Polarization Properties of Energetic Pulsars at Meterwavelengths

Polarization behavior shows a transition in the pulsar population, where energetic sources with higher spin-down energy loss, $\dot{E}\gt 1{0}^{34}$ erg s ^−1 , often have fractional linear polarization ( L / I ) close to 100%, while below this range L / I is usually lower than 50%. The polarization...

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Main Authors: Dipanjan Mitra, Rahul Basu, George I. Melikidze
Format: Article
Language:English
Published: IOP Publishing 2025-01-01
Series:The Astrophysical Journal
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Online Access:https://doi.org/10.3847/1538-4357/addab1
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author Dipanjan Mitra
Rahul Basu
George I. Melikidze
author_facet Dipanjan Mitra
Rahul Basu
George I. Melikidze
author_sort Dipanjan Mitra
collection DOAJ
description Polarization behavior shows a transition in the pulsar population, where energetic sources with higher spin-down energy loss, $\dot{E}\gt 1{0}^{34}$ erg s ^−1 , often have fractional linear polarization ( L / I ) close to 100%, while below this range L / I is usually lower than 50%. The polarization behavior has been primarily studied at higher frequencies above 1 GHz, and in this work, we explore the single-pulse polarization behavior in pulsars with $\dot{E}\gt 5\,\times 1{0}^{33}$ erg s ^−1 at a lower frequency range of 300–750 MHz. The polarization behavior can be divided into two categories, the first with L / I  > 70% where the polarization position angle (PPA) follows a single track, and a second group with L / I  <  70% and scattered PPA behavior with or without orthogonal modes. However, there are some single pulses in the first category that also have lower L / I and exhibit the presence of two polarization modes along orthogonal tracks. The radio emission in pulsars arises due to coherent curvature radiation (CCR) from charge bunches, which develops due to nonlinear instabilities in the pulsar plasma forming charge separated envelope solitons. The CCR excites orthogonally polarized X and O modes oriented perpendicular and parallel to the magnetic field line planes, which detach in the plasma and propagate independently. The O mode is 7 times stronger than the X mode but gets damped in the medium. We show that incoherent mixing of the X and O modes with different levels of damping can reproduce the observed polarization features in the energetic pulsar population.
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spelling doaj-art-fa847d8ee8064e6c9358b72f15cf7e3f2025-08-20T02:38:27ZengIOP PublishingThe Astrophysical Journal1538-43572025-01-01987211910.3847/1538-4357/addab1Polarization Properties of Energetic Pulsars at MeterwavelengthsDipanjan Mitra0https://orcid.org/0000-0002-9142-9835Rahul Basu1https://orcid.org/0000-0003-1824-4487George I. Melikidze2https://orcid.org/0000-0003-1879-1659National Centre for Radio Astrophysics, Tata Institute of Fundamental Research , Pune 411007, India; Janusz Gil Institute of Astronomy, University of Zielona Góra , ul. Szafrana 2, 65-516 Zielona Góra, PolandJanusz Gil Institute of Astronomy, University of Zielona Góra , ul. Szafrana 2, 65-516 Zielona Góra, PolandJanusz Gil Institute of Astronomy, University of Zielona Góra , ul. Szafrana 2, 65-516 Zielona Góra, Poland; Evgeni Kharadze Georgian National Astrophysical Observatory , 0301 Abastumani, GeorgiaPolarization behavior shows a transition in the pulsar population, where energetic sources with higher spin-down energy loss, $\dot{E}\gt 1{0}^{34}$ erg s ^−1 , often have fractional linear polarization ( L / I ) close to 100%, while below this range L / I is usually lower than 50%. The polarization behavior has been primarily studied at higher frequencies above 1 GHz, and in this work, we explore the single-pulse polarization behavior in pulsars with $\dot{E}\gt 5\,\times 1{0}^{33}$ erg s ^−1 at a lower frequency range of 300–750 MHz. The polarization behavior can be divided into two categories, the first with L / I  > 70% where the polarization position angle (PPA) follows a single track, and a second group with L / I  <  70% and scattered PPA behavior with or without orthogonal modes. However, there are some single pulses in the first category that also have lower L / I and exhibit the presence of two polarization modes along orthogonal tracks. The radio emission in pulsars arises due to coherent curvature radiation (CCR) from charge bunches, which develops due to nonlinear instabilities in the pulsar plasma forming charge separated envelope solitons. The CCR excites orthogonally polarized X and O modes oriented perpendicular and parallel to the magnetic field line planes, which detach in the plasma and propagate independently. The O mode is 7 times stronger than the X mode but gets damped in the medium. We show that incoherent mixing of the X and O modes with different levels of damping can reproduce the observed polarization features in the energetic pulsar population.https://doi.org/10.3847/1538-4357/addab1Radio pulsars
spellingShingle Dipanjan Mitra
Rahul Basu
George I. Melikidze
Polarization Properties of Energetic Pulsars at Meterwavelengths
The Astrophysical Journal
Radio pulsars
title Polarization Properties of Energetic Pulsars at Meterwavelengths
title_full Polarization Properties of Energetic Pulsars at Meterwavelengths
title_fullStr Polarization Properties of Energetic Pulsars at Meterwavelengths
title_full_unstemmed Polarization Properties of Energetic Pulsars at Meterwavelengths
title_short Polarization Properties of Energetic Pulsars at Meterwavelengths
title_sort polarization properties of energetic pulsars at meterwavelengths
topic Radio pulsars
url https://doi.org/10.3847/1538-4357/addab1
work_keys_str_mv AT dipanjanmitra polarizationpropertiesofenergeticpulsarsatmeterwavelengths
AT rahulbasu polarizationpropertiesofenergeticpulsarsatmeterwavelengths
AT georgeimelikidze polarizationpropertiesofenergeticpulsarsatmeterwavelengths