, Stappers, B W, Younes, G, Bezuidenhout, M C, Caleb, M, Driessen, L N, Jankowski, F, Malenta, M, Morello, V, Sanidas, S, Barr, E, Kramer, M, Fender, R, and Woudt, P
- Subjects
NEUTRON stars ,MAGNETIC flux density ,MAGNETARS ,X-ray telescopes ,PULSARS - Abstract
We report the serendipitous discovery of an extremely intermittent radio pulsar, PSR J1710−3452, with a relatively long spin period of 10.4 s. The object was discovered through the detection of 97 bright radio pulses in only one out of 66 epochs of observations spanning almost three years. The bright pulses have allowed the source to be localized to a precision of 0.5 arcsec through radio imaging. We observed the source location with the Swift X-ray telescope but did not detect any significant X-ray emission. We did not identify any high-energy bursts or multifrequency counterparts for this object. The solitary epoch of detection hinders the calculation of the surface magnetic field strength, but the long period and the microstructure in the single-pulses resembles the emission of radio-loud magnetars. If this is indeed a magnetar, it is located at a relatively high Galactic latitude (2.9°), making it potentially one of the oldest and the most intermittent magnetars known in the Galaxy. The very short activity window of this object is unique and may point towards a yet undetected population of long period, highly transient radio emitting neutron stars. [ABSTRACT FROM AUTHOR]
- Published
- 2023
- Full Text
- View/download PDF
13. Estimation of the Pulsar Braking Index Using the Evolution of the Rotational Kinetic Energy Loss Rate. Testing on the Crab Pulsar.
- Author
-
Zhang, Jianwei
- Subjects
ENERGY dissipation ,KINETIC energy ,NEUTRON stars ,GRANULAR flow ,ANGULAR velocity - Abstract
The slowdown mechanism of rotating neutron stars (NSs) has long been an important topic in pulsar astronomy, which is still an open question of detailed debate. It is widely understood that it arises from the loss of the rotational kinetic energy () through the magnetic dipole radiation (MDR). This simple model would lead to a relation , where and are the spin angular velocity and its time derivative. However, a sole MDR torque may be oversimple and incorrect, and the above relation could be written in a more general form , where is a constant, and is known as the braking index, being 3 for the MDR model. The value of a pulsar could in principle be directly measured through its observation. However, it is difficult to measure the values of due to the effects of the timing noise or glitches, making the sample of pulsars with reliable observations is very tiny (the number ~10). Therefore, this study aims to estimate a pulsar's value without relying on the observation of , by employing a simple and convenient evolution model. In which, the information about the real age of the target pulsar is required as input. Here, we applied this model to the Crab pulsar since it is the only NS source with a known age. Our results inferred its value to be , and also constrained several of its initial parameters, e.g., its initial spin period and energy loss rate were limited to be [s] and [erg/s] , respectively. Our above estimated value for the Crab pulsar is consistent with the observation based on its measurement, as . The departure of its value from the canonical 3 may be interpreted by a combination of a particle wind flow torque and an increase of the magnetic inclination angle, along with the classical MDR model. Our method may be applied to approximately evaluate the values for more Crab-like pulsars in the future if their true ages can be accurately measured through a new methodology. [ABSTRACT FROM AUTHOR]
- Published
- 2023
- Full Text
- View/download PDF
14. Matter ejections behind the highs and lows of the transitional millisecond pulsar PSR J1023+0038.
- Author
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Baglio, M. C., Coti Zelati, F., Campana, S., Busquet, G., D'Avanzo, P., Giarratana, S., Giroletti, M., Ambrosino, F., Crespi, S., Miraval Zanon, A., Hou, X., Li, D., Li, J., Wang, P., Russell, D. M., Torres, D. F., Alabarta, K., Casella, P., Covino, S., and Bramich, D. M.
- Subjects
PULSARS ,BINARY pulsars ,SPECTRAL energy distribution ,SURVEILLANCE radar ,OPTICAL disks ,X-ray binaries ,POLARIMETRY ,ACCRETION disks - Abstract
Transitional millisecond pulsars are an emerging class of sources that link low-mass X-ray binaries to millisecond radio pulsars in binary systems. These pulsars alternate between a radio pulsar state and an active low-luminosity X-ray disc state. During the active state, these sources exhibit two distinct emission modes (high and low) that alternate unpredictably, abruptly, and incessantly. X-ray to optical pulsations are observed only during the high mode. The root cause of this puzzling behaviour remains elusive. This paper presents the results of the most extensive multi-wavelength campaign ever conducted on the transitional pulsar prototype, PSR J1023+0038, covering from the radio to X-rays. The campaign was carried out over two nights in June 2021 and involved 12 different telescopes and instruments, including XMM-Newton, HST, VLT/FORS2 (in polarimetric mode), ALMA, VLA, and FAST. By modelling the broadband spectral energy distributions in both emission modes, we show that the mode switches are caused by changes in the innermost region of the accretion disc. These changes trigger the emission of discrete mass ejections, which occur on top of a compact jet, as testified by the detection of at least one short-duration millimetre flare with ALMA at the high-to-low mode switch. The pulsar is subsequently re-enshrouded, completing our picture of the mode switches. [ABSTRACT FROM AUTHOR]
- Published
- 2023
- Full Text
- View/download PDF
15. X-ray luminosity function of high-mass X-ray binaries: Studying the signatures of different physical processes using detailed binary evolution calculations.
- Author
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Misra, Devina, Kovlakas, Konstantinos, Fragos, Tassos, Lazzarini, Margaret, Bavera, Simone S., Lehmer, Bret D., Zezas, Andreas, Zapartas, Emmanouil, Zepei Xing, Andrews, Jeff J., Dotter, Aaron, Rocha, Kyle Akira, Srivastava, Philipp M., and Meng Sun
- Subjects
STELLAR structure ,BLACK holes ,STELLAR evolution ,LUMINOSITY ,ACCRETION (Astrophysics) ,SUPERNOVA remnants ,X-ray binaries ,ACCRETION disks - Abstract
Context. Many physical processes taking place during the evolution of binary stellar systems remain poorly understood. The everexpanding observational sample of X-ray binaries (XRBs) makes them excellent laboratories for constraining binary evolution theory. Such constraints and useful insights can be obtained by studying the effects of various physical assumptions on synthetic X-ray luminosity functions (XLFs) and comparing them with observed XLFs. Aims. In this work we focus on high-mass X-ray binaries (HMXBs) and study the effects on the XLF of various, poorly constrained assumptions regarding physical processes, such as the common-envelope phase, core collapse, and wind-fed accretion. Methods. We used the new binary population synthesis code POSYDON, which employs extensive precomputed grids of detailed stellar structure and binary evolution models, to simulate the entire evolution of binaries. We generated 96 synthetic XRB populations corresponding to different combinations of model assumptions, including different prescriptions for supernova kicks, supernova remnant masses, common-envelope evolution, circularization at the onset of Roche-lobe overflow, and observable wind-fed accretion. Results. The generated HMXB XLFs are feature-rich, deviating from the commonly assumed single power law. We find a break in our synthetic XLF at luminosity ~1038 erg s1, similar to observed XLFs. However, we also find a general overabundance of XRBs (up to a factor of ~10 for certain model parameter combinations) driven primarily by XRBs with black hole accretors. Assumptions about the transient behavior of Be XRBs, asymmetric supernova kicks, and common-envelope physics can significantly affect the shape and normalization of our synthetic XLFs. We find that less well-studied assumptions regarding the circularization of the orbit at the onset of Roche-lobe overflow and criteria for the formation of an X-ray-emitting accretion disk around wind-accreting black holes can also impact our synthetic XLFs and reduce the discrepancy with observations. Conclusions. Our synthetic XLFs do not always agree well with observations, especially at intermediate X-ray luminosities, which is likely due to uncertainties in the adopted physical assumptions. While some model parameters leave distinct imprints on the shape of the synthetic XLFs and can reduce this deviation, others do not have a significant effect overall. Our study reveals the importance of large-scale parameter studies, highlighting the power of XRBs in constraining binary evolution theory. [ABSTRACT FROM AUTHOR]
