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Dispersion measure: Confusion, Constants & Clarity
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abstract
The dispersion measure (DM) is one of the key attributes of radio pulsars and Fast Radio Bursts (FRBs). There is a mistaken view that the DM is an accurate measure of the column density of electrons between the observer and the source. To start with, the DM, unlike a true column density, is not a Lorentz invariant. Next, the DM also includes contribution from ions and is sensitive to the temperature of the plasma in the intervening clouds. Separately, the primary observable is the dispersion slope, $\mathcal{D}\equiv \Delta{(t)}/\Delta{(\nu^{-2}})$, where $t(\nu)$ is the arrival time at frequency, $\nu$. A scaling factor composed of physical and astronomical constants is needed to convert $\mathcal{D}$ to DM. In the early days of pulsar astronomy the relevant constants were defined to parts per million (ppm). As a result, a convention arose in which this conversion factor was fixed. Over time, several such conventions came about -- recipe for confusion. Meanwhile, over the past several years, the SI system has been restructured and the parsec is now exactly defined. As a result, the present accuracy of the conversion factor is below a part per billion -- many orders of magnitude better than the best measurement errors of $\mathcal{D}$. We are now in an awkward situation wherein the primary "observable", the DM, has incorrect scaling factor(s). To address these two concerns I propose that astronomers report the primary measurement, $\mathcal{D}$ (with a suggested normalization of $10^{15}\,$Hz), and not the DM. Interested users can convert $\mathcal{D}$ to DM without the need to know secret handshakes of the pulsar timing communities.
Forward citations
Cited by 3 Pith papers
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PSRDISP: A novel approach to modeling dispersive processes in single-pulsar noise analysis using epoch-wise dispersion measures
PSRDISP is a Gaussian-process framework that fits dispersion-measure and solar-wind noise directly to epoch-wise dispersion measures, recovering injected signals in simulated pulsar data.
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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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RRAT-like behaviour of PSR B0656+14 observed with I-LOFAR
PSR B0656+14 shows random, memory-less bright pulses at 110-190 MHz, requiring over 47,500 pulses to build a stable profile, resembling rotating radio transients.
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