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A late jet rebrightening revealed from multiwavelength monitoring of the black hole candidate XTE J1752-223

Identifieur interne : 004831 ( PascalFrancis/Curation ); précédent : 004830; suivant : 004832

A late jet rebrightening revealed from multiwavelength monitoring of the black hole candidate XTE J1752-223

Auteurs : D. M. Russell [Pays-Bas] ; P. A. Curran [France] ; T. Munoz-Darias [Italie] ; F. Lewis [Royaume-Uni] ; S. Motta [Italie] ; H. Stiele [Italie] ; T. Belloni [Italie] ; J. C. A. Miller-Jones [Australie] ; P. G. Jonker [Pays-Bas, États-Unis] ; K. O'Brien [États-Unis] ; J. Homan [États-Unis] ; P. Casella [Royaume-Uni] ; P. Gandhi [Japon] ; P. Soleri [Pays-Bas] ; S. Markoff [Pays-Bas] ; D. Maitra [États-Unis] ; E. Gallo [États-Unis] ; M. Cadolle Bel [Espagne]

Source :

RBID : Pascal:12-0042281

Descripteurs français

English descriptors

Abstract

We present optical monitoring of the black hole candidate XTE J1752-223 during its 2009-10 outburst and decay to quiescence. The optical light curve can be described by an exponential decay followed by a plateau, then a more rapid fade towards quiescence. The plateau appears to be due to an extra component of optical emission that brightens and then fades over ∼40 days. We show evidence for the origin of this optical 'flare' to be the synchrotron jet during the decaying hard state, and we identify and isolate both disc and jet components in the spectral energy distributions. The optical flare has the same morphology and amplitude as a contemporaneous X-ray rebrightening. This suggests a common origin, but no firm conclusions can be made favouring or disfavouring the jet producing the X-ray flare. The quiescent optical magnitudes are B ≥ 20.6, V ≥ 21.1, R ≥ 19.5, i' ≥ 19.2. From the optical outburst amplitude we estimate a likely orbital period of <22 h. We also present near-infrared (NIR) photometry and polarimetry and rare mid-IR imaging (8-12 μm) when the source is nearing quiescence. The fading jet component, and possibly the companion star, may contribute to the NIR flux. We derive deep mid-IR flux upper limits and NIR linear polarization upper limits. With the inclusion of radio data, we measure an almost flat jet spectral index between radio and optical; Fν ν∼+0.05. The data favour the jet break to optically thin emission to reside in the IR, but may shift to frequencies as high as the optical or UV during the peak of the flare.
pA  
A01 01  1    @0 0035-8711
A02 01      @0 MNRAA4
A03   1    @0 Mon. Not. R. Astron. Soc.
A05       @2 419
A06       @2 2
A08 01  1  ENG  @1 A late jet rebrightening revealed from multiwavelength monitoring of the black hole candidate XTE J1752-223
A11 01  1    @1 RUSSELL (D. M.)
A11 02  1    @1 CURRAN (P. A.)
A11 03  1    @1 MUNOZ-DARIAS (T.)
A11 04  1    @1 LEWIS (F.)
A11 05  1    @1 MOTTA (S.)
A11 06  1    @1 STIELE (H.)
A11 07  1    @1 BELLONI (T.)
A11 08  1    @1 MILLER-JONES (J. C. A.)
A11 09  1    @1 JONKER (P. G.)
A11 10  1    @1 O'BRIEN (K.)
A11 11  1    @1 HOMAN (J.)