- Published
- 2023
- Full Text
- View/download PDF
16. Nanohertz gravitational wave astronomy during SKA era: An InPTA perspective.
- Author
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Joshi, Bhal Chandra, Gopakumar, Achamveedu, Pandian, Arul, Prabu, Thiagaraj, Dey, Lankeswar, Bagchi, Manjari, Desai, Shantanu, Tarafdar, Pratik, Rana, Prerna, Maan, Yogesh, BATRA, Neelam Dhanda, Girgaonkar, Raghav, Agarwal, Nikita, Arumugam, Paramasivan, Basu, Avishek, Bathula, Adarsh, Dandapat, Subhajit, Gupta, Yashwant, Hisano, Shinnosuke, and Kato, Ryo
- Subjects
GRAVITATIONAL wave astronomy ,SUPERMASSIVE black holes ,BINARY black holes ,RADIO telescopes ,BL Lacertae objects ,PULSARS ,GRAVITATIONAL waves - Abstract
Decades long monitoring of millisecond pulsars, which exhibit highly stable rotational periods in pulsar timing array experiments is on the threshold of discovering nanohertz stochastic gravitational wave background. This paper describes the Indian pulsar timing array (InPTA) experiment, which employs the upgraded Giant Metrewave Radio Telescope (uGMRT) for timing an ensemble of millisecond pulsars for this purpose. We highlight InPTA's observation strategies and analysis methods, which are relevant for a future PTA experiment with the more sensitive Square Kilometer Array (SKA) telescope. We show that the unique multi-sub-array multi-band wide-bandwidth frequency coverage of the InPTA, provides dispersion measure estimates with unprecedented precision for PTA pulsars, e.g., ∼ 2 × 10 - 5 pc cm - 3 for PSR J1909-3744. Configuring the SKA-low and SKA-mid as two and four sub-arrays, respectively, it is shown that comparable precision is achievable, using observation strategies similar to those pursued by the InPTA, for a larger sample of 62 pulsars, requiring about 26 and 7 h per epoch for the SKA-mid and the SKA-low telescopes, respectively. We also review the ongoing efforts to develop PTA-relevant general relativistic constructs that will be required to search for nanohertz gravitational waves from isolated super-massive black hole binary systems like blazar OJ 287. These efforts should be relevant to pursue persistent multi-messenger gravitational wave astronomy during the forthcoming era of the SKA telescope, the thirty meter telescope, and the next-generation event horizon telescope. [ABSTRACT FROM AUTHOR]
- Published
- 2022
- Full Text
- View/download PDF
17. Constraints on population I/II neutron star-black hole binary formation by gravitational wave and radio observations.
- Author
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Kinugawa, Tomoya, Nakamura, Takashi, and Nakano, Hiroyuki
- Subjects
GRAVITATIONAL waves ,RADIO waves ,NEUTRON stars ,PULSAR detection ,NEUTRONS ,BINARY pulsars - Abstract
Two neutron star (NS)-black hole (BH) binaries, GW200105 and GW200115 found in the LIGO/Virgo O3b run have smaller BH mass of 6–9 M
⊙ , which is consistent with Population I and II origin. Our population synthesis simulations using 106 Population I and II binaries with appropriate initial parameters show consistent binary mass, event rate, no detection of radio pulsar (PSR), and BH binaries in our Galaxy so far. Especially, we found possible progenitors of GW200105 and GW200115, which were formed at redshift z = 0.15 and z = 1.6 with binary mass of |$(34\,{\mathrm{ M}}_{\odot },\, 9.2\,{\mathrm{ M}}_{\odot })$| and |$(23.7\,{\mathrm{ M}}_{\odot },\, 10.6\,{\mathrm{ M}}_{\odot })$| , respectively. The final masses of these binaries are |$(6.85\,{\mathrm{ M}}_{\odot },\, 2.14\,{\mathrm{ M}}_{\odot })$| and |$(6.04\,{\mathrm{ M}}_{\odot },\, 1.31\,{\mathrm{ M}}_{\odot })$| which look like |$(9.0_{-1.7}^{+1.7}\,{\mathrm{ M}}_{\odot },\, 1.91_{-0.24}^{+0.33}\,{\mathrm{ M}}_{\odot })$| of GW200105 and |$(5.9_{-2.5}^{+2.0}\,{\mathrm{ M}}_{\odot },\, 1.44_{-0.29}^{+0.85}\,{\mathrm{ M}}_{\odot })$| of GW200115, respectively. We also estimate that 2.68–19.7 PSR–BH binaries in our Galaxy will be observed by SKA. The existence of NS–BHs in our Galaxy can be confirmed in future SKA era. Using the GW observation of NS–BH mergers and the radio observation of PSR–BHs in future, we can get more severe constraints on the NS–BH formation process. [ABSTRACT FROM AUTHOR]- Published
- 2022
- Full Text
- View/download PDF
18. On the fractional glitch recoveries and pulsar spin properties.
- Author
-
Eze, Christian I., Iyida, Evaristus U., and Eya, Innocent O.
- Subjects
NEUTRON stars ,MOMENTS of inertia - Abstract
Pulsar glitches are sudden jumps in the spin frequency of an otherwise steadily spinning down neutron star. A glitch, in many pulsars, is followed by a recovery phase in which the pulsars return fully or partially to the pre‐glitch state on a wide range of time scales. This paper statistically investigates the behavior of the glitch recovery parameter, Q, and its relationship with the pulsar rotational parameters. The Q for the different sub‐classes of the glitch sizes appear to arise from different distributions, suggesting a possible different path of recovery or interior dynamics for the recovery of glitches of different sizes. While the Q has moderate relation with characteristic age, rotational frequency, fractional moment of inertia, and coupling parameter, it shows a very weak correlation with spin‐down rate. The implications are discussed. Glitch and glitch recovery appear to have different underlying physics, but both point to some dynamical changes within the interior of the neutron star. [ABSTRACT FROM AUTHOR]
- Published
- 2022
- Full Text
- View/download PDF
19. On the pulsar spin frequency derivatives and the glitch activity.
- Author
-
Eya, I. O., Alhassan, J. A., Iyida, E. U., Chukwude, A. E., and Urama, J. O.
