The g-ray giant flare
from SGR1806-20
K1 SGR 1806-20: first evidence of crustal cracking
| SGR 1806-20 Crustal Cracking
during a giant g-ray flare |
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Authors: Steven J. Schwartz, Silvia Zane, Robert J. Wilson, Frank P. Pijpers, Daniel R. Moore,
D. O. Kataria, Timothy S. Horbury, Andrew N. Fazakerley, Peter J. Cargill |
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Journal-ref: ApJ 627 (2005) L129-L132 [astro-ph/0504056
] |
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Title:
The Gamma-Ray Giant Flare from SGR 1806-20: Evidence of Crustal Cracking via Initial Timescales |
Abstract:
Soft gamma-ray repeaters (SGRs) are neutron stars that emit short (<~1 s) and
energetic (<~ 1042 erg s-1) bursts of soft gamma-rays. Only four of them are currently
known. Occasionally, SGRs have been observed to emit much more energetic "giant flares''
(~1044 - 1045 erg s-1).
These are exceptional and rare events.
We report here on serendipitous
observations of the intense gamma-ray flare from SGR 1806-20 that occurred on 2004 December 27.
Unique data from the Cluster and Double Star TC-2 satellites, designed to study the Earth's
magnetosphere, provide the first observational evidence of three separate timescales within
the early (first 100 ms) phases of this class of events. These observations reveal that
in addition to the initial very steep (<0.25 ms) X-ray onset, there is first a 4.9 ms
exponential rise timescale followed by a continued exponential rise in intensity on a
timescale of 70 ms. These three timescales are a prominent feature of current theoretical models,
including the timescale (several milliseconds) for fracture propagation in the crust of the neutron star.
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[21 Sep 2005]
On 27 December 2004, radiation from the biggest
starquake on a neutron star ever recorded reached Earth. Unique data
obtained by Double Star TC-2 and Cluster satellites enabled a group of
European scientists to find the first observational evidence of cracks in
the neutron star crust, during the initial phase of the starquake. This
result, published 16 June 2005 in the Astrophysical Journal, dicriminates
between current theories on the physical origin of such massive starquakes.
Credit: NASA/HST/ASU/J. Hester et al., NASA/CXC/ASU/J. Hester et al.
Image 1. The Crab pulsar in a composite view from Hubble (optical in blue) and Chandra (X-ray in red).
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Neutron stars and pulsars
Millions of neutron stars populate our Milky Way galaxy. A neutron star
is the remaining core of a massive star, once it has exploded. Made almost
entirely of neutrons (subatomic particles with no electric charge), this
stellar corpse concentrates more than the mass of our Sun within a sphere
of ~20 km diameter. It is so dense that a sugar cube of neutron star on
Earth would weight as much as all of humanity!
Two other physical properties characterise a neutron star, their fast
rotation (or spin) and their high magnetic field.
Astronomers have found
different classes of neutron stars based on these properties. Some of them
are the fastest spinning stars in the Universe (up to hundreds of
revolutions per second); named pulsars (Image 1), as they generate regular
pulses of electromagnetic radiation including radio, visible, X-ray and
gamma-ray wavelengths.
These pulses are often compared to a spinning
lighthouse beacon which appears to flash on and off.
Credit: NASA
Image 2. Artistic impression of cracks on a magnetar in the initial phase of a starquake
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Magnetars
Another class of neutron stars is known as magnetars (Image 2), due to
their ultra-high magnetic field. Their magnetic field intensity is indeed
about 100 gigaTesla (or 1011 T), a thousand times more than an
ordinary neutron star. By comparison, the Earth's magnetic field is about
50 microTesla (5×10-5 T). Most media used for data storage can
be erased if they are exposed to a magnetic field of milliTesla
(10-3 T) intensity.
So far, a dozen of magnetars have been found. Four of them are also
known as soft gamma repeaters, or SGRs, because they sporadically release
large bursts of low energy (soft) gamma rays and (hard) X-rays, usually
during short time periods (~ 0.1 s).
Credit: NASA
Image 3. SGR 1806-20 location.
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Extreme starquake on 27 December 2004
On 27 December 2004, the radiation from an extremely powerful explosion
on the surface of SGR 1806-20 (the numbers indicate its position in the
sky) reached Earth and lasted more than 6 minutes. During the first 200
ms, the amount of energy released was equivalent to what our Sun radiates
in 250 000 years. It is the brightest event known to have impacted the
Earth from an origin outside our solar system.
SGR 1806-20 is located at around 50 000 light-years from Earth on the
far side of our Milky Way galaxy, in the direction of the Sagittarius
constellation (Image 3). A similar blast within 10 light years would have
destroyed the ozone layer and be similar to a major nuclear blast.
Fortunately, the closest known magnetar is 13 000 light years away.
Credit: NASA
Video 1. Artist's impression of a giant flare from a magnetar after the cracking of its surface.
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Missing link found by Double Star and Cluster
Several scientific satellites observed the
giant flare experienced by SGR 1806-20, including ESA γ-ray observatory
INTEGRAL (see related publication by Israel, G.L., et al.). The intensity
of the emissions received may be roughly described as a major peak
followed by a modulated decrease. However, the intensity of this major
peak was hundreds of times stronger than any other observed so far (only
two other giant flares have been recorded in the past 35 years). "For
the first 200 ms it saturated almost all instruments on satellites
equipped to observe γ-rays", underlined Prof. Steve J. Schwartz from
Imperial College London (UK) in his 16 June 2005 Astrophysical Journal paper.
Although designed to study the Earth's magnetosphere, the thermal
electron detectors onboard Double star TC-2 and Cluster satellites
performed unsaturated observations of this initial flare rise and decay
(Image 4). As explained in his 16 June paper, Professor Schwartz and his
co-authors show that these unique data provide the first observational
evidence of three separate timescales within the first 100 ms of this
event. The characteristics of these timescales (such as the number,
duration, shape) play an important role in actual theories of starquakes
on magnetars, which allows discriminating between them.
Based on these measured timescales and current theoretical models, the
following scenario is confirmed in this paper. The giant flare is produced
when the crust of the magnetar can no longer respond almost plastically to
internal magnetic stress and finally cracks. One of the three timescales
even allows an estimation of the fracture size: about 5 km. This is a
significant size considering that SGR 1806-20 has been estimated to be a
sphere of few tens of km in diameter.
Credit: Schwartz et al., 2005]
Image 4.
Combined Double Star TC-2 (triangles) and Cluster 4 High Energy Electron Analyser (gray
circles) count rates. The data have been shifted in time to align
features near the peak count rates. Solid lines show exponential
fits to the steepest TC-2 rise, and also to the TC-2 determination of the period leading to the main peak
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Presence of quasi-periodic oscillations
On 27 June 2005, the Astrophysical Journal published a related study on
SGR 1806-20, this time led by Italian astronomer GianLuca Israel from
INAF-Osservatorio Astronomico di Roma. His data analysis reveals the
presence of quasi-periodic oscillations (or modes) at the end of the 27
December 2004 event.
