Deep NuSTAR and Swift Monitoring Observations of the Magnetar 1E 1841-045

We report on a 350-ks NuSTAR observation of the magnetar 1E 1841-045 taken in 2013 September. During the observation, NuSTAR detected six bursts of short duration, with \(T_{90}

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Hauptverfasser: An, Hongjun, Archibald, Robert F, Hascoet, Romain, Kaspi, Victoria M, Beloborodov, Andrei M, Archibald, Anne M, Beardmore, Andy, Boggs, Steven E, Christensen, Finn E, Craig, William W, Gehrels, Niel, Hailey, Charles J, Harrison, Fiona A, Kennea, Jamie, Kouveliotou, Chryssa, Stern, Daniel, Younes, George, Zhang, William W
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container_title arXiv.org
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creator An, Hongjun
Archibald, Robert F
Hascoet, Romain
Kaspi, Victoria M
Beloborodov, Andrei M
Archibald, Anne M
Beardmore, Andy
Boggs, Steven E
Christensen, Finn E
Craig, William W
Gehrels, Niel
Hailey, Charles J
Harrison, Fiona A
Kennea, Jamie
Kouveliotou, Chryssa
Stern, Daniel
Younes, George
Zhang, William W
description We report on a 350-ks NuSTAR observation of the magnetar 1E 1841-045 taken in 2013 September. During the observation, NuSTAR detected six bursts of short duration, with \(T_{90}
doi_str_mv 10.48550/arxiv.1505.03570
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During the observation, NuSTAR detected six bursts of short duration, with \(T_{90}&lt;1\) s. An elevated level of emission tail is detected after the brightest burst, persisting for \(\sim\)1 ks. The emission showed a power-law decay with a temporal index of 0.5 before returning to the persistent emission level. The long observation also provided detailed phase-resolved spectra of the persistent X-ray emission of the source. By comparing the persistent spectrum with that previously reported, we find that the source hard-band emission has been stable over approximately 10 years. The persistent hard X-ray emission is well fitted by a coronal outflow model, where \(e^{+/-}\) pairs in the magnetosphere upscatter thermal X-rays. Our fit of phase-resolved spectra allowed us to estimate the angle between the rotational and magnetic dipole axes of the magnetar, \(\alpha_{mag}=0.25\), the twisted magnetic flux, \(2.5\times10^{26}\rm \ G\ cm^2\), and the power released in the twisted magnetosphere, \(L_j=6\times10^{36}\rm \ erg\ s^{-1}\). Assuming this model for the hard X-ray spectrum, the soft X-ray component is well fit by a two-blackbody model, with the hotter blackbody consistent with the footprint of the twisted magnetic field lines on the star. We also report on the 3-year Swift monitoring observations obtained since 2011 July. The soft X-ray spectrum remained stable during this period, and the timing behavior was noisy, with large timing residuals.</description><identifier>EISSN: 2331-8422</identifier><identifier>DOI: 10.48550/arxiv.1505.03570</identifier><language>eng</language><publisher>Ithaca: Cornell University Library, arXiv.org</publisher><subject>Axes of rotation ; Blackbody ; Emission spectra ; Magnetars ; Magnetic dipoles ; Magnetic flux ; Magnetism ; Magnetospheres ; Monitoring ; Outflow ; Physics - High Energy Astrophysical Phenomena ; Rotational spectra ; Soft x rays ; X-rays</subject><ispartof>arXiv.org, 2015-05</ispartof><rights>2015. This work is published under http://arxiv.org/licenses/nonexclusive-distrib/1.0/ (the “License”). 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Our fit of phase-resolved spectra allowed us to estimate the angle between the rotational and magnetic dipole axes of the magnetar, \(\alpha_{mag}=0.25\), the twisted magnetic flux, \(2.5\times10^{26}\rm \ G\ cm^2\), and the power released in the twisted magnetosphere, \(L_j=6\times10^{36}\rm \ erg\ s^{-1}\). Assuming this model for the hard X-ray spectrum, the soft X-ray component is well fit by a two-blackbody model, with the hotter blackbody consistent with the footprint of the twisted magnetic field lines on the star. We also report on the 3-year Swift monitoring observations obtained since 2011 July. 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During the observation, NuSTAR detected six bursts of short duration, with \(T_{90}&lt;1\) s. An elevated level of emission tail is detected after the brightest burst, persisting for \(\sim\)1 ks. The emission showed a power-law decay with a temporal index of 0.5 before returning to the persistent emission level. The long observation also provided detailed phase-resolved spectra of the persistent X-ray emission of the source. By comparing the persistent spectrum with that previously reported, we find that the source hard-band emission has been stable over approximately 10 years. The persistent hard X-ray emission is well fitted by a coronal outflow model, where \(e^{+/-}\) pairs in the magnetosphere upscatter thermal X-rays. Our fit of phase-resolved spectra allowed us to estimate the angle between the rotational and magnetic dipole axes of the magnetar, \(\alpha_{mag}=0.25\), the twisted magnetic flux, \(2.5\times10^{26}\rm \ G\ cm^2\), and the power released in the twisted magnetosphere, \(L_j=6\times10^{36}\rm \ erg\ s^{-1}\). Assuming this model for the hard X-ray spectrum, the soft X-ray component is well fit by a two-blackbody model, with the hotter blackbody consistent with the footprint of the twisted magnetic field lines on the star. We also report on the 3-year Swift monitoring observations obtained since 2011 July. The soft X-ray spectrum remained stable during this period, and the timing behavior was noisy, with large timing residuals.</abstract><cop>Ithaca</cop><pub>Cornell University Library, arXiv.org</pub><doi>10.48550/arxiv.1505.03570</doi><oa>free_for_read</oa></addata></record>
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subjects Axes of rotation
Blackbody
Emission spectra
Magnetars
Magnetic dipoles
Magnetic flux
Magnetism
Magnetospheres
Monitoring
Outflow
Physics - High Energy Astrophysical Phenomena
Rotational spectra
Soft x rays
X-rays
title Deep NuSTAR and Swift Monitoring Observations of the Magnetar 1E 1841-045
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