- Subjects
NEUTRON stars ,MOMENTS of inertia ,MOMENTUM transfer ,PULSARS ,SUPERFLUIDITY - Abstract
The number of sudden spin-ups in radio pulsars known as pulsar glitches has increased over the years. Though a consensus has not been reached with regards to the actual cause of the phenomenon, the electromagnetic braking torque on the crust quantified via the magnitude of pulsar spin frequency first derivative, ν ˙ is a key factor in mechanisms put across toward the understanding of the underlying principles involved. The glitch size has been used to establish a quantity used to constrain the mean possible change in pulsar spin frequency (ν) per year due to a glitch known as the 'glitch activity'. Traditionally, the glitch activity parameter A g is calculated from the cumulative glitch sizes in a pulsar at a certain observational time span. In this analysis, we test the possibility of quantifying the A g with the pulsars main spin frequency derivatives (i.e. ν ˙ and ν ¨ ). In this approach, the ratio of the frequency derivatives, i.e. | ν ¨ | / ν ˙ 2 is seen to constrains the glitch activity in radio pulsars. The glitch size is found to be independent of the magnitude of the ratio, however, based on the recorded glitch events, the lower end of | ν ¨ | / ν ˙ 2 distribution appear to have more glitches. The minimum inter-glitch time interval in the ensemble of pulsars scale with the ratio as t g ∼ 3.35 (| ν ¨ | / ν ˙ 2) 0.23 . The A g quantified in this analysis supports the idea of neutron star inner-crust superfluid being the reservoir of momentum transferred during glitches. It suggests that the moment of inertia of the inner-crust to be at most 10% of the entire neutron star moment of inertia. [ABSTRACT FROM AUTHOR]
- Published
- 2022
- Full Text
- View/download PDF
20. Peculiar Objects in the Birthplaces of Radio Pulsars—Stellar-Mass Black Hole Candidates.
- Author
-
Chmyreva, L. and Beskin, G. M.
- Subjects
BLACK holes ,BIRTHPLACES ,NEUTRON stars - Abstract
Abstract—We perform a search for stellar-mass black hole candidates in the spatial regions with increased probability of their occurrence, isolated based on the evolutionary scenarios for compact objects originating in disrupted binaries. We analyze the sources located in these regions with available spectral or photometric data, as well as measured proper motions and distances. Nine objects whose characteristics correspond to the theoretical predictions for the observational manifestations of an isolated black hole are marked for further study as black hole candidates. [ABSTRACT FROM AUTHOR]
- Published
- 2022
- Full Text
- View/download PDF
21. Properties of the emission region in pulsars with opposite subpulse drift directions in different profile components.
- Author
-
Tedila, H. M., Yuen, R., and Han, X. H.
- Subjects
PULSARS ,MAGNETOSPHERE ,PLASMA flow - Abstract
We investigate properties of the emission region as revealed by drifting subpulses of opposite drift directions at different parts of a pulse profile by using the rotating carousel model in an obliquely rotating pulsar magnetosphere of multiple emission states. Subpulse emission is assumed coming from m discrete emission areas that are distributed around the magnetic axis on a rotating carousel. The flow rate of the emission areas is determined by the E × B drift in an emission state, designated by the parameter y , in which E and the associated flow rate are dependent on y . In this model, subpulses appear to drift in an emission state if a relative speed exists between the plasma flow and corotation, and the diversity in the drift rates and directions corresponds to the relative speed being different in different parts of a profile. We apply the model to three pulsars that exhibit drifting subpulses of opposite drift directions to identify the emission states and the values of m . Our results show that different drifting subpulses correspond to particular values of m and y , and the latter implies that different emission states can coexist and operate concurrently in an emission region. We find that m does not show clear dependency on either the obliquity angle or emission state. We demonstrate that subpulse arrangement may vary across an emission region meaning that it is not always uniform on a carousel. We discuss drifting subpulses of opposite drift directions and subpulse drift-rate switching in terms of different emission states in our model, and speculate that they may be two manifestations of the same underlying mechanism. [ABSTRACT FROM AUTHOR]
- Published
- 2021
- Full Text
- View/download PDF
22. The slow rise and recovery of the 2019 Crab pulsar glitch.
- Author
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Shaw, B, Keith, M J, Lyne, A G, Mickaliger, M B, Stappers, B W, Turner, J D, and Weltevrede, P
- Subjects
CRABS ,PULSARS ,NEUTRON stars - Abstract
We present updated measurements of the Crab pulsar glitch of 2019 July 23 using a data set of pulse arrival times spanning ∼5 months. On MJD 58687, the pulsar underwent its seventh largest glitch observed to date, characterized by an instantaneous spin-up of ∼1 μ Hz. Following the glitch, the pulsar's rotation frequency relaxed exponentially towards pre-glitch values over a time-scale of approximately 1 week, resulting in a permanent frequency increment of ∼0.5 μ Hz. Due to our semicontinuous monitoring of the Crab pulsar, we were able to partially resolve a fraction of the total spin-up. This delayed spin-up occurred exponentially over a time-scale of ∼18 h. This is the sixth Crab pulsar glitch for which part of the initial rise was resolved in time and this phenomenon has not been observed in any other glitching pulsars, offering a unique opportunity to study the microphysical processes governing interactions between the neutron star interior and the crust. [ABSTRACT FROM AUTHOR]
- Published
- 2021
- Full Text
- View/download PDF
23. Population synthesis of young neutron stars.
- Author
-
Igoshev, Andrei P. and Kholtygin, Alexander F.
- Abstract
We investigate the fortune of young neutron stars (NS) in the whole volume of the Milky Way with new code for population synthesis. We start our modeling from the birth of massive OB stars and follow their motion in the Galaxy up to the Supernova explosion. Next we integrate the equations of motion of NS in the averaged gravitational potential of the Galaxy. We estimate the mean kick velocities from a comparison the model Z and R-distributions of radio emitting NS with that for galactic NS accordingly ATNF pulsar catalog. We follow the history of the rotational velocity and the surface magnetic field of NS taking into account the significant magnetic field decay during the first million year of a neutron star's life. The derived value for the mean time of ohmic decay is 2.3ċ105 years. We model the subsample of galactic radio pulsars which can be detected with available radio telescopes, using a radio beaming model with inhomogeneous distribution of the radio emission in the cone. The distributions functions of the pulsar periods P, period derivatives Ṗ and surface magnetic fields B appear to be in a close agreement with those obtained from an ensemble of neutron stars in the ATNF catalogue. [ABSTRACT FROM PUBLISHER]
- Published
- 2012
- Full Text
- View/download PDF
24. Spin-down rate of the transitional millisecond pulsar PSR J1023+0038 in the optical band with Aqueye+.
- Author
-
Burtovoi, Aleksandr, Zampieri, Luca, Fiori, Michele, Naletto, Giampiero, Spolon, Alessia, Barbieri, Cesare, Papitto, Alessandro, and Ambrosino, Filippo
- Subjects
PHOTON detectors ,PULSARS ,NEUTRON stars ,TIME measurements ,X-ray binaries - Abstract
We present a timing analysis of the transitional millisecond pulsar PSR J1023+0038 using observations taken between 2018 January and 2020 January with the high time resolution photon counter Aqueye+ mounted at the 1.82 m Copernicus telescope in Asiago. We report the first measurement of the timing solution and the frequency derivative of PSR J1023+0038 based entirely on optical data. The spin-down rate of the pulsar is (−2.53 ± 0.04) × 10
−15 Hz2 , which is ∼20 per cent slower than that measured from the X-ray observations taken in 2013–2016 and ∼5 per cent faster than that measured in the radio band during the rotation-powered state. [ABSTRACT FROM AUTHOR]- Published