"These modes are likely to be associated with global seismic
oscillations. In particular, the large crustal fracturing inferred by us
can easily excite toroidal modes with characteristic frequencies in the
observed range", commented Professor Schwartz in his 16 June paper.
Therefore, Double Star TC-2 and Cluster data have not only enabled to
directly estimate crustal properties of magnetars, they have also linked
interior magnetic processes and their external consequences during giant flares.
"Cluster and Double Star were designed to study the various
boundary layers of the Earth's magnetosphere, including the physics of
magnetic reconnection. Such boundary layer physics has application
throughout the astrophysical plasma universe, and it is therefore
appropriate that these missions contribute in a more direct way to the
study of magnetic reorganisation in an astrophysical object outside the
solar system", concluded Professor Schwartz.
This new result illustrates the complementarity of the Double Star and
the Cluster missions. New results from both missions will be discussed
this week (19-23 September) at ESTEC during a five day symposium gathering
more than 200 researchers coming from Europe, USA, China and Japan.
Related articles
K. Hurley, S. E. Boggs, D. M. Smith, R. C. Duncan, R. Lin, A. Zoglauer,
S. Krucker, G. Hurford, H. Hudson, C. Wigger, W. Hajdas, C. Thompson, I.
Mitrofanov, A. Sanin, W. Boynton, C. Fellows, A. von Kienlin, G. Lichti,
A. Rau, T. Cline, (RHESSI)
An exceptionally bright flare from SGR 1806–20 and the
origins of short-duration γ-ray bursts, Nature 434, 1098-1103 (28 April
2005)
Israel, G. L., T. Belloni, L. Stella, Y. Rephaeli, D. E. Gruber, P. Casella, S. Dall'Osso, N. Rea,
(RXTE)
Discovery of rapid X-ray oscillations in the tail of the SGR 1806-20 hyperflare,
ApJ, 628:L53–L56, 2005
K2
SGR 1806-20 recorded by INTEGRAL SPI Anti-Coincidence Shield
Zum Thema |
Teil 1 Gamma-Blitz traf die Erde
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The first giant flare from SGR 1806-20
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Gamma-Blitz von Magnetar trifft Erde Lösung für mysteriöses kosmisches Rätsel?
[21 Sep 2005] (G. Lichti, A. von Kienlin)
Abb. 1: Magnetar mit extrem starken Magnetfeld.
Solch ein Objekt wird als Ort des Gammastrahlenausbruchs vermutet. (Bild: R. Mallozzi/NASA)
Abb. 2: Lichtkurve des Ausbruchs von SGR 1806-20, gemessen mit dem Antikoinzidenzschild des
Spektrometers SPI auf dem INTEGRAL-Satelliten. Zu sehen ist der kurze Hauptausbruch bei 0 Sekunden,
von dem nur der unterste Teil zu sehen ist. Das Maximum ist etwa 22 mal höher als im Bild gezeigt.
Danach setzt das pulsierende Nachleuchten ein, das bis etwa 200 Sekunden deutlich zu sehen ist.
(Bild: A. von Kienlin, MPE)
Abb. 3: Überblick und Details der Lichtkurve des Ausbruchs von SGR 1806-20. (Bild: A. von Kienlin, MPE)
Am 27. Dezember 2004 um 22:30:26 MEZ wurde die Erde von einer gewaltigen Wellenfront von Gamma- und
Röntgenstrahlung getroffen. Es war der stärkste Fluß von hochenergetischer
Strahlung, der bisher auf der Erde gemessen wurde. Er war sogar stärker
als der stärkste jemals gemessene Flare (Strahlungsausbruch) von der
Sonne. Das interessante an dieser Entdeckung ist die Entstehung dieser
Strahlung. Sie stammt nämlich von einem winzigen Himmelskörper, einem
extrem dichten Neutronenstern mit einem äußerst starken Magnetfeld, der
sich auf der anderen Seite unserer Milchstraße in etwa 50 000
Lichtjahren Entfernung befindet. Dieser Magnetar, der einen Durchmesser
wie eine mittlere Großstadt und eine Masse vergleichbar mit der Sonne hat,
erlitt eine gewaltige magnetische Instabilität, wobei sich sein starkes
Magnetfeld in einen niedrigeren Energiezustand umorientierte. In den
ersten 0.2 s wurde von diesem Objekt die gleiche Energiemenge emittiert
wie von der Sonne in etwa einer Viertelmillion Jahren. Dieser Ausbruch war
etwa 100-mal stärker als der bisher stärkste Ausbruch von einem Magnetar.
Verständlich, daß dieses Ereignis Wissenschaftler auf der ganzen Welt,
darunter auch Wissenschaftler des Max-Planck-Institut für
extraterrestrische Physik in Garching bei München, in Aufregung versetzte
und sie die Daten schnell auswerteten. Erste Ergebnisse sind in einem
Artikel enthalten, der vor kurzem bei Nature zur Veröffentlichung
eingereicht wurde. Sie werfen ein neues Licht auf die Physik von
Magnetaren und tragen dazu bei, ein seit langem existierendes Rätsel um
kosmische Gamma-Strahlenbursts lösen zu können.
Dieses seltene Ereignis wurde von einem Detektor gemessen und sofort
weltweit bekannt gemacht, der von einer Gruppe am Max-Planck-Institut für
extraterrestrische Physik für die INTEGRAL-Mission der ESA gebaut wurde.
Es handelt sich dabei um ein Antikoinzidenzschild des
INTEGRAL-Spektrometers SPI, das aus 91 Blöcken aus sehr schweren und somit
gut für den Nachweis von Gammastrahlung geeigneten
Wismutgermanat-Kristallen (BGO) besteht, die insgesamt 512 kg wiegen.
Dieses Schild, dessen Hauptaufgabe darin besteht, den Hauptdetektor von
SPI von Hintergrundstrahlung abzuschirmen, wird auch als
Gammastrahlendetektor verwendet. Es handelt sich dabei um einen der
sensitivsten Gammaburstdetektoren, der zur Zeit die Erde umkreist. "Allein
durch die Messung dieses Strahlenausbruches hat sich die Entwicklung
dieses Burstdetektors gelohnt", sagt Giselher Lichti, unter dessen Führung
dieser Detektor entwickelt und gebaut wurde. Später wurde dann
festgestellt, daß dieser Burst auch noch von 13 anderen Röntgen- und
Gammadetektoren gemessen wurde, die im interplanetaren Raum zwischen Erde
und Saturn Messungen durchführen. Sogar der russische Coronas-F Satellit
sah diesen Burst, obwohl er sich zur Zeit des Ereignisses hinter der Erde
befand, er die direkte Strahlung von der Quelle also gar nicht messen
konnte. Eine Analyse der Ankunftszeiten ergab, daß dieses Instrument
Gammastrahlen von diesem Burst gemessen hatte, die von der Mondoberfläche reflektiert worden waren.
