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Evolution of neutron stars in wide eccentric low-mass binary systems
High Energy Astrophysical Phenomena · Submitted 27 Jan 2025
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We show that the transition from the ejector to the propeller stage occurs earlier in more eccentric systems, thus increasing the time that neutron stars can spend accreting matter.
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The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
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The abstract, sentence by sentence
Precise astrometric measurement with Gaia satellite resulted in the discovery of tens of wide binary systems consisting of a Sun-like star and an invisible component. The latter can be a white dwarf, a neutron star, or a black hole. In this paper, we model magneto-rotational evolution of neutron stars in wide low-mass binaries accounting for the orbital eccentricity. We aim to calculate when neutron stars in such systems can start to accrete matter from the stellar wind of the companion. We show that the transition from the ejector to the propeller stage occurs earlier in more eccentric systems, thus increasing the time that neutron stars can spend accreting matter. Our calculations show that in the case of efficient spin-down at the propeller stage, a neutron star in an eccentric orbit with $e\gtrsim0.6$ and a standard magnetic field $B=10^{12}$ G can start accreting within a few Gyr. For neutron stars with $B=10^{13}$ G the onset of accretion occurs earlier regardless of the orbital eccentricity. Otherwise, with a lower spin-down rate, such a neutron star will remain at the propeller stage for most of its life.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Precise astrometric measurement with Gaia satellite resulted in the discovery of tens of wide binary systems consisting of a Sun-like star and an invisible component. | background 1.00 | 0.08 | 0.02 | asserted 1.00 |
| s1 | The latter can be a white dwarf, a neutron star, or a black hole. | background 1.00 | 0.05 | 0.02 | hedged possibility 0.82 |
| s2 | In this paper, we model magneto-rotational evolution of neutron stars in wide low-mass binaries accounting for the orbital eccentricity. | contribution 0.57 | 0.85 | 0.04 | asserted 0.79 |
| s3 | We aim to calculate when neutron stars in such systems can start to accrete matter from the stellar wind of the companion. | contribution 0.89 | 0.31 | 0.04 | unclear 0.55 |
| s4 | We show that the transition from the ejector to the propeller stage occurs earlier in more eccentric systems, thus increasing the time that neutron stars can spend accreting matter. | result 0.98 | 0.91 | 0.66 | asserted 1.00 |
| s5 | Our calculations show that in the case of efficient spin-down at the propeller stage, a neutron star in an eccentric orbit with $e\gtrsim0.6$ and a standard magnetic field $B=10^{12}$ G can start accreting within a few Gyr. | result 1.00 | 0.94 | 0.31 | asserted 0.94 |
| s6 | For neutron stars with $B=10^{13}$ G the onset of accretion occurs earlier regardless of the orbital eccentricity. | result 1.00 | 0.86 | 0.11 | asserted 1.00 |
| s7 | Otherwise, with a lower spin-down rate, such a neutron star will remain at the propeller stage for most of its life. | result 0.92 | 0.73 | 0.07 | asserted 0.83 |
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The paper
Original abstract
Precise astrometric measurement with Gaia satellite resulted in the discovery of tens of wide binary systems consisting of a Sun-like star and an invisible component. The latter can be a white dwarf, a neutron star, or a black hole. In this paper, we model magneto-rotational evolution of neutron stars in wide low-mass binaries accounting for the orbital eccentricity. We aim to calculate when neutron stars in such systems can start to accrete matter from the stellar wind of the companion. We show that the transition from the ejector to the propeller stage occurs earlier in more eccentric systems, thus increasing the time that neutron stars can spend accreting matter. Our calculations show that in the case of efficient spin-down at the propeller stage, a neutron star in an eccentric orbit with $e\gtrsim0.6$ and a standard magnetic field $B=10^{12}$ G can start accreting within a few Gyr. For neutron stars with $B=10^{13}$ G the onset of accretion occurs earlier regardless of the orbital eccentricity. Otherwise, with a lower spin-down rate, such a neutron star will remain at the propeller stage for most of its life.
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How the literature uses it
1 arXiv paper cite this in 1 sentence
What it cites · 27 sentences without a confident label
Builds on 2 papers
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In the second paper [ref] we modeled the NS evolution in a wide binary with a solar-like companion in a circular orbit.
Probing the propeller regime with wide neutron star binaries · Introduction · 0.84
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In the first paper [ref] , we applied various propeller models to analyse magneto-rotational evolution of NSs in symbiotic X-ray binaries.
Probing the Propeller Regime with Symbiotic X-ray Binaries · Introduction · 0.88
Uses the method or tool of 3 papers
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To describe the spin evolution of an NS we follow the general approach presented e.g., by [ref] .
Spin evolution of neutron stars · Main parameters · 0.92
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In our model, it is derived from the solution of the Bondi-Hoyle-Lyttleton (BHL) problem (see [ref] for a review).
A Review of Bondi--Hoyle--Lyttleton Accretion · Main parameters · 0.83
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We follow [ref] in defining this parameter: [equation]
Centrifugal barriers in magnetospheric accretion · Magneto-rotational evolution of a neutron star · 0.92
Uses data or values from 6 papers
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The NS can both spin up and spin down, so the angular momentum consists of two terms [equation] The spin-down torque is [equation] where coefficient $k_t=0.4$ [ref] .
Probing the Propeller Regime with Symbiotic X-ray Binaries · Magneto-rotational evolution of a neutron star · 0.83
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According to [ref] , this is a typical value for the slow component of the wind at distances $r≳0.2$ AU from the star (we consider $r<0.2$ AU hereafter).
Stellar Winds on the Main-Sequence I: Wind Model · The model of a binary system · 0.96
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Based on observations, [ref] have estimated how the mass-loss rate scales with mass, radius, and the rotational frequency $Ω_*$ of the Sun-like star
Stellar Winds on the Main-Sequence II: the Evolution of Rotation and Winds · Influence of variations in stellar parameters · 0.83
Compares with 2 papers
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Contrary to the case of NSs with $B_0=10^12$ G in circular orbits considered by [ref] , the NSs with the same field but in eccentric orbits can switch to the propeller stage within the lifetime of their companions.
Probing the propeller regime with wide neutron star binaries · Summary and conclusions · 0.86
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This is similar to the case of the evolution of isolated NSs; see, e.g., [ref] .
Early Accretion Onset in Long-Period Isolated Pulsars · Model of the magneto-rotational evolution · 0.81
Cites as background 4 papers
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Generally, the field decays on several different timescales [ref] .
Evolution of neutron star magnetic fields · Magneto-rotational evolution of a neutron star · 0.97
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In these systems an NS is accreting from the wind of a red giant companion [ref] .
On its way to the neutron star-white dwarf binary graveyard, IGR J16194-2810, a first ascent M giant X-ray binary · Introduction · 0.87
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In these systems an NS is accreting from the wind of a red giant companion [ref] .
Wind-accreting Symbiotic X-ray Binaries · Introduction · 0.87
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