Observational selection effects on radio pulsars are minimal for masses, but significant for orbits and spins
Abstract
The masses of Galactic pulsars in binaries measured through radio timing point to structure in the mass distribution with implications for dense matter and astrophysical formation processes: a bimodal shape with peaks at ∼ 1.3 M⊙ and ∼ 1.6 M⊙, with a cutoff above ∼2 M⊙. However, this observed population of radio pulsars is shaped not only by intrinsic pulsar properties, such as birth masses, binary evolutionary pathways and dense-matter constraints, but also by observational effects. In existing catalogs of pulsar mass measurements, observational selection effects influence (i) which systems are detected in the first place (detectability) and (ii) which systems yield well-measured masses (measurability). In this work, we revisit the radio pulsar population distribution in the context of observational effects associated with pulsar radio timing. Simulating systems of radio pulsars and timing observations, we track the process by which a given system ends up in an observational dataset and estimate the impact of the binary and pulsar parameters. We fold this selection function into hierarchical population inference and extract the intrinsic astrophysical distribution of pulsars observed with radio timing. We jointly infer the populations of pulsar mass, companion mass, orbital eccentricity, orbital period and pulsar spin period. Selection effects have minimal impact on the mass distributions, but more significantly affect other parameters. The ratio of circular-to-eccentric systems shifts from an observed 1 : 1 to an astrophysical, selection-corrected 2 : 1 ratio, while the true population is shifted toward longer orbital and spin periods than observed.
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BibTeX
@misc{drummond2026observational,
title = {{Observational selection effects on radio pulsars are minimal for masses, but significant for orbits and spins}},
author = {Lisa V. Drummond and Katerina Chatziioannou and Emmanuel Fonseca},
howpublished = {arXiv},
year = {2026},
month = sep,
doi = {10.48550/arxiv.2609.03157},
eprint = {2609.03157},
archivePrefix = {arXiv},
url = {https://arxiv.org/abs/2609.03157},
}
RIS
TY - UNPB
TI - Observational selection effects on radio pulsars are minimal for masses, but significant for orbits and spins
AU - Lisa V. Drummond
AU - Katerina Chatziioannou
AU - Emmanuel Fonseca
PY - 2026
DA - 2026/09/02
PB - arXiv
DO - 10.48550/arxiv.2609.03157
UR - https://arxiv.org/abs/2609.03157
AB - The masses of Galactic pulsars in binaries measured through radio timing point to structure in the mass distribution with implications for dense matter and astrophysical formation processes: a bimodal shape with peaks at ∼ 1.3 M_⊙ and ∼ 1.6 M_⊙, with a cutoff above ∼2 M_⊙. However, this observed population of radio pulsars is shaped not only by intrinsic pulsar properties, such as birth masses, binary evolutionary pathways and dense-matter constraints, but also by observational effects. In existing catalogs of pulsar mass measurements, observational selection effects influence (i) which systems are detected in the first place (detectability) and (ii) which systems yield well-measured masses (measurability). In this work, we revisit the radio pulsar population distribution in the context of observational effects associated with pulsar radio timing. Simulating systems of radio pulsars and timing observations, we track the process by which a given system ends up in an observational dataset and estimate the impact of the binary and pulsar parameters. We fold this selection function into hierarchical population inference and extract the intrinsic astrophysical distribution of pulsars observed with radio timing. We jointly infer the populations of pulsar mass, companion mass, orbital eccentricity, orbital period and pulsar spin period. Selection effects have minimal impact on the mass distributions, but more significantly affect other parameters. The ratio of circular-to-eccentric systems shifts from an observed 1 : 1 to an astrophysical, selection-corrected 2 : 1 ratio, while the true population is shifted toward longer orbital and spin periods than observed.
ER -