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Long‐term spectral and timing properties of the soft gamma‐ray repeater SGR 1833−0832 and detection of extended X‐ray emission around the radio pulsar PSR B1830−08

Identifieur interne : 000C63 ( Istex/Corpus ); précédent : 000C62; suivant : 000C64

Long‐term spectral and timing properties of the soft gamma‐ray repeater SGR 1833−0832 and detection of extended X‐ray emission around the radio pulsar PSR B1830−08

Auteurs : P. Esposito ; G. L. Israel ; R. Turolla ; F. Mattana ; A. Tiengo ; A. Possenti ; S. Zane ; N. Rea ; M. Burgay ; D. Götz ; S. Mereghetti ; L. Stella ; M. H. Wieringa ; J. M. Sarkissian ; T. Enoto ; P. Romano ; T. Sakamoto ; Y. E. Nakagawa ; K. Makishima ; Nakazawa ; H. Nishioka ; C. François-Martin

Source :

RBID : ISTEX:43BA55885B793AD60EC9C7DD943FDE0DBD67425B

English descriptors

Abstract

SGR 1833−0832 was discovered on 2010 March 19, thanks to the Swift detection of a short hard X‐ray burst and follow‐up X‐ray observations. Since then, it was repeatedly observed with Swift, Rossi X‐ray Timing Explorer and XMM–Newton. Using these data, which span about 225 d, we studied the long‐term spectral and timing characteristics of SGR 1833−0832. We found evidence for diffuse emission surrounding SGR 1833−0832, which is most likely a halo produced by the scattering of the point‐source X‐ray radiation by dust along the line of sight, and we show that the source X‐ray spectrum is well described by an absorbed blackbody, with temperature kT∼ 1.2 keV and absorbing column NH= (10.4 ± 0.2) × 1022 cm−2, while different or more complex models are disfavoured. The source persistent X‐ray emission remained fairly constant at ∼3.7 × 10−12 erg cm−2 s−1 for the first ∼20 d after the onset of the bursting episode, then it faded by a factor of ∼40 in the subsequent ∼140 d, following a power‐law trend with index α≃−0.5. We obtained a phase‐coherent timing solution with the longest baseline (∼225 d) to date for this source which, besides period P= 7.565 4084(4) s and period derivative  s s−1, includes higher order period derivatives. We also report on our search of the counterpart to the soft gamma‐ray repeater (SGR) at radio frequencies using the Australia Telescope Compact Array and the Parkes Radio Telescope. No evidence for radio emission was found, down to flux densities of 0.9 mJy (at 1.5 GHz) and 0.09 mJy (at 1.4 GHz) for the continuum and pulsed emissions, respectively, consistently with other observations at different epochs. Finally, the analysis of the field of PSR B1830−08 (J1833−0827), which was serendipitously imaged by the XMM–Newton observations, led to the discovery of the X‐ray pulsar wind nebula generated by this 85‐ms radio pulsar. We discuss its possible association with the unidentified TeV source HESS J1834−087.