Wegen der Stärke des Bursts und seiner
durchdringenden Strahlung konnten auch Detektoren diesen Burst messen, die
nicht auf die Stelle am Himmel gerichtet waren, von dem die Strahlung kam.
Die Gammastrahlung durchdrang nämlich die Abschirmungen aus Metall oder
Kristallen und brachte die Detektoren kurzzeitig in die Sättigung. Zum
Glück ist die Atmosphäre für diese Strahlung undurchdringlich, da sie die
Atome der Hochatmosphäre ionisiert und dabei absorbiert wird, so daß das
Leben auf der Erde nicht in Gefahr war. Lediglich die auf dem Satelliten
Integral angebrachten Zähler des vom Max-Planck-Institut für
extraterrestrische Physik gebauten Burstdetektors sind so ausgelegt, daß
sie nicht gesättigt wurden. "Das Verhalten der vom MPE gebauten Detektoren
unter so hohem Strahlungsfluß muß noch genauer untersucht werde, um eine
direkte Abschätzung der gesamten Energieabstrahlung dieses Ereignisses zu
erlauben", sagt Andreas von Kienlin, ebenfalls Wissenschaftler am MPE, der
das Instrument am Boden und im Orbit kalibriert und eingestellt hat. Mit
einer Zeitauflösung von 50 ms liefert das vom Max-Planck-Institut für
extraterrestrische Physik gebaute Instrument auch eine hochaufgelöste Lichtkurve.
Very-Large Array in Socorro, New Mexico,
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Die Position des Objektes, das den Ausbruch zeigte, befindet sich in
der Konstellation Sagittarius (zur Zeit des Ausbruchs nur etwa 5º von der
Sonne entfernt), in der Nähe des galaktischen Zentrums. Mit Hilfe des
interplanetaren Netzwerkes, einem Zusammenschluß von mehreren
Satellitenmissionen, gelang es Kevin Hurley von der Universität Berkeley
in Kalifornien mittels Triangulation die Position des Objektes so genau zu
bestimmen, daß man es mit dem bekannten Magnetar SGR 1806-20
identifizieren konnte (SGR steht für Soft Gamma-Ray Repeater, weil diese
Sterne gelegentlich Bursts von weicher Gammastrahlung emittieren). Diese
Position wurde sehr genau von Radioastronomen des Very-Large Array in
Socorro, New Mexico, durch Messung eines verglimmenden Nachleuchtens bei
Radiowellen bestätigt. Die Beobachtung dieses Nachleuchtens liefert
außerdem wichtige Informationen über den Explosionsmechanismus und wird zu
einem besseren Verständnis des beobachteten Phänomens beitragen.
Der Ausbruch begann mit der Emission von harter Gammaemission, die nur
einen Bruchteil einer Sekunde dauerte, aber den Großteil der emittierten
Energie enthielt. Dieser Ausbruch war gefolgt von einer schwächeren
Röntgenemission, die mehr als 6 Minuten andauerte und deren Intensität mit
einer Periode von 7.56 s oszillierte. Diese Oszillation wird mit der
Rotationsperiode des Neutronensterns in Verbindung gebracht. Die
Messungen zeigten, daß die Energieverteilung der Gammaquanten des
Hauptausbruches charakteristisch für ein ultra-heißes thermisches Glühen
(Plasma) ist. Genau das, was die Wissenschaftler von einem Magnetar
erwarten, der leichte hochenergetische Teilchen ausstößt (im wesentlichen
Elektronen und Positronen, den Antiteilchen der Elektronen). Die meisten
dieser Teilchen zerstrahlten offensichtlich in reine Gammastrahlen, die
dann in den interstellaren Raum entwichen. Radiobeobachtungen erzählen uns
jedoch, daß wenig Strahlung von diesen Teilchen selbst im Radiobereich
erzeugt wurde. Die oszillierende Röntgenemission stammt offenbar von
übriggebliebenen Elektronen, Positronen und Gammastrahlen, die im
Magnetfeld des Magnetars eingeschlossen sind. Die Theorie sagt vorher, daß
solch ein heißer eingeschlossener Feuerball (trapped fireball) innerhalb
von Minuten schrumpfen und verdampfen sollte. Seine Helligkeit scheint zu
oszillieren, weil der Feuerball über das Magnetfeld on die Oberfläche des
rotierenden Neutronensterns gebunden ist.
Bild: A. von Kienlin, MPE
Lichtkurve des Ausbruchs von SGR 1806-20, gemessen mit dem Antikoinzidenzschild des
Spektrometers SPI auf dem INTEGRAL-Satelliten. Zu sehen ist der kurze Hauptausbruch bei 0 Sekunden,
von dem nur der unterste Teil zu sehen ist. Das Maximum ist etwa 22 mal höher als im Bild gezeigt.
Danach setzt das pulsierende Nachleuchten ein, das bis etwa 200 Sekunden deutlich zu sehen ist.
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Die riesige Energiemenge des Ausbruchs vom 27. Dezember 2004 legt eine
neue Lösung für ein altes Problem der Gammastrahlen-Burstastronomie nahe.
Es handelt sich um die Frage, was die Quellen der so genannten
"Short-Duration Gamma-Ray Bursts" sind. In den letzten 35 Jahren hat man
Hunderte von kurzen (<2 s) mysteriösen Blitzen von hochenergetischer
Strahlung aus den Tiefen des Raumes gemessen, ohne daß man weiß, woher
diese gemessene Strahlung kommt. Eine Hypothese besagt, daß diese
Strahlung bei der Verschmelzung von zwei kompakten Objekten (z. B. von
zwei Neutronensternen oder einem Neutronensternmit einem Schwarzen Loch)
entstehen könnte. Die neuen Beobachtungen lassen nun eine weitere
Interpretation der Beobachtungen zu. Es könnte sich dabei nämlich zum Teil
um Ausbrüche wie dem am 27. Dezember beobachteten handeln. Danach können
solche kurzen Ausbrüche auf Grund ihrer Intensität von sehr fernen
Galaxien beobachtet werden. Ein Ereignis mit der vor kurzem gemessen
Stärke könnte bis zu Entfernungen von einigen Hundertmillionen Lichtjahren
beobachtet werden. Da sich in diesem Entfernungsbereich viele Galaxien
befinden müßte man solche Ereignisse häufig sehen. Man könnte damit also
die Beobachtungen zu einem beträchtlichen Teil, wenn nicht sogar ganz, erklären.
