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  • EDP Sciences  (5)
  • Geyer, M.  (5)
  • 1
    In: Astronomy & Astrophysics, EDP Sciences, Vol. 657 ( 2022-01), p. A56-
    Abstract: MeerKAT’s large number (64) of 13.5 m diameter antennas, spanning 8 km with a densely packed 1 km core, create a powerful instrument for wide-area surveys, with high sensitivity over a wide range of angular scales. The MeerKAT Galaxy Cluster Legacy Survey (MGCLS) is a programme of long-track MeerKAT L -band (900−1670 MHz) observations of 115 galaxy clusters, observed for ∼6−10 h each in full polarisation. The first legacy product data release (DR1), made available with this paper, includes the MeerKAT visibilities, basic image cubes at ∼8″ resolution, and enhanced spectral and polarisation image cubes at ∼8″ and 15″ resolutions. Typical sensitivities for the full-resolution MGCLS image products range from ∼3−5 μJy beam −1 . The basic cubes are full-field and span 2° × 2°. The enhanced products consist of the inner 1.2° × 1.2° field of view, corrected for the primary beam. The survey is fully sensitive to structures up to ∼10′ scales, and the wide bandwidth allows spectral and Faraday rotation mapping. Relatively narrow frequency channels (209 kHz) are also used to provide H  I mapping in windows of 0  〈   z   〈  0.09 and 0.19  〈   z   〈  0.48. In this paper, we provide an overview of the survey and the DR1 products, including caveats for usage. We present some initial results from the survey, both for their intrinsic scientific value and to highlight the capabilities for further exploration with these data. These include a primary-beam-corrected compact source catalogue of ∼626 000 sources for the full survey and an optical and infrared cross-matched catalogue for compact sources in the primary-beam-corrected areas of Abell 209 and Abell S295. We examine dust unbiased star-formation rates as a function of cluster-centric radius in Abell 209, extending out to 3.5 R 200 . We find no dependence of the star-formation rate on distance from the cluster centre, and we observe a small excess of the radio-to-100 μm flux ratio towards the centre of Abell 209 that may reflect a ram pressure enhancement in the denser environment. We detect diffuse cluster radio emission in 62 of the surveyed systems and present a catalogue of the 99 diffuse cluster emission structures, of which 56 are new. These include mini-halos, halos, relics, and other diffuse structures for which no suitable characterisation currently exists. We highlight some of the radio galaxies that challenge current paradigms, such as trident-shaped structures, jets that remain well collimated far beyond their bending radius, and filamentary features linked to radio galaxies that likely illuminate magnetic flux tubes in the intracluster medium. We also present early results from the H  I analysis of four clusters, which show a wide variety of H  I mass distributions that reflect both sensitivity and intrinsic cluster effects, and the serendipitous discovery of a group in the foreground of Abell 3365.
    Type of Medium: Online Resource
    ISSN: 0004-6361 , 1432-0746
    RVK:
    RVK:
    Language: English
    Publisher: EDP Sciences
    Publication Date: 2022
    detail.hit.zdb_id: 1458466-9
    SSG: 16,12
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  • 2
    In: Astronomy & Astrophysics, EDP Sciences, Vol. 664 ( 2022-08), p. A27-
    Abstract: We report the discovery of 13 new pulsars in the globular cluster NGC 1851 by the TRAPUM Large Survey Project using the MeerKAT radio telescope. The discoveries consist of six isolated millisecond pulsars (MSPs) and seven binary pulsars, of which six are MSPs and one is mildly recycled. For all the pulsars, we present the basic kinematic, astrometric, and orbital parameters, where applicable, as well as their polarimetric properties, when these are measurable. Two of the binary MSPs (PSR J0514−4002D and PSR J0514−4002E) are in wide and extremely eccentric ( e   〉  0.7) orbits with a heavy white dwarf and a neutron star as their companion, respectively. With these discoveries, NGC 1851 is now tied with M28 as the cluster with the third largest number of known pulsars (14). Its pulsar population shows remarkable similarities with that of M28, Terzan 5, and other clusters with comparable structural parameters. The newly found pulsars are all located in the innermost regions of NGC 1851 and will likely enable, among other things, detailed studies of the cluster structure and dynamics.
