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A model for nulling and mode changing in pulsars
High Energy Astrophysical Phenomena · Submitted 16 Dec 2009
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We propose that in some pulsars the magnetosphere has different states with different geometries or/and different distributions of currents, it occasionally switches between them.
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The abstract, sentence by sentence
We propose that in some pulsars the magnetosphere has different states with different geometries or/and different distributions of currents, it occasionally switches between them. These states have different spindown rates and emission beams, in some of the states no radioemission is produced at all. Switching into a different state manifests as a mode change when we see different parts of the emission beam or the beams in different states have significantly different geometries, it manifests as nulling when we either miss the new beam or no radioemission is generated in the new state. We show that modest variations in the beam shape can be accompanied by large variations in the pulsar spindown rate W - the dependence of W on the opening angle of the emission beam $\alpha$ can be as strong as W\propto\alpha^4. We speculate about physical mechanisms which may cause reconfiguration of the magnetosphere.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We propose that in some pulsars the magnetosphere has different states with different geometries or/and different distributions of currents, it occasionally switches between them. | contribution 0.97 | 0.33 | 0.50 | hedged possibility 0.62 |
| s1 | These states have different spindown rates and emission beams, in some of the states no radioemission is produced at all. | contribution 0.46 | 0.19 | 0.15 | asserted 0.99 |
| s2 | Switching into a different state manifests as a mode change when we see different parts of the emission beam or the beams in different states have significantly different geometries, it manifests as nulling when we either miss the new beam or no radioemission is generated in the new state. | interpretation 0.89 | 0.14 | 0.30 | asserted 0.98 |
| s3 | We show that modest variations in the beam shape can be accompanied by large variations in the pulsar spindown rate W - the dependence of W on the opening angle of the emission beam $\alpha$ can be as strong as W\propto\alpha^4. | result 1.00 | 0.90 | 0.25 | asserted 0.98 |
| s4 | We speculate about physical mechanisms which may cause reconfiguration of the magnetosphere. | interpretation 0.63 | 0.21 | 0.04 | speculative 1.00 |
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Original abstract
We propose that in some pulsars the magnetosphere has different states with different geometries or/and different distributions of currents, it occasionally switches between them. These states have different spindown rates and emission beams, in some of the states no radioemission is produced at all. Switching into a different state manifests as a mode change when we see different parts of the emission beam or the beams in different states have significantly different geometries, it manifests as nulling when we either miss the new beam or no radioemission is generated in the new state. We show that modest variations in the beam shape can be accompanied by large variations in the pulsar spindown rate W - the dependence of W on the opening angle of the emission beam $\alpha$ can be as strong as W\propto\alpha^4. We speculate about physical mechanisms which may cause reconfiguration of the magnetosphere.
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3 arXiv papers cite this in 5 sentences
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Cites it as background 1 paper
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Many models have been developed to explain the phenomena; some consider the plasma in the magnetosphere and how it is connected to the global charge distribution [ref] , others suggest variations in the particle acceleration region [ref] or a twisted magnetosphere [ref] .
Understanding the Neutron Star Population with the SKAO Telescopes · Rotating Radio Transients and Intermittent Pulsars · 0.94
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