Wie kann man sich nun den enormen Energieausstoß von einem solchen
Magnetar erklären? Die Erfinder des Magnetarmodells, die Theoretiker
Robert Duncan und Christopher Thompson, schlagen
folgendes neue Szenario vor, um den gigantischen Energieausstoß bei einem
solchen Flare erklären zu können: um ihre Idee verstehen zu können, muß
man sich erst einmal das ungeheuer starke Magnetfeld eines Magnetars
bewußt machen, das um einen Faktor 1000 stärker ist als das eines normalen
Neutronensterns (das bereits eine Billion (1012) mal stärker
ist als das Magnetfeld der Erde). In solchen starken Feldern wird z. B.
ein Wasserstoffatom so stark deformiert, daß es nadelförmig wird (~200 mal
schmäler als lang). So ein Stern hat tief in seinem Inneren ein stark
verdrilltes Magnetfeld, dessen Magnetfeldlinien sich wie eine Uhrfeder um
die Rotationsachse winden. Sein äußeres Magnetfeld jedoch ähnelt mehr oder
weniger dem eines Dipols eines Stabmagneten (vergleichbar dem
Erdmagnetfeld). Man glaubt, daß das verdrillte innere Magnetfeld das
Überbleibsel der schnellen Rotation ist, die der Stern bei seiner Geburt
mitbekam. Es enthält den größten Teil der magnetischen Energie des Sterns.
Dieses Magnetfeld übt unvermeidlicherweise eine Kraft von unten auf die 1
km dicke Kruste des Sterns mit einem Radius von 10 km aus. Mit der Zeit
wird diese Kraft die Kruste so verschieben, daß die nördliche magnetische
Hemisphäre sich gegenüber der südlichen verschiebt. Das hat zum einen zur
Folge, daß sich das äußere Magnetfeld verdrillt und zum anderen, daß
starke Ladungsströme um den Stern fließen. Wenn sich die Magnetfelder
immer stärker verdrillen, dann lassen diese Ströme den Stern hell im
hochenergetischen Röntgenbereich aufscheinen. Die Verdrillung des äußeren
Magnetfeldes beeinflußt auch die Rotation des Sterns und führt zu einer stärkeren Abbremsung.
Das scheint mit dem Magnetar SGR 1806-20 im Jahr
2004 passiert zu sein. Von März 2004 bis zum Ausbruch im Dezember hat SGR
1806-20 viele einzelne schwache Ausbrüche gezeigt, die auf eine
Verschiebung der Kruste hindeuteten (diese Ausbrüche waren weniger stark
als der Riesenausbruch vom Dezember, aber einzelne Bursts emittierten in
einem Bruchteil einer Sekunde immer noch soviel Energie wie die Sonne in
einem Jahr). SGR 1806-20 wurde also immer heller im Röntgenlicht, mit
Emission von immer mehr harten Röntgenphotonen und einer stärkeren
Abbremsung. Alle diese Messungen deuteten darauf hin, daß sich das äußere
Magnetfeld mehr und mehr verdrillte. In dem Modell für den Ausbruch vom
27. Dezember von Duncan und Thompson wurde die Verdrillung so stark, daß
der Stern mit seiner Kruste instabil wurde. Die Spannung des äußeren
Magnetfelds hat sich dann in einem enormen Ausbruch entladen und das
Magnetfeld hat sich dann in einem niedrigeren und unverdrillten Zustand neu angeordnet.
K3 Supergiant Fast X-ray Transients (SFXTs)
[16 November 2005]
Eine neue Klasse von Röntgendoppelsternen
mit Superriesen als Partner eines kompakten Objekts
(vermutlich eines Neutronensterns) hat der ESA-Satellit Integral entdeckt - und von solchen
»supergiant fast X-ray transients« könnte es sogar eine Menge in der Milchstraße geben,
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Supergiant Fast X-ray Transients — A new class |
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Authors: Ignacio Negueruela, David M. Smith, Pablo Reig, Sylvain Chaty, Jose Miguel Torrejon |
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Journal-ref: ESA-SP 604 (2005) Proceedings of "The X-ray Universe 2005" [astro-ph/0511088 ] |
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Title: Supergiant Fast X-ray Transients:
A new class of high mass X-ray binaries unveiled by INTEGRAL |
| Abstract:
INTEGRAL monitoring of the Galactic Plane is revealing a growing number of
recurrent X-ray transients, characterised by short outbursts with very fast
rise times (~ tens of minutes) and typical durations of a few hours. Here we
show that several of these transients are associated with OB supergiants and
hence define a new class of massive X-ray binaries which we call Supergiant
Fast X-ray Transients (SFXTs). Many other transient X-ray sources display
similar X-ray characteristics, suggesting that they belong to the same class.
Since they are difficult to detect and their number is growing fast and
steadily, they could represent a major class of X-ray binaries.
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Integral reveals new class of ‘supergiant’ X-ray binary stars
ESA’s Integral gamma-ray observatory has discovered a new, highly populated class
of X-ray fast ‘transient’ binary stars, undetected in previous observations.
With this discovery, Integral confirms how much it is contributing to revealing a whole hidden Universe.
The new class of double star systems is characterised by a very compact object that produces highly energetic,
recurrent and fast-growing X-ray outbursts, and a very luminous ‘supergiant’ companion.
INTEGRAL / Blondin
Interaction between compact stellar object and wind of a supergiant
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The compact object can be an accreting body such as a black hole, a neutron star or a pulsar. Scientists
have called such class of objects ‘supergiant fast X-ray transients’. ‘Transients’ are systems
which display periods of enhanced X-ray emission.
Before the launch of Integral, only a dozen X-ray binary stars containing supergiants had been detected.
Actually, scientists thought that such high-mass X-ray systems were very rare, assuming that only a few of
them would exist at once since stars in supergiant phase have a very short lifetime.
However, Integral’s data combined with other X-ray satellite
observations indicate that transient supergiant X-ray binary systems
are probably much more abundant in our Galaxy than previously thought.
In particular, Integral is showing that such ‘supergiant fast X-ray transients’, characterised by
fast outbursts and supergiant companions, form a wide class that lies hidden throughout the Galaxy.
Supergiant fast X-ray transients
IBIS / INTEGRAL
The figure shows an artist's impression of the stellar wind and mass transfer around a supergiant with a
light curve observed with IBIS onboard INTEGRAL overlayed.
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Due to the transitory nature, in most cases these
systems were not detected by other observatories because they lacked
the combination of sensitivity, continuous coverage and wide field of view of Integral.
They show short outbursts with very fast rising times – reaching
the peak of the flare in only a few tens of minutes – and typically
lasting a few hours only. This makes the main difference with most
other observed transient X-ray binary systems, which display longer
outbursts, lasting typically a few weeks up to months.
In the latter case, the long duration of the outburst is
consistent with a ‘viscous’ mass exchange between the star and an accreting compact object.