    Type of Medium: Online Resource
    ISSN: 0004-6361 , 1432-0746
    RVK:
    RVK:
    Language: English
    Publisher: EDP Sciences
    Publication Date: 2022
    detail.hit.zdb_id: 1458466-9
    SSG: 16,12
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  • 3
    In: Astronomy & Astrophysics, EDP Sciences, Vol. 674 ( 2023-06), p. A169-
    Abstract: PSR J1933−6211 is a pulsar with a spin period of 3.5 ms in a 12.8 d nearly circular orbit with a white dwarf companion. Its high proper motion and low dispersion measure result in such significant interstellar scintillation that detections with a high signal-to-noise ratio have required long observing durations or fortuitous timing. In this work, we turn to the sensitive MeerKAT telescope, and combined with historic Parkes data, are able to leverage the kinematic and relativistic effects of PSR J1933−6211 to constrain its 3D orbital geometry and the component masses. We obtain a precise proper motion magnitude of 12.42 (3) mas yr −1 and a parallax of 1.0 (3) mas, and we also measure their effects as secular changes in the Keplerian parameters of the orbit: a variation in the orbital period of 7 (1)×10 −13 s s −1 and a change in the projected semi-major axis of 1.60 (5)×10 −14 s s −1 . A self-consistent analysis of all kinematic and relativistic effects yields a distance to the pulsar of $ 1.6^{+0.2}_{-0.3} $ kpc, an orbital inclination, i  = 55 (1) deg, and a longitude of the ascending node, $ \Omega = 255^{+8}_{-14} $ deg. The probability densities for Ω and i and their symmetric counterparts, 180 −  i and 360 − Ω, are seen to depend on the chosen fiducial orbit used to measure the time of passage of periastron ( T 0 ). We investigate this unexpected dependence and rule out software-related causes using simulations. Nevertheless, we constrain the masses of the pulsar and its companion to be $ 1.4^{+0.3}_{-0.2}\,M_\odot $ and 0.43 (5)  M ⊙ , respectively. These results strongly disfavour a helium-dominated composition for the white dwarf companion. The similarity in the spin, orbital parameters, and companion masses of PSRs J1933−6211 and J1614−2230 suggests that these systems underwent case A Roche-lobe overflow, an extended evolutionary process that occurs while the companion star is still on the main sequence. However, PSR J1933−6211 has not accreted significant matter: its mass is still at ∼1.4  M ⊙ . This highlights the low accretion efficiency of the spin-up process and suggests that observed neutron star masses are mostly a result of supernova physics, with minimum influence of subsequent binary evolution.
    Type of Medium: Online Resource
    ISSN: 0004-6361 , 1432-0746
    RVK:
    RVK:
    Language: English
    Publisher: EDP Sciences
    Publication Date: 2023
    detail.hit.zdb_id: 1458466-9
    SSG: 16,12
    Location Call Number Limitation Availability
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  • 4
    In: Astronomy & Astrophysics, EDP Sciences, Vol. 671 ( 2023-03), p. A72-
    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 Ṗ b  = −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.
    Type of Medium: Online Resource
    ISSN: 0004-6361 , 1432-0746
    RVK:
    RVK:
    Language: English
    Publisher: EDP Sciences
    Publication Date: 2023
    detail.hit.zdb_id: 1458466-9
    SSG: 16,12
    Location Call Number Limitation Availability
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  • 5
    In: Astronomy & Astrophysics, EDP Sciences, Vol. 665 ( 2022-09), p. A53-
    Abstract: Context. PSR J0955−6150 is a member of an enigmatic class of eccentric millisecond pulsar (MSP) and helium white dwarf (He WD) systems (eMSPs), whose binary evolution is poorly understood and believed to be strikingly different to that of traditional MSP+He WD systems in circular orbits. Aims. Measuring the masses of the stars in this system is important for testing the different hypotheses for the formation of eMSPs. Methods. We carried out timing observations of this pulsar with the Parkes radio telescope using the 20 cm multibeam and ultra-wide bandwidth low-frequency (UWL) receivers, and the L -band receiver of the MeerKAT radio telescope. The pulse profiles were flux and polarisation calibrated, and a rotating-vector model (RVM) was fitted to the position angle of the linear polarisation of the combined MeerKAT data. Pulse times of arrival (ToAs) were obtained from these using standard pulsar analysis techniques and analysed using the TEMPO 2 timing software. Results. Our observations reveal a strong frequency evolution of this MSP’s intensity, with a flux density spectral index ( α ) of −3.13(2). The improved sensitivity of MeerKAT resulted in a greater than tenfold improvement in the timing precision obtained compared to our older Parkes observations. This, combined with the eight-year timing baseline, has allowed precise measurements of a very small proper motion and three orbital post-Keplerian parameters, namely the rate of advance of periastron, ω̇  = 0.00152(1) deg yr −1 , and the orthometric Shapiro delay parameters, h 3  = 0.89(7) μs and ς = 0.88(2). Assuming general relativity, we obtain M p  = 1.71(2)  M ⊙ for the mass of the pulsar and M c  = 0.254(2)  M ⊙ for the mass of the companion; the orbital inclination is 83.2(4) degrees. Crucially, assuming that the position angle of the linear polarisation follows the RVM, we find that the spin axis has a misalignment relative to the orbital angular momentum of 〉 4.8deg at 99% confidence level. Conclusions. While the value of M p falls well within the wide range observed in eMSPs, M c is significantly smaller than expected from several formation hypotheses proposed, which are therefore unlikely to be correct and can be ruled out; M c is also significantly different from the expected value for an ideal low mass X-ray binary evolution scenario. If the misalignment between the spin axis of the pulsar and the orbital angular momentum is to be believed, it suggests that the unknown process that created the orbital eccentricity of the binary was also capable of changing its orbital orientation, an important evidence for understanding the origin of eMSPs.
    Type of Medium: Online Resource
    ISSN: 0004-6361 , 1432-0746
    RVK:
    RVK:
    Language: English
    Publisher: EDP Sciences
    Publication Date: 2022
    detail.hit.zdb_id: 1458466-9
    SSG: 16,12
    Location Call Number Limitation Availability
    BibTip Others were also interested in ...
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