- 2020
- Full Text
- View/download PDF
25. On the origin of GW190425.
- Author
-
Romero-Shaw, Isobel M, Farrow, Nicholas, Stevenson, Simon, Thrane, Eric, and Zhu, Xing-Jiang
- Subjects
BINARY stars ,NEUTRON stars ,B stars ,MASS transfer ,RADIO astronomy ,NEUTRON counters - Abstract
The LIGO/Virgo collaborations recently announced the detection of a binary neutron star merger, GW190425. The mass of GW190425 is significantly larger than the masses of Galactic double neutron stars known through radio astronomy. We hypothesize that GW190425 formed differently from Galactic double neutron stars, via unstable 'case BB' mass transfer. According to this hypothesis, the progenitor of GW190425 was a binary consisting of a neutron star and a ∼4– |$5\, {\mathrm{ M}_\odot }$| helium star, which underwent common-envelope evolution. Following the supernova of the helium star, an eccentric double neutron star was formed, which merged in |${\lesssim }10\, {\rm Myr}$|. The helium star progenitor may explain the unusually large mass of GW190425, while the short time to merger may explain why similar systems are not observed in radio. To test this hypothesis, we measure the eccentricity of GW190425 using publicly available LIGO/Virgo data. We constrain the eccentricity at |$10\, {\rm Hz}$| to be e ≤ 0.007 with |$90{{\ \rm per\ cent}}$| confidence. This provides no evidence for or against the unstable mass transfer scenario, because the binary is likely to have circularized to e ≲ 10
−4 by the time it was detected. Future detectors will help to reveal the formation channel of mergers similar to GW190425 using eccentricity measurements. [ABSTRACT FROM AUTHOR]- Published
- 2020
- Full Text
- View/download PDF
26. Radiative pulsar magnetospheres: aligned rotator.
- Author
-
Pétri, J
- Subjects
MAGNETOSPHERE ,PARTICLE acceleration ,OHM'S law ,NEUTRON stars ,STELLAR rotation ,PULSARS - Abstract
Force-free neutron star magnetospheres are nowadays well known and found through numerical simulations. Even extension to general relativity has recently been achieved. However, those solutions are by definition dissipationless, meaning that the star is unable to accelerate particles and let them radiate any photon. Interestingly, the force-free model has no free parameter however it must be superseded by a dissipative mechanism within the plasma. In this Letter, we investigate the magnetosphere electrodynamics for particles moving in the radiation reaction regime, using the limit where acceleration is fully balanced by radiation, also called Aristotelian dynamics. An Ohm's law is derived, from which the dissipation rate is controlled by a one parameter family of solutions depending on the pair multiplicity κ. The spatial extension of the dissipation zone is found self-consistently from the simulations. We show that the radiative magnetosphere of an aligned rotator tends to the force-free regime whenever the pair multiplicity becomes moderately large, κ ≫ 1. However, for low multiplicity, a substantial fraction of the spin-down energy goes into particle acceleration and radiation in addition to the Poynting flux, the latter remaining only dominant for large multiplicities. We show that the work done on the plasma occurs predominantly in the equatorial current sheet right outside the light-cylinder. [ABSTRACT FROM AUTHOR]
- Published
- 2020
- Full Text
- View/download PDF
27. The minimum rotation period of millisecond pulsars.
- Author
-
Ertan, Ünal and Alpar, M Ali
- Subjects
NEUTRON stars ,X-ray binaries ,MAGNETIC dipoles ,NEUTRON diffusion ,ROTATIONAL motion ,BINARY pulsars ,PULSARS - Abstract
A simple and natural explanation for the minimum period of millisecond pulsars follows from a correlation between the accretion rate and the frozen surface dipole magnetic field resulting from ohmic diffusion through the neutron star crust in initial stages of accretion in low-mass X-ray binaries. [ABSTRACT FROM AUTHOR]
- Published
- 2021
- Full Text
- View/download PDF
28. XMM-Newton observations of PSR J0726−2612, a radio-loud XDINS.
- Author
-
Rigoselli, Michela, Mereghetti, Sandro, Suleimanov, Valery, Potekhin, Alexander Y., Turolla, Roberto, Taverna, Roberto, and Pintore, Fabio
- Subjects
X-ray spectra ,NEUTRON stars ,PULSARS ,X-rays - Abstract
We present the results of an XMM-Newton observation of the slowly rotating (P = 3.4 s), highly magnetized (B ≈ 3 × 10
13 G) radio pulsar PSR J0726–2612. A previous X-ray observation with the Chandra satellite showed that some of the properties of PSR J0726–2612 are similar to those of the X-ray-dim isolated neutron stars (XDINSs), a small class of nearby slow pulsars characterized by purely thermal X-ray spectra and undetected in the radio band. We confirm the thermal nature of the X-ray emission of PSR J0726–2612, which can be fitted by the sum of two blackbodies with temperatures k T 1 = 0. 074 − 0.011 + 0.006 $ kT_1 = 0.074_{-0.011}^{+0.006} $ kT1 =0.074+0.006 -0.011 keV and k T 2 = 0. 14 − 0.02 + 0.04 $ kT_2=0.14_{-0.02}^{+0.04} $ kT2 =0.14+0.004 -0.002 keV and emitting radii R 1 = 10. 4 − 2.8 + 10.8 $ R_1=10.4_{-2.8}^{+10.8} $ R1 =10.4+10.8 -2.8 km and R 2 = 0. 5 − 0.3 + 0.9 $ R_2=0.5_{-0.3}^{+0.9} $ R2 =0.5+0.9 -0.3 km, respectively (assuming a distance of 1 kpc). A broad absorption line modeled with a Gaussian profile centered at 0. 39 − 0.03 + 0.02 $ 0.39_{-0.03}^{+0.02} $ 0.39+0.02 -0.03 keV is required in the fit. The pulse profile of PSR J0726–2612 is characterized by two peaks with similar intensity separated by two unequal minima, a shape and pulsed fraction that cannot be reproduced without invoking magnetic beaming of the X-ray emission. The presence of a single radio pulse suggests that in PSR J0726–2612 the angles that the dipole axis and the line of sight make with the rotation axis, ξ and χ, respectively, are similar. This geometry differs from that of the two radio-silent XDINSs with double-peaked pulse profiles similar to that of PSR J0726–2612, for which ξ ∼ 90° and χ ∼ 45° have recently been estimated. These results strengthen the similarity between PSR J0726–2612 and the XDINSs and support the possibility that the lack of radio emission from the latter might simply be due to an unfavorable viewing geometry. [ABSTRACT FROM AUTHOR]- Published
- 2019
- Full Text
- View/download PDF
29. Thermal X-ray emission identified from the millisecond pulsar PSR J1909–3744.
- Author
-
Webb, N. A., Leahy, D., Guillot, S., Baillot d'Etivaux, N., Barret, D., Guillemot, L., Margueron, J., and Miller, M. C.