A11 12  1    @1 CASELLA (P.)
A11 13  1    @1 GANDHI (P.)
A11 14  1    @1 SOLERI (P.)
A11 15  1    @1 MARKOFF (S.)
A11 16  1    @1 MAITRA (D.)
A11 17  1    @1 GALLO (E.)
A11 18  1    @1 CADOLLE BEL (M.)
A14 01      @1 Astronomical Institute 'Anton Pannekoek', University of Amsterdam, PO Box 94249 @2 1090 GE Amsterdam @3 NLD @Z 1 aut. @Z 15 aut.
A14 02      @1 Laboratoire AIM, CEA/IRFU-Université Paris Diderot-CNRS/INSU, CEA DSM/IRFU/SAp, Centre de Saclay @2 91191 Gif-sur-Yvette @3 FRA @Z 2 aut.
A14 03      @1 INAF-Osservatorio Astronomico di Brera, Via E. Bianchi 46 @2 23807 Merate (LC @3 ITA @Z 3 aut. @Z 5 aut. @Z 6 aut. @Z 7 aut.
A14 04      @1 Faulkes Telescope Project, University of Glamorgan @2 Pontypridd CF37 1DL @3 GBR @Z 4 aut.
A14 05      @1 Department of Physics and Astronomy, The Open Universiy, Walton Hall @2 Milton Keynes MK7 6AA @3 GBR @Z 4 aut.
A14 06      @1 International Centre for Radio Astronomy Research, Curtin University, GPO Box U1987 @2 Perth, WA 6845 @3 AUS @Z 8 aut.
A14 07      @1 SRON, Netherlands Institute for Space Research, Sorbonnelaan 2 @2 3584 CA, Utrecht @3 NLD @Z 9 aut.
A14 08      @1 Harvard-Smithsonian Center for Astrophysics, 60 Garden Street @2 Cambridge, MA 02138 @3 USA @Z 9 aut.
A14 09      @1 Department of Astraphysics, IMAPP, Radboud University Nijmegen, PO Box 9010 @2 6500 GL Nijmegen @3 NLD @Z 9 aut.
A14 10      @1 Department of Physics, University of California @2 Santa Barbara, CA 93106-9530 @3 USA @Z 10 aut.
A14 11      @1 MIT Kavli Institute for Astrophysics and Space Research, 70 Vassar Street @2 Cambridge, MA 02139 @3 USA @Z 11 aut.
A14 12      @1 School of Physics and Astronomy, University of Southampton @2 Southampton, Hampshire SO17 IBJ @3 GBR @Z 12 aut.
A14 13      @1 ISAS, Japan Aerospace Exploration Agency, 3-1-1 Yoshinodai, chuo-ku @2 Sngamihara, Kanagawa 229-8510 @3 JPN @Z 13 aut.
A14 14      @1 Kapteyn Astronomical Institute, University of Groningen, PO Box 800 @2 9700 AV Groningen @3 NLD @Z 14 aut.
A14 15      @1 Department of Astronomy, University of Michigan, 500 Church Street @2 Ann Arbor, MI 48109 @3 USA @Z 16 aut. @Z 17 aut.
A14 16      @1 ESAC, ISOC, Villanueva de la Canada, Madrid P. O. Box 78 @2 28691 @3 ESP @Z 18 aut.
A20       @1 1740-1751
A21       @1 2012
A23 01      @0 ENG
A43 01      @1 INIST @2 2067 @5 354000506050220740
A44       @0 0000 @1 © 2012 INIST-CNRS. All rights reserved.
A45       @0 1 p.1/4
A47 01  1    @0 12-0042281
A60       @1 P
A61       @0 A
A64 01  1    @0 Monthly Notices of the Royal Astronomical Society
A66 01      @0 USA
C01 01    ENG  @0 We present optical monitoring of the black hole candidate XTE J1752-223 during its 2009-10 outburst and decay to quiescence. The optical light curve can be described by an exponential decay followed by a plateau, then a more rapid fade towards quiescence. The plateau appears to be due to an extra component of optical emission that brightens and then fades over ∼40 days. We show evidence for the origin of this optical 'flare' to be the synchrotron jet during the decaying hard state, and we identify and isolate both