In ‘supergiant fast X-ray transients’, associated with highly
luminous supergiant stars, the short duration of the outburst seems
to point to a different and peculiar mass exchange mechanism between the two bodies.
This may have something to do with the way the strong radiative
winds, typical of highly massive stars, feed the compact object with stellar material.
Interaction between compact stellar object and wind of a supergiant
Scientists are now thinking about the reasons for such short outbursts. It could be due to the supergiant
donor ejecting material in a non-continuous way. For example, a clumpy and intrinsically variable nature of
a supergiant’s radiative winds may give rise to sudden episodes of increased accretion rate, leading to the
fast X-ray flares.
Alternatively, the flow of material transported by the wind may become, for reasons not very well understood,
very turbulent and irregular when falling into the enormous gravitational potential of the compact object.
“In any case, we are pretty confident that the fast outbursts are associated to the mass transfer mode from
the supergiant star to the compact object,” says Ignacio Negueruela.
“We believe that the short outbursts cannot be related to the nature of the compact companion, as we observed
fast outbursts in cases where the compact objects were very different - black holes, slow X-ray pulsars or
fast X-ray pulsars.”
Studying sources such as ‘supergiant fast X-ray transients’, and understanding the reasons for their behaviour,
is very important to increase our knowledge of accretion processes of compact stellar
objects. Furthermore, it is providing valuable insight into the
evolution paths that lead to the formation of high-mass X-ray binary systems.
Though the role of Integral has been key in the discovery of this
class of objects, there have been important contributions from other X-ray satellites.
In particular, the work that led to this discovery was started by US collaborator David Smith, using
Rossi XTE data on XTE J1739-302, appearing in the article ‘XTE J1739-302 as a supergiant fast X-ray transient’
by D.M. Smith, et al. 2006.
K3.2 XTE J1739-285 (n = 1122 Hz)
Zum Thema |
J1748-2446ad — Spinning Pulsar Smashes Record
|
Gravitationsstrahlung
|
|
XTE J1739-285 — n = 1122 Hz |
 |
Authors: P. Kaaret, Z. Prieskorn, J.J.M. in 't Zand, S. Brandt, N. Lund, S. Mereghetti, D. Gotz,
E. Kuulkers, J.A. Tomsick |
 |
Journal-ref: ApJ 657 (2007) L97 [astro-ph/0611716 ] |
 |
Title: Discovery of 1122 Hz X-Ray Burst Oscillations from the Neutron-Star X-Ray Transient
XTE J1739-285 | Abstract:
We report the discovery of oscillations at 1122 Hz in an X-ray burst
from the X-ray transient XTE J1739-285. The signal has a peak Leahy power of
42.8 and, after consideration of the number of trials, has a chance probability
of occurrence of 4 × 10-5 equivalent to a 4.2 sigma detection.
The oscillation frequency suggests that XTE J1739-285 contains the fastest rotating neutron
star yet found. We also found millisecond quasiperiodic oscillations in the
persistent emission with frequencies ranging from 757 Hz to 862 Hz.
We detected
seven X-ray bursts and derive an upper limit on the source distance of about 10.6 kpc from the brightest burst.
1. Introduction
Weakly magnetized neutron stars can be spun up to rates of several 100 Hz by accretion in low-mass X-ray
binaries (Alpar et al. 1982). The first direct measurements of millisecond spin rates in actively accreting
neutron stars in low-mass X-ray binaries (LMXBs) came from the discovery of oscillations in thermonuclear X-ray
bursts occurring on the neutron star surface (Strohmayer et al. 1996).
The burst oscillation frequencies were later found to be nearly equal to those of coherent pulsations
implying that the burst oscillation frequency indicates the neutron star spin rate. This X-ray technique has
no known biases against the detection of very high spin rates, unlike radio pulsation searches, and the sample
of X-ray burst oscillation frequencies has been exploited to constrain the neutron star spin rate distribution.
Analysis of a sample of 11 X-ray measured spin frequencies in the range 270-619 Hz suggests a limiting spin
rate near 760 Hz if the distribution is uniform and bounded (Chakrabarty et al. 2003). This is below the
expected maximum spin frequency possible without centrifugal breakup and has been interpreted as evidence that
some physical process, possibly gravitational radiation, limits the maximum possible spin rate.
However, the discovery of a radio pulsar spinning at 716 Hz, a frequency above
any previously measured in X-rays, suggests that the true maximum spin rate is higher (Hessels et al. 2006).
Here, we describe observations made with the Rossi X-Ray Timing Explorer (RXTE)
following the detection of X-ray bursts from the transient source XTE J1739-285 as part of a program to search
for millisecond oscillations in both X-ray bursts and persistent emission from neutron star X-ray binaries which
are newly discovered or found to be active. We detected seven X-ray bursts and found oscillations at a frequency
of 1122 Hz in the brightest burst. This suggests that XTE J1739-285 contains the most rapidly rotating neutron
star yet discovered.
2. OBSERVATIONS OF XTE J1739-285
XTE J1739-285 was discovered during RXTE PCA scans of the Galactic bulge on 1999 October 19
(Markwardt et al. 1999) and underwent short outbursts in May 2001 and October 2003. The source became
active again in August 2005 (Bodaghee et al. 2005) and two X-ray bursts were detected with the JEM-X instrument
on INTEGRAL on 2005 September 30 and October 4 (Brandt et al. 2005).
Triggered by the detection of the X-ray bursts, we obtained 19 observations using RXTE in the period
beginning 2005 October 12 and ending 2005 November 16.
References
Alpar, M.A., A.F. Cheng, M.A. Ruderman, J. Shaham, 1982 Nature 300, 728
Chakrabarty, D., Morgan, E.H., Muno, M.P., Galloway, D.K., et al. 2003, Nature 424, 42
Hessels, J.W.T, Ranson, S.M., Stairs, I.H., Freire, C.C., Kaspi, V.M., Camilo, F. 2006, Science 311, 1901
Strohmayer, T.E., et al., 1996, ApJ 469, L9
Strohmayer, T.E. & Markwardt, C.B. 2002, ApJ 577, 337
Strohmayer, T.E. & Markwardt, C.B., Swank, J.H., in ’t Zand, J. 2003, ApJ 596, L67
|
|
Integral points to the fastest spinning neutron star
[16 February 2007] Astronomers using ESA's gamma-ray observatory, Integral, have detected what appears to be
the fastest spinning neutron star yet. This tiny stellar corpse is spinning 1122 times every second.
If confirmed, the discovery gives astronomers the chance to glimpse the insides of the dead star.
|
The neutron star, known by its catalogue number XTE J1739-285, was discovered during one of its active phases
on 19 October 1999 by NASA's Rossi X-Ray Timing Explorer (RXTE) satellite. In August 2005, while Integral was
monitoring the bulge of the Galaxy, XTE J1739-285 started to come back to life. About a month later Integral
discovered the first short bursts of X-rays from the object.