Url:
DOI: 10.1111/j.1365-2966.2011.19022.x

Links to Exploration step

ISTEX:43BA55885B793AD60EC9C7DD943FDE0DBD67425B

Le document en format XML

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<name sortKey="Gotz, D" sort="Gotz, D" uniqKey="Gotz D" first="D." last="Götz">D. Götz</name>
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<name sortKey="Mereghetti, S" sort="Mereghetti, S" uniqKey="Mereghetti S" first="S." last="Mereghetti">S. Mereghetti</name>
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<name sortKey="Stella, L" sort="Stella, L" uniqKey="Stella L" first="L." last="Stella">L. Stella</name>
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<mods:affiliation>Department of Physics, University of Tokyo, 7‐3‐1 Hongo, Bunkyo‐ku, Tokyo 113‐0033, Japan</mods:affiliation>
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<name sortKey="Nakazawa, " sort="Nakazawa, " uniqKey="Nakazawa " first="" last="Nakazawa"> Nakazawa</name>
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<name sortKey="Nishioka, H" sort="Nishioka, H" uniqKey="Nishioka H" first="H." last="Nishioka">H. Nishioka</name>
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<name sortKey="Francois Artin, C" sort="Francois Artin, C" uniqKey="Francois Artin C" first="C." last="François-Martin">C. François-Martin</name>
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<title level="a" type="main">Long‐term spectral and timing properties of the soft gamma‐ray repeater SGR 1833−0832 and detection of extended X‐ray emission around the radio pulsar PSR B1830−08</title>
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<mods:affiliation>Mullard Space Science Laboratory, University College London, Holmbury St Mary, Dorking, Surrey RH5 6NT</mods:affiliation>
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<name sortKey="Mattana, F" sort="Mattana, F" uniqKey="Mattana F" first="F." last="Mattana">F. Mattana</name>
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</affiliation>
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<name sortKey="Possenti, A" sort="Possenti, A" uniqKey="Possenti A" first="A." last="Possenti">A. Possenti</name>
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<name sortKey="Rea, N" sort="Rea, N" uniqKey="Rea N" first="N." last="Rea">N. Rea</name>
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<name sortKey="Burgay, M" sort="Burgay, M" uniqKey="Burgay M" first="M." last="Burgay">M. Burgay</name>
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<name sortKey="Gotz, D" sort="Gotz, D" uniqKey="Gotz D" first="D." last="Götz">D. Götz</name>
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<mods:affiliation>AIM (UMR 7158 CEA/DSM‐CNRS‐Université Paris Diderot) Irfu/Service d’Astrophysique, Saclay, F‐91191 Gif‐sur‐Yvette Cedex, France</mods:affiliation>
</affiliation>
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<name sortKey="Mereghetti, S" sort="Mereghetti, S" uniqKey="Mereghetti S" first="S." last="Mereghetti">S. Mereghetti</name>
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<mods:affiliation>INAF – Istituto di Astrofisica Spaziale e Fisica Cosmica – Milano, via E. Bassini 15, I‐20133 Milano, Italy</mods:affiliation>
</affiliation>
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<name sortKey="Stella, L" sort="Stella, L" uniqKey="Stella L" first="L." last="Stella">L. Stella</name>
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<mods:affiliation>INAF – Osservatorio Astronomico di Roma, via Frascati 33, I‐00040 Monteporzio Catone, Italy</mods:affiliation>
</affiliation>
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<name sortKey="Wieringa, M H" sort="Wieringa, M H" uniqKey="Wieringa M" first="M. H." last="Wieringa">M. H. Wieringa</name>
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<name sortKey="Sarkissian, J M" sort="Sarkissian, J M" uniqKey="Sarkissian J" first="J. M." last="Sarkissian">J. M. Sarkissian</name>
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<name sortKey="Enoto, T" sort="Enoto, T" uniqKey="Enoto T" first="T." last="Enoto">T. Enoto</name>
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<mods:affiliation>Kavli Institute for Particle Astrophysics & Cosmology (KIPAC), SLAC/Stanford University, PO Box 20450, MS 29, Stanford, CA 94309, USA</mods:affiliation>
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<name sortKey="Romano, P" sort="Romano, P" uniqKey="Romano P" first="P." last="Romano">P. Romano</name>
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<name sortKey="Sakamoto, T" sort="Sakamoto, T" uniqKey="Sakamoto T" first="T." last="Sakamoto">T. Sakamoto</name>
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<name sortKey="Nakagawa, Y E" sort="Nakagawa, Y E" uniqKey="Nakagawa Y" first="Y. E." last="Nakagawa">Y. E. Nakagawa</name>