disc and jet components in the spectral energy distributions. The optical flare has the same morphology and amplitude as a contemporaneous X-ray rebrightening. This suggests a common origin, but no firm conclusions can be made favouring or disfavouring the jet producing the X-ray flare. The quiescent optical magnitudes are B ≥ 20.6, V ≥ 21.1, R ≥ 19.5, i' ≥ 19.2. From the optical outburst amplitude we estimate a likely orbital period of <22 h. We also present near-infrared (NIR) photometry and polarimetry and rare mid-IR imaging (8-12 μm) when the source is nearing quiescence. The fading jet component, and possibly the companion star, may contribute to the NIR flux. We derive deep mid-IR flux upper limits and NIR linear polarization upper limits. With the inclusion of radio data, we measure an almost flat jet spectral index between radio and optical; Fν <is proportional to> ν∼+0.05. The data favour the jet break to optically thin emission to reside in the IR, but may shift to frequencies as high as the optical or UV during the peak of the flare.
C02 01  3    @0 001E03
C03 01  3  FRE  @0 Jet @5 26
C03 01  3  ENG  @0 Jets @5 26
C03 02  3  FRE  @0 Trou noir @5 27
C03 02  3  ENG  @0 Black holes @5 27
C03 03  X  FRE  @0 Quiescence @5 28
C03 03  X  ENG  @0 Quiescence @5 28
C03 03  X  SPA  @0 Quietud @5 28
C03 04  3  FRE  @0 Courbe lumière @5 29
C03 04  3  ENG  @0 Light curves @5 29
C03 05  X  FRE  @0 Emission optique @5 30
C03 05  X  ENG  @0 Light emission @5 30
C03 05  X  SPA  @0 Emisión óptica @5 30
C03 06  X  FRE  @0 Sursaut optique @5 31
C03 06  X  ENG  @0 Optical burst @5 31
C03 06  X  SPA  @0 Arrebato óptico @5 31
C03 07  X  FRE  @0 Densité spectrale énergie @5 32
C03 07  X  ENG  @0 Spectral energy distribution @5 32
C03 07  X  SPA  @0 Densidad espectral energía @5 32
C03 08  3  FRE  @0 Morphologie @5 33
C03 08  3  ENG  @0 Morphology @5 33
C03 09  X  FRE  @0 Photométrie IR @5 34
C03 09  X  ENG  @0 Infrared photometry @5 34
C03 09  X  SPA  @0 Fotometría IR @5 34
C03 10  3  FRE  @0 Polarimétrie @5 35
C03 10  3  ENG  @0 Polarimetry @5 35
C03 11  X  FRE  @0 Borne supérieure @5 36
C03 11  X  ENG  @0 Upper bound @5 36
C03 11  X  SPA  @0 Cota superior @5 36
C03 12  3  FRE  @0 Polarisation rectiligne @5 37
C03 12  3  ENG  @0 Linear polarization @5 37
C03 13  3  FRE  @0 Indice spectral @5 38
C03 13  3  ENG  @0 Spectral index @5 38
C03 14  X  FRE  @0 Déplacement fréquence @5 39
C03 14  X  ENG  @0 Frequency shift @5 39
C03 14  X  SPA  @0 Desplazamiento frecuencia @5 39
C03 15  3  FRE  @0 Accrétion @5 40
C03 15  3  ENG  @0 Accretion @5 40
C03 16  3  FRE  @0 Disque accrétion @5 41
C03 16  3  ENG  @0 Accretion disks @5 41
C03 17  3  FRE  @0 Binaire RX @5 42
C03 17  3  ENG  @0 X-ray binary stars @5 42
C03 18  X  FRE  @0 Source RX binaire @5 43
C03 18  X  ENG  @0 Binary X ray source @5 43
C03 18  X  SPA  @0 Fuente RX binaria @5 43
C03 19  3  FRE  @0 Cosmologie @5 44
C03 19  3  ENG  @0 Cosmology @5 44
C03 20  3  FRE  @0 Source RX cosmique @5 45
C03 20  3  ENG  @0 Cosmic x-ray sources @5 45
N21       @1 023
N44 01      @1 OTO
N82       @1 OTO