Image credit: NASA/Dana Berry
Fig. .— This artist's impression shows a spinning neutron star (pulsar) approximately 10 kilometres in diameter.
When a neutron star orbits another star, its strong gravitational field can pull gas from the other star.
This coats the surface of the neutron star. When the coating reaches a height of between 5-10 metres, the gas
ignites in a thermonuclear explosion. This massive release of energy generally lasts from between several
seconds to several minutes and a burst of X-rays is released.
|
Erik Kuulkers, who leads the Galactic bulge monitoring programme, informed Philip Kaaret,
that things were still hotting up near the end of October. Kaaret arranged for the RXTE satellite to observe
XTE J1739-285 between 31 October and 16 November.
Together the two satellites recorded about twenty bursts between September and November.
Just because a star dies, it doesn't mean its life is over. A neutron star is the tiny heart of a collapsed
star. Measuring about 10 kilometres across, yet containing something like the mass of the Sun, the interior of
a neutron star is the most exotic realm that astronomers can imagine. According to their calculations a
thimbleful of neutron star material weighs a hundred million tonnes.
When a neutron star orbits another star, its strong gravitational field can pull gas from the other star.
This coats the surface of the neutron star. When the coating reaches a height of between 5-10 metres, the gas
ignites in a thermonuclear explosion. This massive release of energy generally lasts from between several
seconds to several minutes and a burst of X-rays is released.
Previous observations of other neutron stars have shown that the X-rays emitted during bursts display
oscillations that correspond to the rotation rate of the neutron stars. So the team began analysing the
XTE J1739-285 bursts for oscillations. What they found was astounding. In the brightest burst, which RXTE
recorded on 4 November, there were indeed oscillations but they were nearly twice as fast as any previously
observed.
"It was quite a surprise to us," admits Kuulkers. However, after running a series of checks, the team
satisfied themselves that the oscillations were indeed taking place 1122 times a second (1122 Hz).
Previously, the fastest neutron stars were known to spin with frequencies between 270-619 Hz.
This had led some astronomers to estimate, using statistical arguments, that the fastest a neutron star
could spin was 760 Hz. If the new observations are confirmed, XTE J1739-285 smashes this limit.
"Our detection is just above the level where we think there is something real. We definitely need more
observations. If we see the signal again, then everyone will believe it," says Kuulkers.
This doesn't mean that neutron stars can spin as fast as they like.
If the spin is too fast, even the crushing gravity of the star will be unable to hold matter to the surface
and the star will break up. The exact break-up speed depends on the internal conditions of a neutron star
and as yet, astronomers do not know these precisely.
"Our putative 1122 Hz detection places a serious constraint on neutron star models.
If we can find more stars that spin in this range, it will certainly allow us to exclude some models of their
interior structure," says Kuulkers.
So, now it is just a matter of patience. The astronomers will keep watch, not only for XTE J1739-285 to
burst again, but also for other fast-spinning X-ray neutron stars.
| — |
 |
Authors: C. M. Zhang, H.X. Yin, Y.H. Zhao, Y.C. Wei, X.D. Li |
 |
Journal-ref: PASP (2007) [0708.3566 ] |
 |
Title: Does Sub-millisecond Pulsar XTE J1739-285 Contain a Low Magnetic Neutron Star or Quark Star? |
Abstract:
With the possible detection of the fastest spinning nuclear-powered pulsar XTE
J1739-285 of frequency 1122 Hz (0.8913 ms), it arouses us to constrain the
mass and radius of its central compact object and to imply the stellar matter
compositions: neutrons or quarks.
Spun-up by the accreting materials to such a
high rotating speed, the compact star should have either a small radius or
short innermost stable circular orbit. By the empirical relation between the
upper kHz quasi-periodic oscillation frequency and star spin frequency, a
strong constraint on mass and radius is obtained as 1.51 solar masses and 10.9
km, which excludes most equations of states (EOSs) of normal neutrons and
strongly hints the star promisingly to be a strange quark star. Furthermore,
the star magnetic field is estimated to be about 4 × 107 G < B
< 108 G , which reconciles with those of millisecond radio pulsars,
revealing the clues of the evolution linkage of two types of astrophysical objects.
1. Introduction
The most rapidly spinning astrophysical object in the universe, named XTE J1739-285,
rotating 1122 times per second, has been declaimed to be detected recently in the accreting
X-ray binary system (Kaaret et al. 2007), which is the first sub-millisecond pulsar (spin
period 0.89 ms) coming into our view since the discovery of the first radio pulsar by Jocelyn
Bell and Anthony Hewish forty years ago (Hewish, Bell & Pilkingston et al. 1968) if the
1122 Hz is a spin frequency.
If the declared spin frequency 1122 Hz is fully confirmed, then
this compact object breaks through the record of the fastest radio pulsar with the spinning
frequency of 716 Hz (1.39 ms) discovered recently (Hessels et al. 2006).
References
Hessels, J. W. T., Ransom, S. M., Stairs, I. H., et al. 2006, Science, 311, 1901
Hewish, A., Bell, J., & Pilkington, J. D. et al.1968, Nature, 217, 709
Kaaret, P., Prieskorn, Z., & in’t Zand, J., et al. 2007, ApJ, 657, L97
|
|
— |
 |
Authors: Bejger, M.; Haensel, P.; Zdunik, J.L. |
 |
Journal-ref: A&A (2008) [astro-ph/0612216 ] |
 |
Title: Rotation at 1122 Hz and the neutron star structure |
Abstract:
• Aims.
Recent observations of XTE J1739-285 suggest that it contains a neutron star rotating at 1122 Hz. Such rotation
imposes bounds on the structure of neutron star in XTE J1739-285. These bounds may be used to constrain poorly
known equation of state of dense matter at densities > 1015 g cm-3.
• Methods.
One-parameter families of stationary configurations rotating rigidly at 1122 Hz are constructed, using a
precise 2-D code solving Einstein equations. Hydrostatic equilibrium solutions are tested for stability with
respect to axi-symmetric perturbations. A set of ten diverse EOSs of neutron stars is considered. Hypothetical
strange stars are also studied.
• Results.
For each EOS, the family of possible neutron star models is limited by the mass shedding limit, corresponding
to maximum allowed equatorial radius, Rmax, and by the instability with respect to the axi-symmetric
perturbations, reached at the minimum allowed equatorial radius, Rmin.
We get Rmin ~ 10 − 13 km, and Rmax ~ 16 − 18 km, with
allowed mass 1.4−2.3 M .
Allowed stars with hyperonic or exotic-phase core are supramassive and have a very narrow
mass range. Quark star with accreted crust might be allowed, provided such a model is able to
reproduce X-ray bursts from XTE J1739-285.