- Subjects
PULSARS ,X-rays ,NEUTRON stars ,EQUATIONS of state ,STELLAR mass ,PAIR production ,MASS measurement - Abstract
Context. Pulsating thermal X-ray emission from millisecond pulsars can be used to obtain constraints on the neutron star equation of state, but to date only five such sources have been identified. Of these five millisecond pulsars, only two have well-constrained neutron star masses, which improve the determination of the radius via modelling of the X-ray waveform. Aims. We aim to find other millisecond pulsars that already have well-constrained mass and distance measurements that show pulsed thermal X-ray emission in order to obtain tight constraints on the neutron star equation of state. Methods. The millisecond pulsar PSR J1909–3744 has an accurately determined mass, M = 1.54 ± 0.03 M
⊙ (1σ error) and distance, D = 1.07 ± 0.04 kpc. We analysed XMM-Newton data of this 2.95 ms pulsar to identify the nature of the X-ray emission. Results. We show that the X-ray emission from PSR J1909–3744 appears to be dominated by thermal emission from the polar cap. Only a single component model is required to fit the data. The black-body temperature of this emission is $ {kT}=0.26^{0.03}_{0.02} $ keV and we find a 0.2–10 keV un-absorbed flux of 1.1 × 10−14 erg cm−2 s−1 or an un-absorbed luminosity of 1.5 × 1030 erg s−1 . Conclusion. Thanks to the previously determined mass and distance constraints of the neutron star PSR J1909–3744, and its predominantly thermal emission, deep observations of this object with future X-ray facilities should provide useful constraints on the neutron star equation of state. [ABSTRACT FROM AUTHOR]- Published
- 2019
- Full Text
- View/download PDF
30. Modeling Pulsars in dense star clusters.
- Author
-
Ye, Claire S., Kremer, Kyle, Chatterjee, Sourav, Rodriguez, Carl L., and Rasio, Frederic A.
- Abstract
Over a hundred millisecond radio pulsars (MSPs) have been observed in globular clusters (GCs), motivating theoretical studies of the formation and evolution of these sources through stellar evolution coupled to stellar dynamics. Here we study MSPs in GCs using realistic N -body simulations with our Cluster Monte Carlo code. We show that neutron stars (NSs) formed in electron-capture supernovae can be spun up through mass transfer to form MSPs. Both NS formation and spin-up through accretion are greatly enhanced through dynamical interaction processes. We find that our models for average GCs at the present day with masses ≍ 2 × 10
5 M⊙ can produce up to 10 – 20 MSPs, while a very massive GC model with mass ≍ 106 M⊙ can produce close to 100. We show that the number of MSPs is anti-correlated with the total number of stellar-mass black holes (BHs) retained in the host cluster. As a result, the number of MSPs in a GC could be used to place constraints on its BH population. Some intrinsic properties of MSP systems in our models (such as the magnetic fields and spin periods) are in good overall agreement with observations. [ABSTRACT FROM AUTHOR]- Published
- 2019
- Full Text
- View/download PDF
31. Precise optical timing of PSR J1023+0038, the first millisecond pulsar detected with Aqueye+ in Asiago.
- Author
-
Zampieri, Luca, Burtovoi, Aleksandr, Fiori, Michele, Naletto, Giampiero, Spolon, Alessia, Barbieri, Cesare, Papitto, Alessandro, and Ambrosino, Filippo
- Subjects
PULSARS ,PHOTON detectors ,PULSAR detection ,NEUTRON stars ,X-ray binaries ,X-rays - Abstract
We report the first detection of an optical millisecond pulsar with the fast photon counter Aqueye+ in Asiago. This is an independent confirmation of the detection of millisecond pulsations from PSR J1023+0038 obtained with SiFAP at the Telescopio Nazionale Galileo. We observed the transitional millisecond pulsar PSR J1023+0038 with Aqueye+ mounted at the Copernicus telescope in 2018 January. Highly significant pulsations were detected. The rotational period is in agreement with the value extrapolated from the X-ray ephemeris, while the time of passage at the ascending node is shifted by 11.55 ± 0.08 s from the value predicted using the orbital period from the X-rays. An independent optical timing solution is derived over a baseline of a few days that has an accuracy of ∼0.007 in pulse phase (∼12 μs in time). This level of precision is needed to derive an accurate coherent timing solution for the pulsar and to search for possible phase shifts between the optical and X-ray pulses using future simultaneous X-ray and optical observations. [ABSTRACT FROM AUTHOR]
- Published
- 2019
- Full Text
- View/download PDF
32. Unification of strongly magnetized neutron stars with regard to X‐ray emission from hot spots.
- Author
-
Yoneyama, T., Hayashida, K., Nakajima, H., and Matsumoto, H.
- Subjects
NEUTRON stars ,MAGNETARS ,X-ray spectra ,MAGNETIC flux density ,SOFT X rays ,MAGNETIC fields - Abstract
Strongly magnetized isolated neutron stars (NSs) are categorized into two families according, mainly, to their magnetic field strength. The one with a higher magnetic field of 1014–1015 Gauss is called "magnetar," and the other is the X‐ray isolated neutron star (XINS) with 1013 Gauss. Both magnetars and XINSs show thermal emission in X‐rays, whose spectra are different. The soft X‐ray spectrum (below 10 keV) of a magnetar is reproduced with a two‐temperature blackbody (2BB), whereas that of an XINS shows only a single‐temperature blackbody (1BB), and its temperature is even lower than that of magnetars. On the basis of the magnetic field and temperature, it is often speculated that XINSs may be old and cooled magnetars. However, no other strong observational evidence has yet been reported to support the speculation. Here, we report that all the seven known XINSs show high‐temperature emission, which should have a similar origin to that of magnetars. Analyzing all the XMM‐Newton data of the XINSs with the highest statistics ever achieved, we find that their X‐ray spectra are all reproduced with a 2BB model, similar to magnetars, as opposed to the traditional 1BB model. Their emission radii and temperature ratios are also similar to those of magnetars except for two XINSs, which show significantly smaller radii than the others. The remarkable similarity in the X‐ray spectra between XINSs and magnetars suggests that the origins of their emitting regions are also the same. The lower temperature in XINSs can be explained if XINSs are older than magnetars. Therefore, this result is another observational indication that supports the standard hypothesis of classification of highly magnetized NSs. This article is based on our paper Yoneyama et al. (2019; accepted to PASJ). [ABSTRACT FROM AUTHOR]
- Published
- 2019
- Full Text
- View/download PDF
33. Impact of inter-correlated initial binary parameters on double black hole and neutron star mergers.
- Author
-
Klencki, J., Moe, M., Gladysz, W., Chruslinska, M., Holz, D. E., and Belczynski, K.
