Radio pulsars scintillate because their emission travels through the ionized interstellar medium along multiple paths, which interfere with each other. It has long been realized that, independent of their nature, the regions responsible for the scintillation could be used as ‘interstellar lenses’ to localize pulsar emission regions1,2. Most such lenses, however, resolve emission components only marginally, limiting results to statistical inferences and detections of small positional shifts3,4,5. As lenses situated close to their source offer better resolution, it should be easier to resolve emission regions of pulsars located in high-density environments such as supernova remnants6 or binaries in which the pulsar’s companion has an ionized outflow. Here we report observations of extreme plasma lensing in the ‘black widow’ pulsar, B1957+20, near the phase in its 9.2-hour orbit at which its emission is eclipsed by its companion’s outflow7,8,9. During the lensing events, the observed radio flux is enhanced by factors of up to 70–80 at specific frequencies. The strongest events clearly resolve the emission regions: they affect the narrow main pulse and parts of the wider interpulse differently. We show that the events arise naturally from density fluctuations in the outer regions of the outflow, and we infer a resolution of our lenses that is comparable to the pulsar’s radius, about 10 kilometres. Furthermore, the distinct frequency structures imparted by the lensing are reminiscent of what is observed for the repeating fast radio burst FRB 121102, providing observational support for the idea that this source is observed through, and thus at times strongly magnified by, plasma lenses10.
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We thank A. Bilous for sharing and discussing her results which motivated this analysis. We thank the rest of our scintillometry group for discussions and support throughout. R.M., M.H.v.K., U.-L.P. and K.V. are funded through NSERC. I-S.Y was supported by a SOSCIP Consortium Postdoctoral Fellowship.Reviewer information
Nature thanks S. Ransom and J. Hessels for their contribution to the peer review of this work.
Extended data figures and tables
The brown dwarf companion is irradiated by the pulsar wind, causing it to be hotter on the side facing the pulsar26, and inflated, nearly filling its Roche lobe27. Outflowing material is shocked by the pulsar wind, leaving a cometary-like tail of material. This tail is asymmetric because of the companion’s orbital motion, which leads to eclipse egress lasting substantially longer than ingress. The companion and separations are drawn roughly to scale, whereas the pulsar is not: the light cylinder radius of 76 km would be indistinguishable on this figure. The inclination of the system is conservatively constrained to (ref. 13). vp and vc are the velocities of the pulsar and companion, a is the semi-major axis of the orbit, and Rroche is the Roche lobe of the companion.
Shown is the excess dispersion measure relative to the interstellar dispersion, with insets focusing on regions of strong lensing. The excess dispersion is estimated from delays in pulse arrival times (see Methods); at our observing frequency of 330 MHz, ΔDM = 0.001 pc cm−3 corresponds to a delay of 38 μs. The scatter around the curves is intrinsic. During periods of strong lensing, it is at a level of 2.6 × 10−5 pc cm−3, corresponding to variations in delay time of 1 μs.
a–e, Each row shows pulse profiles for 10-s segments (left, in 128 phase bins), and the corresponding magnification distributions. The segments are taken from: a, a quiescent region, showing a log-normal magnification distribution (repeated using a dotted line in b–e for comparison); b, eclipse ingress, showing some lensing events, reflected in the tail to high magnification; although hard to see, the average flux is reduced to about 70% by absorption in eclipsing material); c, the first post-eclipse lensing period, showing extreme magnifications but little change in average flux; d, in between the two post-eclipse strong lensing periods, showing only weak lensing on relatively long, approximately 100-ms timescales; e, the second post-eclipse period of strong lensing.
An almost edge-on (left) and a face-on (right) view of the lensing geometry. We assume that the source is at a separation from the pulsar equal to the semi-major axis a of the binary system and moves on a trajectory parallel to the lens plane. A source at the focal point (X, Y) will illuminate the entire elliptical lens coherently, leading to strong magnification. In general, the focal point may not be at the centre of the ellipse (although it is likely to be within it), and the source trajectory [xs(t), ys(t)] may not intersect the focal point or the elliptical region.