1. Introduction
Because of their strong gravity, neutron stars can be very rapid rotators; theoretical studies indicate that
they could rotate at submillisecond periods, i.e., at frequency nmax =
1/period > 1000 Hz (e.g., Cook et al. 1994a, Salgado et al. 1994).
References
Cook G. B., Shapiro S.L., Teukolsky S.A. 1994a ApJ, 424, 823
Cook G. B., Shapiro S.L., Teukolsky S.A. 1994b ApJ, 423, L117
Salgado M., Bonazzola S., Gourgoulhon E., Haensel P., 1994, A&A 108, 455
|
K3.3 XTE J1739-302
|
XTE J1739-302 — fast X-ray transient |
 |
Authors: D.M. Smith, W.A. Heindl, C.B. Markwardt, J.H. Swank, I. Negueruela, T.E. Harrison, L. Huss |
 |
Journal-ref: ApJ 638 (2006) 974-981 [astro-ph/0510658 ] |
 |
Title: XTE J1739-302 as a supergiant fast X-ray transient |
Abstract:
XTE J1739-302 is a transient X-ray source with unusually short outbursts,
lasting on the order of hours.
Here we give a summary of X-ray observations we
have made of this object in outburst with the Rossi X-ray Timing Explorer
(RXTE) and at a low level of activity with the Chandra X-ray Observatory, as
well as observations made by other groups. Visible and infrared spectroscopy of
the mass donor of XTE J1739-302 are presented in a companion paper.
The X-ray spectrum is hard both at low levels and in outburst, but somewhat variable, and
there is strong variability in the absorption column from one outburst to
another. Although no pulsation has been observed, the outburst data from
multiple observatories show a characteristic timescale for variability on the order of 1500-2000 s.
The Chandra localization (right ascension 17h 39m 11.58s,
declination -30o 20' 37.6'', J2000) shows that despite being located less than
2 degrees from the Galactic Center and highly absorbed, XTE J1739-302 is
actually a foreground object with a bright optical counterpart. The combination
of a very short outburst timescale and a supergiant companion is shared with
several other recently-discovered systems, forming a class we designate as
Supergiant Fast X-ray Transients (SFXTs). Three persistently bright X-ray
binaries with similar supergiant companions have also produced extremely short,
bright outbursts: Cyg X-1, Vela X-1, and 1E 1145.1-6141.
INTRODUCTION
|
|
XTE J1739-302 — d ~ 2.3 kpc — O8 Iab(f) |
 |
Authors: Negueruela, Ignacio; Smith, David M.; Harrison, Thomas E.; Torrejón, José Miguel |
 |
Journal-ref: ApJ 638 (2006) 982 [astro-ph/0510675 ] |
 |
Title: The Optical Counterpart to the Peculiar X-Ray Transient XTE J1739-302 |
Abstract:
The weak X-ray transient XTE J1739-302, characterized by extremely short outbursts, has recently been
identified with a reddened star. Here we present spectroscopy and photometry of the counterpart, identifying it
as a O8 Iab(f) supergiant at a distance of ~2.3 kpc.
XTE J1739-302 thus becomes the prototype of the new class of supergiant fast X-ray transients (SFXTs).
The optical and infrared spectra of the counterpart to XTE J1739-302 do not reveal any obvious
characteristics setting it apart from other X-ray binaries with supergiant companions, which
display a very different type of X-ray light curve.
1. Introduction
The X-ray transient XTE J1739−302 = AX J1739.1−3020 = IGR J17391−3021 is highly unusual because of its
extremely short outbursts. The only outburst that was monitored over its full extent was found to last less
than one day.
A pointed Chandra observation led to the unambiguous identification of the optical counterpart to
XTE J1739−302. As discussed in Paper I, the interest of XTE J1739−302 stems from the fact that there seems
to be a large number of similar objects, characterized by supergiant donors, low quiescence X-ray
luminosities and short (< 1d) outbursts, which we term Supergiant Fast X-ray Transients (SFXTs).
4. Discussion
Until recently, it was widely believed that High-Mass X-ray Binaries (HMXBs) with supergiant
donors were always persistent X-ray sources, while Be/X-ray binaries were mostly transients, though
some of them were persistent low-luminosity X-ray sources. Supergiant HMXBs are believed to be powered by
direct accretion from the strong radiative wind of the supergiant. They display typical X-ray luminosities
in the LX ~ 1035-36 erg s-1 range, which are relatively constant
over the long run, though presenting strong short-term stochastic variability.
The behavior of XTE J1739−302 differs from this pattern in two important respects. On the
one hand, its quiescent X-ray luminosity is rather lower than this
(LX < 1034 erg s-1) and the lightcurve
shows abrupt “outbursts” lasting only several hours.
A third interesting property of XTE J1739−302 is the fact that the absorption column density derived
from the fits to X-ray spectra is not only larger than the expected interstellar absorption,
but also highly variable
(NH = (4 - 38)× 1022 cm-2).
|
K3.4
Long-term monitoring of XTE J1739-302
|
XTE J1739-302 — Porb ~ 8 d |
 |
Authors: P. Blay, S. Martínez-Núñez, I. Negueruela, K. Pottschmidt,
D.M. Smith, J.M. Torrejón, P. Reig, P. Kretschmar, I. Kreykenbohm |
 |
Journal-ref: (2008) [0806.4097 ] |
 |
Title: INTEGRAL long-term monitoring of the Supergiant Fast X-ray Transient XTE J1739-302 |
Abstract:
• Context.
In the past few years, a new class of High Mass X-Ray Binaries (HMXRB) has been claimed to exist, the
Supergiant Fast X-ray Transients (SFXT). These are X-ray binary systems with a compact companion orbiting a
supergiant star which show very short and bright outbursts in a series of activity periods overimposed on
longer quiescent periods. Only very recently the first attempts to model the behaviour of these sources have
been published, some of them within the framework of accretion from clumpy stellar winds.
• Aims.
Our goal is to analyze the properties of XTE J1739-302/IGR J17391-3021 within the context of the clumpy
structure of the supergiant wind.
• Methods.
We have used INTEGRAL and RXTE/PCA observations in order to obtain broad band (1 – 200 keV) spectra and light
curves of XTE J1739-302 and investigate its X-ray spectrum and temporal variability.
• Results.
We have found that XTE J1739-302 follows a much more complex behaviour than expected. Far from presenting a
regular variability pattern, XTE J1739-302 shows periods of high, intermediate, and low flaring activity.
1. Introduction
Wind-fed Supergiant X-Ray Binaries (SGXRBs) display high energy emission arising from the accretion of material
in the wind of an OB supergiant onto the compact component of the system (a neutron star -NS- or black hole in
orbit around the supergiant). SGXRBs are persistent X-ray sources, displaying an X-ray luminosity
LX ~ 1036 erg s-1. Because of the physical
characteristics of wind accretion, their emission is variable on short timescales, with frequent flares, but
relatively stable on the long term (for example, the long-term RXTE/ASM lightcurve of Vela X-1, averaged and
smoothed with a running window of 30 d length, shows variations by only a factor of ~ 4; Ribo et al. 2006).