- Subjects
BINARY systems (Astronomy) ,BLACK holes ,NEUTRON stars ,PARAMETER estimation ,REDSHIFT - Abstract
The distributions of the initial main-sequence binary parameters are one of the key ingredients in obtaining evolutionary predictions for compact binary (BH–BH/BH–NS/NS–NS) merger rates. Until now, such calculations were done under the assumption that initial binary parameter distributions were independent. For the first time, we implement empirically derived inter-correlated distributions of initial binary parameters primary mass (M
1 ), mass ratio (q), orbital period (P), and eccentricity (e). Unexpectedly, the introduction of inter-correlated initial binary parameters leads to only a small decrease in the predicted merger rates by a factor of ≲2–3 relative to the previously used non-correlated initial distributions. The formation of compact object mergers in the isolated classical binary evolution favours initial binaries with stars of comparable masses (q ≈ 0.5–1) at intermediate orbital periods (log P (days) = 2–4). New distributions slightly shift the mass ratios towards lower values with respect to the previously used flat q distribution, which is the dominant effect decreasing the rates. New orbital periods (∼1.3 more initial systems within log P (days) = 2–4), together with new eccentricities (higher), only negligibly increase the number of progenitors of compact binary mergers. Additionally, we discuss the uncertainty of merger rate predictions associated with possible variations of the massive-star initial mass function (IMF). We argue that evolutionary calculations should be normalized to a star formation rate (SFR) that is obtained from the observed amount of UV light at wavelength 1500 Å (an SFR indicator). In this case, contrary to recent reports, the uncertainty of the IMF does not affect the rates by more than a factor of ∼2. Any change to the IMF slope for massive stars requires a change of SFR in a way that counteracts the impact of IMF variations on compact object merger rates. In contrast, we suggest that the uncertainty in cosmic SFR at low metallicity can be a significant factor at play. [ABSTRACT FROM AUTHOR]- Published
- 2018
- Full Text
- View/download PDF
34. Local merger rates of double neutron stars.
- Author
-
Chruslinska, Martyna
- Abstract
The first detection of gravitational waves from a merging double neutron star (DNS) binary implies a much higher rate of DNS coalescences in the local Universe than typically estimated on theoretical grounds. The recent study by Chruslinska et al. (2018) shows that apart from being particularly sensitive to the common envelope treatment, DNS merger rates appear rather robust against variations of several factors probed in their study (e.g. conservativeness of the mass transfer, angular momentum loss, and natal kicks), unless extreme assumptions are made. Confrontation with the improving observational limits may allow to rule out some of the extreme models. To correctly compare model predictions with observational limits one has to account for the other factors that affect the rates. One of those factors relates to the assumed history of star formation and chemical evolution of the Universe and its impact on the final results needs to be better constrained. [ABSTRACT FROM AUTHOR]
- Published
- 2018
- Full Text
- View/download PDF
35. A new X-ray look into four old pulsars.
- Author
-
Rigoselli, Michela and Mereghetti, Sandro
- Subjects
PULSARS ,HEAT radiation & absorption ,LUMINOSITY ,NEUTRON stars ,TEMPERATURE - Abstract
We report on the X-ray properties of four rotation-powered pulsars with characteristic ages in the range 0.3–5 Myr, derived from the analysis of XMM–Newton archival observations. We found convincing evidence of thermal emission only in the phase-averaged spectrum of PSR B0114+58, which is well fitted by a blackbody with temperature kT = 0.17 ± 0.02 keV and emitting radius R = 405
+110 −90 m, consistent with the size of its polar cap. The three other considered pulsars, PSR B0628−28, PSR B0919+06, and PSR B1133+16, have phase-averaged spectra that can be described well by single power laws with photon index Γ ~ 3. The 3σ upper limits on the bolometric luminosity of a possible thermal component with temperatures in the range ~0.05−2 keV are Lbol ≲ 3.2 × 1028 erg s−1 and Lbol ≲ 2.4 × 1029 erg s−1 , for PSR B0628−28 and PSR B0919+06, respectively. On the other hand, we found possible evidence that the pulsed emission of PSR B0628−28 is thermal. Two absorption lines at ~0.22 keV and ~0.44 keV are detected in the spectrum of PSR B1133+16. They are best interpreted as proton cyclotron features, implying the presence of multipolar components with a field of a few 1013 G at the neutron star polar caps. We discuss our results in the context of high-energy emission models of old rotation-powered pulsars. [ABSTRACT FROM AUTHOR]- Published
- 2018
- Full Text
- View/download PDF
36. What will eROSITA reveal among X-ray faint isolated neutron stars?
- Author
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Pires, Adriana M., Weltevrede, P., Perera, B.B.P., Preston, L.L., and Sanidas, S.
- Abstract
Since the discovery of the first radio pulsar fifty years ago, the population of neutron stars in our Galaxy has grown to over 2,600. A handful of these sources, exclusively seen in X-rays, show properties that are not observed in normal pulsars. Despite their scarcity, they are key to understanding aspects of the neutron star phenomenology and evolution. The forthcoming all-sky survey of eROSITA will unveil the X-ray faint end of the neutron star population at unprecedented sensitivity; therefore, it has the unique potential to constrain evolutionary models and advance our understanding of the sources that are especially silent in the radio and γ-ray regimes. In this contribution I discuss the expected role of eROSITA, and the challenges it will face, at probing the galactic neutron star population. [ABSTRACT FROM AUTHOR]
- Published
- 2017
- Full Text
- View/download PDF
37. Pulsar Glitches.
- Author
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Manchester, R. N., Weltevrede, P., Perera, B.B.P., Preston, L.L., and Sanidas, S.
- Abstract
The first known pulsar glitch was discovered in the Vela pulsar at both Parkes and Goldstone in March 1969. Since then the number of known glitches has grown enormously, with more than 520 glitches now known in more than 180 pulsars. Details of glitch parameters and post-glitch recoveries are described and some implications for the physics of neutron stars are discussed. [ABSTRACT FROM AUTHOR]
- Published
- 2017
- Full Text
- View/download PDF
38. Correlated emission and spin-down variability in radio pulsars.
- Author
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Shaw, Benjamin, Stappers, Benjamin W., Brook, Paul R., Karastergiou, Aris, Lyne, Andrew G., Weltevrede, P., Perera, B.B.P., Preston, L.L., and Sanidas, S.
- Abstract
The recent revelation that there are correlated period derivative and pulse shape changes in pulsars has dramatically changed our understanding of timing noise as well as the relationship between the radio emission and the properties of the magnetosphere as a whole. Using Gaussian processes we are able to model timing and emission variability using a regression technique that imposes no functional form on the data. We revisit the pulsars first studied by Lyne et al. (2010). We not only confirm the emission and rotational transitions revealed therein, but reveal further transitions and periodicities in 8 years of extended monitoring. We also show that in many of these objects the pulse profile transitions between two well-defined shapes, coincident with changes to the period derivative. With a view to the SKA and other telescopes capable of higher cadence we also study the detection limitations of period derivative changes. [ABSTRACT FROM AUTHOR]
- Published
- 2017
- Full Text
- View/download PDF
39. Braking indices and spin evolution: something is loose inside neutron stars.
- Author
-
Espinoza, Cristóbal M., Weltevrede, P., Perera, B.B.P., Preston, L.L., and Sanidas, S.