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Pascal:12-0042281

Le document en format XML

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<title xml:lang="en" level="a">A late jet rebrightening revealed from multiwavelength monitoring of the black hole candidate XTE J1752-223</title>
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<term>Cosmic x-ray sources</term>
<term>Cosmology</term>
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<term>Trou noir</term>
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<term>Densité spectrale énergie</term>
<term>Morphologie</term>
<term>Photométrie IR</term>
<term>Polarimétrie</term>
<term>Borne supérieure</term>
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<div type="abstract" xml:lang="en">We present optical monitoring of the black hole candidate XTE J1752-223 during its 2009-10 outburst and decay to quiescence. The optical light curve can be described by an exponential decay followed by a plateau, then a more rapid fade towards quiescence. The plateau appears to be due to an extra component of optical emission that brightens and then fades over ∼40 days. We show evidence for the origin of this optical 'flare' to be the synchrotron jet during the decaying hard state, and we identify and isolate both disc and jet components in the spectral energy distributions. The optical flare has the same morphology and amplitude as a contemporaneous X-ray rebrightening. This suggests a common origin, but no firm conclusions can be made favouring or disfavouring the jet producing the X-ray flare. The quiescent optical magnitudes are B ≥ 20.6, V ≥ 21.1, R ≥ 19.5, i' ≥ 19.2. From the optical outburst amplitude we estimate a likely orbital period of <22 h. We also present near-infrared (NIR) photometry and polarimetry and rare mid-IR imaging (8-12 μm) when the source is nearing quiescence. The fading jet component, and possibly the companion star, may contribute to the NIR flux. We derive deep mid-IR flux upper limits and NIR linear polarization upper limits. With the inclusion of radio data, we measure an almost flat jet spectral index between radio and optical; F
<sub>ν</sub>
ν
<sup>∼+0.05</sup>
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<fC03 i1="04" i2="3" l="FRE">
<s0>Courbe lumière</s0>
<s5>29</s5>
</fC03>
<fC03 i1="04" i2="3" l="ENG">
<s0>Light curves</s0>
<s5>29</s5>
</fC03>
<fC03 i1="05" i2="X" l="FRE">
<s0>Emission optique</s0>
<s5>30</s5>
</fC03>
<fC03 i1="05" i2="X" l="ENG">
<s0>Light emission</s0>
<s5>30</s5>
</fC03>
<fC03 i1="05" i2="X" l="SPA">
<s0>Emisión óptica</s0>
<s5>30</s5>
</fC03>
<fC03 i1="06" i2="X" l="FRE">
<s0>Sursaut optique</s0>
<s5>31</s5>
</fC03>
<fC03 i1="06" i2="X" l="ENG">
<s0>Optical burst</s0>
<s5>31</s5>
</fC03>
<fC03 i1="06" i2="X" l="SPA">
<s0>Arrebato óptico</s0>
<s5>31</s5>
</fC03>
