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DM-power: an algorithm for high precision dispersion measure with application to fast radio bursts
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abstract
We present DM-power, a new method for precisely determining the dispersion measure (DM) of radio bursts, and apply it to the Fast Radio Burst (FRB) source FRB~20180916B. Motivated by the complex structure on multiple time scales seen in FRBs, DM-power optimizes the DM by combining measurements at multiple Fourier frequencies in the power spectrum of the burst. By optimally weighting the measurements at each Fourier frequency, DM-power finds a burst DM that effectively incorporates information on many different burst timescales. We validate this technique on simulated Gaussian pulse profiles with a precision down to $\sigma_{\rm DM} \sim 0.001~{\rm pc~cm}^{-3}$, and then apply it to bursts from pulsar B0329+54 and FRB~20180916B. The precision of these DM measurements are sufficient to measure a statistically significant variation in DM over a $\approx 2$ hr span. While this variation could be the result of electron density variations along the line of sight, it is more like that the observed variation is the result of intrinsic frequency-dependent burst structure that can mimic a dispersive delay.
Forward citations
Cited by 3 Pith papers
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Decadal evolution of a repeating fast radio burst source
Long-term monitoring of repeating FRB 20121102A reveals a significant decline in local dispersion measure and a 70% drop in rotation measure, indicating an evolving magnetized environment likely from a young supernova...
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Cross-validation of six dispersion measure estimation methods for FRB 20240114A
Cross-validation of six DM methods on 2874 FRB 20240114A bursts shows morphology-driven scatter and residual second-to-minute apparent DM fluctuations that cannot be real line-of-sight plasma changes.
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The magnetar model's energy crisis for a prolific repeating fast radio burst source
FRB 20240114A's estimated energy output over 214 days exceeds 86% of a typical magnetar's dipole magnetic energy, the strongest such constraint yet, if typical beaming and efficiency are assumed.
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