- Abstract
Braking indices are used to describe the evolution of pulsars rotation, and can offer insights into the braking mechanism that dominates the slow down. Here we discuss the main difficulties associated with measuring braking indices and the complexity of interpreting these measurements. Considering recent braking index measurements on pulsars with large and regular glitches, we comment on the significant effects that the loosely coupled superfluid inside pulsars might have on their spin evolution. [ABSTRACT FROM AUTHOR]
- Published
- 2017
- Full Text
- View/download PDF
40. The Radio and X-ray Mode-Switching Pulsar PSR B0943+10.
- Author
-
Mereghetti, Sandro and Rigoselli, Michela
- Subjects
PULSARS ,NEUTRON stars ,X-ray binaries ,STARS ,BINARY pulsars - Abstract
Observations obtained in the last years challenged the widespread notion that rotation-powered neutron stars are steady X-ray emitters. Besides a few allegedly rotation-powered neutron stars that showed 'magnetar-like' variability, a particularly interesting case is that of PSR B0943+10. Recent observations have shown that this pulsar, well studied in the radio band where it alternates between a bright and a quiescent mode, displays significant X-ray variations, anticorrelated in flux with the radio emission. The study of such synchronous radio/X-ray mode switching opens a new window to investigate the processes responsible for the pulsar radio and high-energy emission. Here we review the main X-ray properties of PSR B0943+10 derived from recent coordinated X-ray and radio observations. [ABSTRACT FROM AUTHOR]
- Published
- 2017
- Full Text
- View/download PDF
41. X-ray bounds on the r-mode amplitude in millisecond pulsars.
- Author
-
Schwenzer, Kai, Boztepe, Tuğba, Güver, Tolga, and Vurgun, Eda
- Subjects
PULSARS ,PULSATING stars ,RADIATION sources ,STARS ,COMPACT objects (Astronomy) - Abstract
r-mode asteroseismology provides a unique way to study the internal composition of compact stars. Due to their precise timing, recycled millisecond radio pulsars present a particularly promising class of sources. Although their thermal properties are still poorly constrained, X-ray data is very useful for asteroseismology since r-modes could strongly heat a star. Using known and new upper bounds on the temperatures and luminosities of several non-accreting millisecond radio pulsars, we derive bounds on the r-mode amplitude as low as α ≲10
-8 and discuss the impact on scenarios for their internal composition. [ABSTRACT FROM AUTHOR]- Published
- 2017
- Full Text
- View/download PDF
42. Consequences of a strong phase transition in the dense matter equation of state for the rotational evolution of neutron stars.
- Author
-
Bejger, M., Blaschke, D., Haensel, P., Zdunik, J. L., and Fortin, M.
- Subjects
NEUTRON stars ,EQUATIONS of state ,PHASE transitions ,STELLAR evolution ,STELLAR rotation - Abstract
Aims. We explore the implications of a strong first-order phase transition region in the dense matter equation of state in the interiors of rotating neutron stars, and the resulting creation of two disjoint families of neutron-star configurations (the so-called high-mass twins). Methods. We numerically obtained rotating, axisymmetric, and stationary stellar configurations in the framework of general relativity, and studied their global parameters and stability. Results. The instability induced by the equation of state divides stable neutron star configurations into two disjoint families: neutron stars (second family) and hybrid stars (third family), with an overlapping region in mass, the high-mass twin-star region. These two regions are divided by an instability strip. Its existence has interesting astrophysical consequences for rotating neutron stars. We note that it provides a natural explanation for the rotational frequency cutoff in the observed distribution of neutron star spins, and for the apparent lack of back-bending in pulsar timing. It also straightforwardly enables a substantial energy release in a mini-collapse to another neutron-star configuration (core quake), or to a black hole. [ABSTRACT FROM AUTHOR]
- Published
- 2017
- Full Text
- View/download PDF
43. Follow-up of isolated neutron star candidates from the eROSITA survey.
- Author
-
Pires, A. M., Schwope, A. D., and Motch, C.
- Subjects
NEUTRON stars ,MAGNETARS ,PULSAR detection ,OPEN clusters of stars ,MONTE Carlo method - Abstract
Peculiar groups of X-ray emitting isolated neutron stars, which include magnetars, the "magnificent seven", and central compact objects in supernova remnants, escape detection in standard pulsar surveys. Yet, they constitute a key element in understanding the neutron star evolution and phenomenology. Their use in population studies in the galactic scale has been hindered by the rarity of their detection. The all-sky survey of the extended Roentgen Survey with an Imaging Telescope Array (eROSITA) on-board the forthcoming Spectrum-Roentgen-Gamma (SRG) mission has the unique potential to unveil the X-ray faint part of the population and constrain evolutionary models. To create a forecast for the 4-year all-sky survey, we perform Monte Carlo simulations of a population synthesis model, where we follow the evolutionary tracks of thermally emitting neutron stars in the Milky Way and test their detectability. In this paper, we discuss strategies for pinpointing the most promising candidates for follow-up observing campaigns using current and future facilities. [ABSTRACT FROM AUTHOR]
- Published
- 2017
- Full Text
- View/download PDF
44. Ejector and propeller spin-down: how might a superluminous supernova millisecond magnetar become the 6.67 h pulsar in RCW 103.
- Author
-
Ho, Wynn C. G. and Andersson, Nils
- Subjects
EJECTOR pumps ,AXIAL flow pumps ,SUPERNOVAE ,MAGNETARS ,MAGNETIC fields ,NEUTRON stars - Abstract
The X-ray source 1E 161348-5055 in the supernova remnant RCW 103 recently exhibited X-ray activity typical of magnetars, i.e. neutron stars with magnetic fields ... 10
14 -1015 G. However, 1E 161348-5055 has an observed period of 6.67 h, in contrast to magnetars which have a spin period of seconds. Here we describe a simple model which can explain the spin evolution of 1E 161348-5055, as well as other magnetars, from an initial period of milliseconds that would be required for dynamo generation of magnetar-strength magnetic fields. We propose that the key difference between 1E 161348-5055 and other magnetars is the persistence of a remnant disc of small total mass. This disc caused 1E 161348-5055 to undergo ejector and propeller phases in its life, during which strong torques caused a rapid increase of its spin period. By matching its observed spin period and ≈1-3 kyr age, we find that 1E 161348-5055 has the (slightly) highest magnetic field of all known magnetars, with B ~ 5 x 1015 G, and that its disc had a mass of ~1024 g, comparable to that of the asteroid Ceres. [ABSTRACT FROM AUTHOR]- Published
- 2017
- Full Text
- View/download PDF
45. Interplanetary GPS using pulsar signals.
- Author
-
Becker, W., Bernhardt, M. G., and Jessner, A.
- Subjects
PULSARS ,NEUTRON stars ,NAVIGATION (Astronautics) ,GLOBAL Positioning System ,ASTRONAUTICS - Abstract
An external reference system suitable for deep space navigation can be defined by fast spinning and strongly magnetized neutron stars, called pulsars. Their beamed periodic signals have timing stabilities comparable to atomic clocks and provide characteristic temporal signatures that can be used as natural navigation beacons, quite similar to the use of GPS satellites for navigation on Earth. By comparing pulse arrival times measured on-board a spacecraft with predicted pulse arrivals at a reference location, the spacecraft position can be determined autonomously and with high accuracy everywhere in the solar system and beyond. The unique properties of pulsars make clear already today that such a navigation system will have its application in future astronautics. In this paper we describe the basic principle of spacecraft navigation using pulsars and report on the current development status of this novel technology. (© 2015 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim) [ABSTRACT FROM AUTHOR]
- Published
- 2015
- Full Text
- View/download PDF
46. Magnetic field growth in young glitching pulsars with a braking index.
- Author
-
Ho, Wynn C. G.