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<mods:affiliation>High Energy Astrophysics Laboratory, Institute of Physical and Chemical Research (RIKEN), Wako, Saitama 351‐0198, Japan</mods:affiliation>
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<name sortKey="Makishima, K" sort="Makishima, K" uniqKey="Makishima K" first="K." last="Makishima">K. Makishima</name>
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<mods:affiliation>High Energy Astrophysics Laboratory, Institute of Physical and Chemical Research (RIKEN), Wako, Saitama 351‐0198, Japan</mods:affiliation>
</affiliation>
<affiliation>
<mods:affiliation>Department of Physics, University of Tokyo, 7‐3‐1 Hongo, Bunkyo‐ku, Tokyo 113‐0033, Japan</mods:affiliation>
</affiliation>
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<name sortKey="Nakazawa, " sort="Nakazawa, " uniqKey="Nakazawa " first="" last="Nakazawa"> Nakazawa</name>
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<mods:affiliation>Department of Physics, University of Tokyo, 7‐3‐1 Hongo, Bunkyo‐ku, Tokyo 113‐0033, Japan</mods:affiliation>
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<name sortKey="Nishioka, H" sort="Nishioka, H" uniqKey="Nishioka H" first="H." last="Nishioka">H. Nishioka</name>
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<mods:affiliation>Department of Physics, University of Tokyo, 7‐3‐1 Hongo, Bunkyo‐ku, Tokyo 113‐0033, Japan</mods:affiliation>
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<mods:affiliation>Université Denis Diderot – Paris 7, 4 place Jussieu, F‐75252 Paris Cedex 5, France</mods:affiliation>
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<term>Ancillary response</term>
<term>Arbitrary distance</term>
<term>Astron</term>
<term>Australia telescope</term>
<term>Background counts</term>
<term>Background maps</term>
<term>Better statistics</term>
<term>Black squares</term>
<term>Blackbody</term>
<term>Blackbody model</term>
<term>Blackbody spectrum</term>
<term>Blackbody temperature</term>
<term>Blue stars</term>
<term>Bottom panel</term>
<term>Burgay</term>
<term>Cambridge univ</term>
<term>Centre</term>
<term>Column density</term>
<term>Compact emission</term>
<term>Compact structure</term>
<term>Data sets</term>
<term>Diffuse emission</term>
<term>Effective area</term>
<term>Energy band</term>
<term>Energy range</term>
<term>Epic instrument</term>
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<term>Event lists</term>
<term>Exponential function</term>
<term>Gaensler</term>
<term>Galactic plane</term>
<term>Halo</term>
<term>Halo spectra</term>
<term>Hess</term>
<term>Higher ratio</term>
<term>Hobbs</term>
<term>Hydrogen column density</term>
<term>Inaf istituto</term>
<term>Kargaltsev pavlov</term>
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<term>Large absorption</term>
<term>Large window mode</term>
<term>Light curves</term>
<term>Magnetars</term>
<term>Magnetospheric twist</term>
<term>Mereghetti</term>
<term>Minimum ratio</term>
<term>Mnras</term>
<term>Monthly notices</term>
<term>More details</term>
<term>Mosaicked image</term>
<term>Neutron star</term>
<term>Outburst</term>
<term>Paris cedex</term>
<term>Paris diderot</term>
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<term>Persistent emission</term>
<term>Phase residuals</term>
<term>Phase shifts</term>
<term>Photon</term>
<term>Photon index</term>
<term>Point source</term>
<term>Possible association</term>
<term>Proper motion direction</term>
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<term>Radio magnetars</term>
<term>Radio observations</term>
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<term>Radio pulsars</term>
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<term>Rossi timing explorer</term>
<term>Rotational energy loss</term>
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<term>Rxte data</term>
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<div type="abstract" xml:lang="en">SGR 1833−0832 was discovered on 2010 March 19, thanks to the Swift detection of a short hard X‐ray burst and follow‐up X‐ray observations. Since then, it was repeatedly observed with Swift, Rossi X‐ray Timing Explorer and XMM–Newton. Using these data, which span about 225 d, we studied the long‐term spectral and timing characteristics of SGR 1833−0832. We found evidence for diffuse emission surrounding SGR 1833−0832, which is most likely a halo produced by the scattering of the point‐source X‐ray radiation by dust along the line of sight, and we show that the source X‐ray spectrum is well described by an absorbed blackbody, with temperature kT∼ 1.2 keV and absorbing column NH= (10.4 ± 0.2) × 1022 cm−2, while different or more