Abstract:Interstellar scintillation (ISS), observed as time variation in the intensity of a compact radio source, is caused by small-scale structure in the electron density of the interstellar plasma. Dynamic spectra of ISS show modulation in radio frequency and time. Here we relate the (two-dimensional) power spectrum of the dynamic spectrum-the secondary spectrum-to the scattered image of the source. Recent work has identified remarkable parabolic arcs in secondary spectra. Each point in a secondary spectrum correspo… Show more
“…Appendix C develops a rudimentary analytical theory of arcs that is valid in the two asymptotic regimes U T1 and U 3 1. The discussion there complements the more detailed physical approach taken by Cordes et al (2006). The behavior of arcs in the transition regime U $ few, and in the presence of anisotropic turbulence, deserves further analytical and numerical study, but it is beyond the scope of this work.…”
Section: Comparison With Numerical Resultsmentioning
confidence: 83%
“…Secondary spectra often show a concentration of power along parabolic ridges f ¼ AEaf 2 t (Stinebring et al 2001). Cordes et al (2006) have given a theoretical explanation of this phenomenon, according to which the coefficient a ¼ zk 2 /(cv 2 ? ), where z is the effective distance of the screen of equation (1).…”
Section: Appendix C Parabolic Arcs In Secondary Spectramentioning
confidence: 99%
“…Presumably, also, arcs should be more prominent when scattering is dominated by a thin ''screen'' rather than distributed along the line of sight, since integration over z would further soften the final square root in equation (C5). These points are made by Cordes et al (2006).…”
Section: Appendix C Parabolic Arcs In Secondary Spectramentioning
We present a fitting function to describe the statistics of flux modulations caused by interstellar scintillation. The function models a very general quantity: the cross-correlation of the flux observed from a compact radio source of finite angular size observed at two frequencies and at two positions or times. The formula will be useful for fitting data from sources such as intraday variables and gamma-ray burst afterglows. These sources are often observed at relatively high frequencies (several gigahertz), where interstellar scattering is neither very strong nor very weak, so that asymptotic formulae are inapplicable.
“…Appendix C develops a rudimentary analytical theory of arcs that is valid in the two asymptotic regimes U T1 and U 3 1. The discussion there complements the more detailed physical approach taken by Cordes et al (2006). The behavior of arcs in the transition regime U $ few, and in the presence of anisotropic turbulence, deserves further analytical and numerical study, but it is beyond the scope of this work.…”
Section: Comparison With Numerical Resultsmentioning
confidence: 83%
“…Secondary spectra often show a concentration of power along parabolic ridges f ¼ AEaf 2 t (Stinebring et al 2001). Cordes et al (2006) have given a theoretical explanation of this phenomenon, according to which the coefficient a ¼ zk 2 /(cv 2 ? ), where z is the effective distance of the screen of equation (1).…”
Section: Appendix C Parabolic Arcs In Secondary Spectramentioning
confidence: 99%
“…Presumably, also, arcs should be more prominent when scattering is dominated by a thin ''screen'' rather than distributed along the line of sight, since integration over z would further soften the final square root in equation (C5). These points are made by Cordes et al (2006).…”
Section: Appendix C Parabolic Arcs In Secondary Spectramentioning
We present a fitting function to describe the statistics of flux modulations caused by interstellar scintillation. The function models a very general quantity: the cross-correlation of the flux observed from a compact radio source of finite angular size observed at two frequencies and at two positions or times. The formula will be useful for fitting data from sources such as intraday variables and gamma-ray burst afterglows. These sources are often observed at relatively high frequencies (several gigahertz), where interstellar scattering is neither very strong nor very weak, so that asymptotic formulae are inapplicable.
“…We use a model of scintillation arcs developed in Stinebring et al (2001), Hill et al (2003), Cordes et al (2004), and Walker et al (2004) and summarized here. The essential features of the model are that the dominant scattering occurs in a thin screen along the line of sight and there is detectable scattering through angles large compared to the half-width of the pulsar image.…”
We have detected a strong deflection of radio waves from the pulsar PSR B0834ϩ06 in scintillation observations. Interference between the undeflected pulsar image and deflected subimages allows single-dish interferometry of the interstellar medium with submilliarcsecond resolution. We infer the presence of scattering structure(s) similar to those that are thought to cause extreme scattering events in quasar flux monitoring programs: size ∼0.2 AU (an angular size of 0.1 mas) with an electron overdensity of տ10 3 compared to the warm ionized medium. The deflectors are nearly stationary in a scattering screen that is thin (Շ5% of the pulsar-observer distance in extent), is located 70% of the way from the Earth to the pulsar, and has been seen consistently in observations dating back 20 years. The pulsar scans the scattering screen at a velocity of 110 km s Ϫ1 with a detection radius of 15 mas. Pulsar observations such as these-particularly with a new generation of low-frequency radio telescopes with large collecting areas-hold promise for improving constraints on the poorly understood physical characteristics and space density of the deflecting structures. Such observations may also prove useful in correcting deviations that the deflectors produce in high-precision timing of millisecond pulsars.
“…Parabolic arcs have been observed in this system, and they provide a different view of the ISS. This method is not fully independent of the timescale analysis but it has a different dependence on anisotropy, which is the critical feature of our analysis (Cordes et al 2004). …”
Section: Anisotropy Analysis For J0737à3039mentioning
We have examined the interstellar scintillations of the pulsars in the double-pulsar binary system. Near the time of the eclipse of pulsar A by the magnetosphere of B, the scintillations from both pulsars should be highly correlated because the radiation is passing through the same interstellar plasma. We report confirmation of this effect using 820 and 1400 MHz observations made with the Green Bank Telescope. The correlation allows us to constrain the projected relative position of the two pulsars at closest approach to be 4000 AE 2000 km, corresponding to an inclination that is only 0N29 AE 0N14 away from 90 . It also produces a two-dimensional map of the spatial correlation of the interstellar scintillation. This shows that the interstellar medium in the direction of the pulsars is significantly anisotropic. When this anisotropy is included in the orbital fitting, the transverse velocity of the center of mass is reduced from the previously published value of 141 AE 8:5 km s À1 to 66 AE 15 km s À1 .
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