- Subjects
STELLAR magnetic fields ,PULSARS ,NEUTRON stars ,STELLAR rotation ,ACCRETION (Astrophysics) - Abstract
In the standard scenario for spin evolution of isolated neutron stars, a young pulsar slows down with a surface magnetic field B that does not change. Thus the pulsar follows a constant B trajectory in the phase space of spin period and spin period time derivative. Such an evolution predicts a braking index n = 3 while the field is constant and n > 3 when the field decays. This contrasts with all nine observed values being n < 3. Here we consider a magnetic field that is buried soon after birth and diffuses to the surface. We use a model of a growing surface magnetic field to fit observations of the three pulsars with lowest n: PSR J0537-6910 with n = -1.5, PSR B0833-45 (Vela) with n = 1.4, and PSR J1734-3333 with n = 0.9. By matching the age of each pulsar, we determine their magnetic field and spin period at birth and confirm the magnetar-strength field of PSR J1734-3333. Our results indicate that all three pulsars formed in a similar way to central compact objects (CCOs), with differences due to the amount of accreted mass. We suggest that magnetic field emergence may play a role in the distinctive glitch behaviour of low braking index pulsars, and we propose glitch behaviour and characteristic age as possible criteria in searches for CCO descendants. [ABSTRACT FROM AUTHOR]
- Published
- 2015
- Full Text
- View/download PDF
47. The binary nature of PSR J2032+4127.
- Author
-
Lyne, A. G., Stappers, B. W., Keith, M. J., Ray, P. S., Kerr, M., Camilo, F., and Johnson, T. J.
- Subjects
BINARY stars ,SOLAR radio emission ,PULSARS ,NEUTRON stars ,OPEN clusters of stars - Abstract
PSR J2032+4127 is a γ -ray and radio-emitting pulsar which has been regarded as a young luminous isolated neutron star. However, its recent spin-down rate has extraordinarily increased by a factor of 2. We present evidence that this is due to its motion as a member of a highlyeccentric binary system with an ~15-M
⊙ Be star,MT91 213. Timing observations show that, not only are the positions of the two stars coincident within 0.4 arcsec, but timing models of binary motion of the pulsar fit the data much better than a model of a young isolated pulsar. MT91 213, and hence the pulsar, lie in the Cyg OB2 stellar association, which is at a distance of only 1.4-1.7 kpc. The pulsar is currently on the near side of, and accelerating towards, the Be star, with an orbital period of 20-30 yr. The next periastron is well constrained to occur in early 2018, providing an opportunity to observe enhanced high-energy emission as seen in other Be-star binary systems. [ABSTRACT FROM AUTHOR]- Published
- 2015
- Full Text
- View/download PDF
48. Properties and observability of glitches and anti-glitches in accreting pulsars.
- Author
-
Ducci, L., Pizzochero, P. M., Doroshenko, V., Santangelo, A., Mereghetti, S., and Ferrigno, C.
- Subjects
STAR observations ,ACCRETION disks ,X-ray astronomy ,PULSAR detection ,NEUTRON stars ,X-ray binaries ,STARQUAKES - Abstract
Several glitches have been observed in young, isolated radio pulsars, while a clear detection in accretion-powered X-ray pulsars is still lacking. We use the Pizzochero snowplow model for pulsar glitches as well as starquake models to determine for the first time the expected properties of glitches in accreting pulsars and their observability. Since some accreting pulsars show accretion-induced long-term spin-up, we also investigate the possibility that anti-glitches occur in these stars. We find that glitches caused by quakes in a slow accreting neutron star are very rare and their detection extremely unlikely. On the contrary, glitches and anti-glitches caused by a transfer of angular momentum between the superfluid neutron vortices and the non-superfluid component may take place in accreting pulsars more often. We calculate the maximum jump in angular velocity of an anti-glitch and we find that it is expected to be ∆Ωa-gl ≈ 10
-5 -10-4 rad s-1 .We also note that since accreting pulsars usually have rotational angular velocities lower than those of isolated glitching pulsars, both glitches and anti-glitches are expected to have long rise and recovery timescales compared to isolated glitching pulsars, with glitches and anti-glitches appearing as a simple step in angular velocity. Among accreting pulsars, we find that GX 1+4 is the best candidate for the detection of glitches with currently operating X-ray instruments and future missions such as the proposed Large Observatory for X-ray Timing (LOFT). [ABSTRACT FROM AUTHOR]- Published
- 2015
- Full Text
- View/download PDF
49. THE BINARY COMPANION OF YOUNG, RELATIVISTIC PULSAR J1906+0746.
- Author
-
VAN LEEUWEN, J., KASIAN, L., STAIRS, I. H., LORIMER, D. R., CAMILO, F., CHATTERJEE, S., COGNARD, I., DESVIGNES, G., FREIRE, P. C. C., JANSSEN, G. H., KRAMER, M., LYNE, A. G., NICE, D. J., RANSOM, S. M., STAPPERS, B. W., and WEISBERG, J. M.
- Subjects
PULSARS ,PULSATING stars ,STELLAR atmospheres ,SOLAR atmosphere ,ASTROPHYSICS ,ASTRONOMY ,RADIO telescopes - Abstract
PSR J1906+0746 is a young pulsar in the relativistic binary with the second-shortest known orbital period, of 3.98 hr. We here present a timing study based on five years of observations, conducted with the five largest radio telescopes in the world, aimed at determining the companion nature. Through the measurement of three post-Keplerian orbital parameters, we find the pulsar mass to be 1.291(11) M
☉ , and the companion mass 1.322(11) M☉ , respectively. These masses fit well in the observed collection of double neutron stars (DNSs), but are also compatible with other systems where a young pulsar such as J1906+0746 is orbited by a white dwarf (WD). Neither radio pulsations nor dispersion-inducing outflows that could have further established the companion nature were detected. We derive an H I-absorption distance, which indicates that an optical confirmation of a WD companion is very challenging. The pulsar is fading fast due to geodetic precession, limiting future timing improvements. We conclude that the young pulsar J1906+0746 is likely part of a DNS, or is otherwise orbited by an older WD, in an exotic system formed through two stages of mass transfer. [ABSTRACT FROM AUTHOR]- Published
- 2015
- Full Text
- View/download PDF
50. Neutron Stars: Formed, Spun and Kicked.
- Author
-
Kalogera, V., Valsecchi, F., and Willems, B.
- Subjects
NEUTRON stars ,STAR formation ,STELLAR activity ,ELECTRON capture ,ACCRETION (Astrophysics) - Abstract
One of the primary goals when studying stellar systems with neutron stars has been to reveal the physical properties of progenitors and understand how neutron star spins and birth kicks are determined. Over the years a consensus understanding had been developed, but recently some of the basic elements of this understanding are being challenged by current observations of some binary systems and their theoretical interpretation. In what follows we review such recent developments and highlight how they are interconnected; we particularly emphasize some of the assumptions and caveats of theoretical interpretations and examine their validity (e.g., in connection to the unknown radial velocities of pulsars or the nuances of multi-dimensional statistical analyses). The emerging picture does not erase our earlier understanding; instead it broadens it as it reveals additional pathways for neutron star formation and evolution: neutron stars probably form at the end of both core collapse of Fe cores of massive stars and electron-capture supernovae of ONeMg cores of lower-mass stars; birth kicks are required to be high (well in excess of 100 km s
-1 ) for some neutron stars and low (<100 km s-1 ) for others depending on the formation process; and spin up may occur not just through Roche-lobe overflow but also through wind accretion or phases of hypercritical accretion during common envelope evolution. [ABSTRACT FROM AUTHOR]- Published
- 2008
- Full Text
- View/download PDF
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