complex models are disfavoured. The source persistent X‐ray emission remained fairly constant at ∼3.7 × 10−12 erg cm−2 s−1 for the first ∼20 d after the onset of the bursting episode, then it faded by a factor of ∼40 in the subsequent ∼140 d, following a power‐law trend with index α≃−0.5. We obtained a phase‐coherent timing solution with the longest baseline (∼225 d) to date for this source which, besides period P= 7.565 4084(4) s and period derivative  s s−1, includes higher order period derivatives. We also report on our search of the counterpart to the soft gamma‐ray repeater (SGR) at radio frequencies using the Australia Telescope Compact Array and the Parkes Radio Telescope. No evidence for radio emission was found, down to flux densities of 0.9 mJy (at 1.5 GHz) and 0.09 mJy (at 1.4 GHz) for the continuum and pulsed emissions, respectively, consistently with other observations at different epochs. Finally, the analysis of the field of PSR B1830−08 (J1833−0827), which was serendipitously imaged by the XMM–Newton observations, led to the discovery of the X‐ray pulsar wind nebula generated by this 85‐ms radio pulsar. We discuss its possible association with the unidentified TeV source HESS J1834−087.</div>
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<p>SGR 1833−0832 was discovered on 2010 March 19, thanks to the
<hi rend="italic">Swift</hi>
detection of a short hard X‐ray burst and follow‐up X‐ray observations. Since then, it was repeatedly observed with
<hi rend="italic">Swift</hi>
,
<hi rend="italic">Rossi X‐ray Timing Explorer</hi>
and
<hi rend="italic">XMM–Newton</hi>
. Using these data, which span about 225 d, we studied the long‐term spectral and timing characteristics of SGR 1833−0832. We found evidence for diffuse emission surrounding SGR 1833−0832, which is most likely a halo produced by the scattering of the point‐source X‐ray radiation by dust along the line of sight, and we show that the source X‐ray spectrum is well described by an absorbed blackbody, with temperature
<hi rend="italic">kT</hi>
∼ 1.2 keV and absorbing column
<hi rend="italic">N</hi>
<hi rend="subscript">H</hi>
= (10.4 ± 0.2) × 10
<hi rend="superscript">22</hi>
 cm
<hi rend="superscript">−2</hi>
, while different or more complex models are disfavoured. The source persistent X‐ray emission remained fairly constant at ∼3.7 × 10
<hi rend="superscript">−12</hi>
erg cm
<hi rend="superscript">−2</hi>
 s
<hi rend="superscript">−1</hi>
for the first ∼20 d after the onset of the bursting episode, then it faded by a factor of ∼40 in the subsequent ∼140 d, following a power‐law trend with index α≃−0.5. We obtained a phase‐coherent timing solution with the longest baseline (∼225 d) to date for this source which, besides period
<hi rend="italic">P</hi>
= 7.565 4084(4) s and period derivative
<graphic url="equation/MNR_19022_mu1.gif" rend="inline image"></graphic>
 s s
<hi rend="superscript">−1</hi>
, includes higher order period derivatives. We also report on our search of the counterpart to the soft gamma‐ray repeater (SGR) at radio frequencies using the Australia Telescope Compact Array and the Parkes Radio Telescope. No evidence for radio emission was found, down to flux densities of 0.9 mJy (at 1.5 GHz) and 0.09 mJy (at 1.4 GHz) for the continuum and pulsed emissions, respectively, consistently with other observations at different epochs. Finally, the analysis of the field of PSR B1830−08 (J1833−0827), which was serendipitously imaged by the
<hi rend="italic">XMM–Newton</hi>
observations, led to the discovery of the X‐ray pulsar wind nebula generated by this 85‐ms radio pulsar. We discuss its possible association with the unidentified TeV source HESS J1834−087.</p>
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<term xml:id="k3">X‐rays: individual: PSR B1830−08 (J1833−0827)</term>
<term xml:id="k4">X‐rays: individual: SGR 1833−0832</term>
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<unparsedEditorialHistory>Accepted 2011 May 6. Received 2011 May 4; in original form 2011 April 12</unparsedEditorialHistory>
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<keyword xml:id="k4">X‐rays: individual: SGR 1833−0832</keyword>
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<title type="main">ABSTRACT</title>
<p>SGR 1833−0832 was discovered on 2010 March 19, thanks to the
<i>Swift</i>
detection of a short hard X‐ray burst and follow‐up X‐ray observations. Since then, it was repeatedly observed with
<i>Swift</i>
,
<i>Rossi X‐ray Timing Explorer</i>
and
<i>XMM–Newton</i>
. Using these data, which span about 225 d, we studied the long‐term spectral and timing characteristics of SGR 1833−0832. We found evidence for diffuse emission surrounding SGR 1833−0832, which is most likely a halo produced by the scattering of the point‐source X‐ray radiation by dust along the line of sight, and we show that the source X‐ray spectrum is well described by an absorbed blackbody, with temperature