<fC03 i1="07" i2="X" l="FRE">
<s0>Densité spectrale énergie</s0>
<s5>32</s5>
</fC03>
<fC03 i1="07" i2="X" l="ENG">
<s0>Spectral energy distribution</s0>
<s5>32</s5>
</fC03>
<fC03 i1="07" i2="X" l="SPA">
<s0>Densidad espectral energía</s0>
<s5>32</s5>
</fC03>
<fC03 i1="08" i2="3" l="FRE">
<s0>Morphologie</s0>
<s5>33</s5>
</fC03>
<fC03 i1="08" i2="3" l="ENG">
<s0>Morphology</s0>
<s5>33</s5>
</fC03>
<fC03 i1="09" i2="X" l="FRE">
<s0>Photométrie IR</s0>
<s5>34</s5>
</fC03>
<fC03 i1="09" i2="X" l="ENG">
<s0>Infrared photometry</s0>
<s5>34</s5>
</fC03>
<fC03 i1="09" i2="X" l="SPA">
<s0>Fotometría IR</s0>
<s5>34</s5>
</fC03>
<fC03 i1="10" i2="3" l="FRE">
<s0>Polarimétrie</s0>
<s5>35</s5>
</fC03>
<fC03 i1="10" i2="3" l="ENG">
<s0>Polarimetry</s0>
<s5>35</s5>
</fC03>
<fC03 i1="11" i2="X" l="FRE">
<s0>Borne supérieure</s0>
<s5>36</s5>
</fC03>
<fC03 i1="11" i2="X" l="ENG">
<s0>Upper bound</s0>
<s5>36</s5>
</fC03>
<fC03 i1="11" i2="X" l="SPA">
<s0>Cota superior</s0>
<s5>36</s5>
</fC03>
<fC03 i1="12" i2="3" l="FRE">
<s0>Polarisation rectiligne</s0>
<s5>37</s5>
</fC03>
<fC03 i1="12" i2="3" l="ENG">
<s0>Linear polarization</s0>
<s5>37</s5>
</fC03>
<fC03 i1="13" i2="3" l="FRE">
<s0>Indice spectral</s0>
<s5>38</s5>
</fC03>
<fC03 i1="13" i2="3" l="ENG">
<s0>Spectral index</s0>
<s5>38</s5>
</fC03>
<fC03 i1="14" i2="X" l="FRE">
<s0>Déplacement fréquence</s0>
<s5>39</s5>
</fC03>
<fC03 i1="14" i2="X" l="ENG">
<s0>Frequency shift</s0>
<s5>39</s5>
</fC03>
<fC03 i1="14" i2="X" l="SPA">
<s0>Desplazamiento frecuencia</s0>
<s5>39</s5>
</fC03>
<fC03 i1="15" i2="3" l="FRE">
<s0>Accrétion</s0>
<s5>40</s5>
</fC03>
<fC03 i1="15" i2="3" l="ENG">
<s0>Accretion</s0>
<s5>40</s5>
</fC03>
<fC03 i1="16" i2="3" l="FRE">
<s0>Disque accrétion</s0>
<s5>41</s5>
</fC03>
<fC03 i1="16" i2="3" l="ENG">
<s0>Accretion disks</s0>
<s5>41</s5>
</fC03>
<fC03 i1="17" i2="3" l="FRE">
<s0>Binaire RX</s0>
<s5>42</s5>
</fC03>
<fC03 i1="17" i2="3" l="ENG">
<s0>X-ray binary stars</s0>
<s5>42</s5>
</fC03>
<fC03 i1="18" i2="X" l="FRE">
<s0>Source RX binaire</s0>
<s5>43</s5>
</fC03>
<fC03 i1="18" i2="X" l="ENG">
<s0>Binary X ray source</s0>
<s5>43</s5>
</fC03>
<fC03 i1="18" i2="X" l="SPA">
<s0>Fuente RX binaria</s0>
<s5>43</s5>
</fC03>
<fC03 i1="19" i2="3" l="FRE">
<s0>Cosmologie</s0>
<s5>44</s5>
</fC03>
<fC03 i1="19" i2="3" l="ENG">
<s0>Cosmology</s0>
<s5>44</s5>
</fC03>
<fC03 i1="20" i2="3" l="FRE">
<s0>Source RX cosmique</s0>
<s5>45</s5>
</fC03>
<fC03 i1="20" i2="3" l="ENG">
<s0>Cosmic x-ray sources</s0>
<s5>45</s5>
</fC03>
<fN21>
<s1>023</s1>
</fN21>
<fN44 i1="01">
<s1>OTO</s1>
</fN44>
<fN82>
<s1>OTO</s1>
</fN82>
</pA>
</standard>
</inist>
</record>

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   |texte=   A late jet rebrightening revealed from multiwavelength monitoring of the black hole candidate XTE J1752-223
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