<i>kT</i>
∼ 1.2 keV and absorbing column
<i>N</i>
<sub>H</sub>
= (10.4 ± 0.2) × 10
<sup>22</sup>
 cm
<sup>−2</sup>
, while different or more complex models are disfavoured. The source persistent X‐ray emission remained fairly constant at ∼3.7 × 10
<sup>−12</sup>
erg cm
<sup>−2</sup>
 s
<sup>−1</sup>
for the first ∼20 d after the onset of the bursting episode, then it faded by a factor of ∼40 in the subsequent ∼140 d, following a power‐law trend with index α≃−0.5. We obtained a phase‐coherent timing solution with the longest baseline (∼225 d) to date for this source which, besides period
<i>P</i>
= 7.565 4084(4) s and period derivative
<inlineGraphic alt="inline image" location="equation/MNR_19022_mu1.gif" href=""></inlineGraphic>
 s s
<sup>−1</sup>
, includes higher order period derivatives. We also report on our search of the counterpart to the soft gamma‐ray repeater (SGR) at radio frequencies using the Australia Telescope Compact Array and the Parkes Radio Telescope. No evidence for radio emission was found, down to flux densities of 0.9 mJy (at 1.5 GHz) and 0.09 mJy (at 1.4 GHz) for the continuum and pulsed emissions, respectively, consistently with other observations at different epochs. Finally, the analysis of the field of PSR B1830−08 (J1833−0827), which was serendipitously imaged by the
<i>XMM–Newton</i>
observations, led to the discovery of the X‐ray pulsar wind nebula generated by this 85‐ms radio pulsar. We discuss its possible association with the unidentified TeV source HESS J1834−087.</p>
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<affiliation>Mullard Space Science Laboratory, University College London, Holmbury St Mary, Dorking, Surrey RH5 6NT</affiliation>
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<namePart type="family">Romano</namePart>
<affiliation>INAF – Istituto di Astrofisica Spaziale e Fisica Cosmica – Palermo, via U. La Malfa 153, I‐90146 Palermo, Italy</affiliation>
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<roleTerm type="text">author</roleTerm>
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<affiliation>NASA Goddard Space Flight Center, Greenbelt, MD 20771, USA</affiliation>
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<affiliation>High Energy Astrophysics Laboratory, Institute of Physical and Chemical Research (RIKEN), Wako, Saitama 351‐0198, Japan</affiliation>
<affiliation>Department of Physics, University of Tokyo, 7‐3‐1 Hongo, Bunkyo‐ku, Tokyo 113‐0033, Japan</affiliation>
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<abstract lang="en">SGR 1833−0832 was discovered on 2010 March 19, thanks to the Swift detection of a short hard X‐ray burst and follow‐up X‐ray observations. Since then, it was repeatedly observed with Swift, Rossi X‐ray Timing Explorer and XMM–Newton. Using these data, which span about 225 d, we studied the long‐term spectral and timing characteristics of SGR 1833−0832. We found evidence for diffuse emission surrounding SGR 1833−0832, which is most likely a halo produced by the scattering of the point‐source X‐ray radiation by dust along the line of sight, and we show that the source X‐ray spectrum is well described by an absorbed blackbody, with temperature kT∼ 1.2 keV and absorbing column NH= (10.4 ± 0.2) × 1022 cm−2, while different or more complex models are disfavoured. The source persistent X‐ray emission remained fairly constant at ∼3.7 × 10−12 erg cm−2 s−1 for the first ∼20 d after the onset of the bursting episode, then it faded by a factor of ∼40 in the subsequent ∼140 d, following a power‐law trend with index α≃−0.5. We obtained a phase‐coherent timing solution with the longest baseline (∼225 d) to date for this source which, besides period P= 7.565 4084(4) s and period derivative  s s−1, includes higher order period derivatives. We also report on our search of the counterpart to the soft gamma‐ray repeater (SGR) at radio frequencies using the Australia Telescope Compact Array and the Parkes Radio Telescope. No evidence for radio emission was found, down to flux densities of 0.9 mJy (at 1.5 GHz) and 0.09 mJy (at 1.4 GHz) for the continuum and pulsed emissions, respectively, consistently with other observations at different epochs. Finally, the analysis of the field of PSR B1830−08 (J1833−0827), which was serendipitously imaged by the XMM–Newton observations, led to the discovery of the X‐ray pulsar wind nebula generated by this 85‐ms radio pulsar. We discuss its possible association with the unidentified TeV source HESS J1834−087.</abstract>
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