If the orbit is eccentric, the luminosity is modulated on the orbital period of the system
(e.g., Leahy 2002). Stronger short flares, with a fast rise and a typical timescale of the order
of a few hours, have been observed from several systems,
such as Vela X-1 (Laurent et al. 1995; Krivonos et al. 2003) or 4U 1907+09 (Fritz et al. 2006).
Recently, thanks to the improved sensitivity of high energy
missions, many new SGXRBs have been discovered, leading
to the suggestion of new classes of X-ray sources. On the one
hand, there is a number of highly absorbed SGXRBs, invisible
to previous missions due to high absorption in the softer
X-ray bands (e.g., Chaty & Filliatre 2005). On the other hand,
Supergiant Fast X-ray Transients (SFXTs) display fast outbursts,
with a typical duration of a few hours, but stay in quiescence
most of the time (Smith et al. 2006; Negueruela et al.
2006a; Sguera et al. 2006). Unlike in classical SGXRBs, the Xray
luminosity of SFXTs goes down below the sensitivity limit
of the INTErnational Gamma-Ray Astrophysics Laboratory
(INTEGRAL) and they remain undetectable for long time spans.
They can only be observed during an outburst or flare, for a short
time. Though several models have been proposed for this difference
in behaviours, it seems to be a natural consequence of the
clumpy nature of OB star winds (Walter & Zurita Heras 2007;
Negueruela et al. 2008). Sidoli et al. (2007) propose an alternative
hypothesis, based on observations of IGR J11215−5952, in
which the observed flaring activity is due to the interaction of
the compact object with an extended equatorial decretion disc
around the supergiant star.
Although the definition of SFXTs as a putative new class
of objects was only possible when the optical counterparts to
these systems started to be identified, INTEGRAL has contributed
decisively to the characterization of the high energy
behaviour of these sources. So far, ~ 12 SFXTs or related objects
have been detected by INTEGRAL (Walter & Zurita Heras
2007; Sguera et al. 2006). Among them, the best characterized
system is XTE J1739-302 = IGR J17391-3021, generally taken
as the prototype of the class (Smith et al. 2006; Negueruela et al. 2006b).
XTE J1739-302 was discovered by RXTE during a short outburst
in 1997 (Smith et al. 1998), when it was detected only
for a period of a few hours.
The optical counterpartwas identified thanks to a Chandra localization as an O8 Iab(f) supergiant at a
distance of ≈ 2.3 kpc (Negueruela et al. 2006b).
References
Negueruela, I., Smith, D.M., Reig, P., et al. 2006a, ESA SP-604, 165
Negueruela, I., Smith, D.M., Harrison, T.E., & Torrejon, J.M. 2006b, ApJ 638, 982
Negueruela, I., Torrejon, J.M., Reig, P. et al. 2008,
Sguera, V., Bazzano, A., Bird, A. J., et al. 2006, ApJ 646, 452
Sidoli, L., Romano, P., et al. 2007, A&A 476, 1307
Sidoli, L., Romano, P., Mangano, V., et al. 2008,
Smith, D. M., Main, D., Marshall, F., et al. 1998, ApJ 501, L181
Smith, D. M., Heindl, W.A., Markwardt, C.A., et al. 2006, ApJ 638, 974
Walter, R., & Zurita Heras, J.A. 2007, A&A 476, 335
|
K4 A0538-66: a Be/X-ray transient in LMC
|
A0538-66 in quiescence — LX ~ 6 × 1033 erg s-1 |
 |
Authors: P. Kretschmar, J. Wilms, R. Staubert, I. Kreykenbohm, W. A. Heindl |
 |
ref: 5th INTEGRAL Workshop (2004) [astro-ph/0406015 ] |
 |
Title: XMM-Newton Observations of the Be/X-ray transient A0538-66 in quiescence |
Abstract:
We present XMM-Newton observations of the recurrent Be/X-ray transient
A0538-66, situated in the Large Magellanic Cloud, in the quiescent state.
Despite a very low luminosity state of
LX = (5 — 8) × 1033 erg s-1
in the range 0.3 — 10 keV,
the source is clearly detected up to ~8 keV. and can be fitted using either a
power law with photon index alpha=1.9 or a bremsstrahlung spectrum with
kT=3.9 keV. The spectral analysis confirms that the off-state spectrum
is hard without requiring any soft component, contrary to the majority of
neutron stars observed in quiescence up to now.
INTRODUCTION
The recurrent Be/X-ray transient A0538–66 (X0535−668) was discovered in 1977 when two outbursts were observed
with the Ariel 5 satellite (White & Carpenter 1978). In the following years several other outbursts were observed
with HEAO 1 and Einstein with coincident X-ray and optical flares showing a recurrence of 16.65 days
(Skinner 1980) interpreted as the period of an eccentric binary orbit.
This period has been confirmed as a by-product of the MACHO project by Alcock et al. (2001), who also found
a longer optical modulation of 421 days. The optical counterpart, identified by Johnston et al. (1980), was
found to be a member of the Large Magellanic Cloud (LMC) (Pakull & Parmar 1981). Optical and UV spectroscopy
(Charles et al. 1983) classify the counterpart as B2 IIIe star.
Based on the distance to the LMC, the luminosity of the outbursts observed in the first years after detection
can be estimated as around 1039 ergs/s making this a super-Eddington source and one of the most
powerful X-ray binaries known.
An observation with Einstein (HEAO 2) 1980/81 during a strong outburst found 69ms pulsations
(Skinner et al. 1982; Ponman et al. 1984); up to this day this remains the only measure of the pulse period of
this accreting pulsar.
From the rapid spin period and the luminosity
Skinner et al. (1982) inferred an upper limit to the magnetic field of
B ~ 1011 G assuming that matter accreted
onto the polar caps uninhibited by a centrifugal barrier.
In later years the source has been mostly quiescent. Weak outburst activity at two to three orders of
magnitude below the early observations was found in the ROSAT All-Sky Survey in 1990
(Mavromatakis & Haberl 1993) and in an ASCA observation in 1995 (Corbet et al. 1997);
Alcock C., Allsman R.A., Alves D.R., et al. 2001, MNRAS, 321, 678
Charles P.A., Booth L., Densham R.H., et al. 1983, MNRAS, 202, 657
Corbet R.H.D., Charles P.A., Southwell K.A., Smale A.P. 1997, ApJ, 476, 833
Johnston M.D., Griffiths R.E., Ward M.J. 1980, Nature, 285, 26
Mavromatakis F., Haberl F. 1993, A&A, 274, 304
Ponman T.J., SkinnerG.K., Bedford D.K. 1984, MNRAS, 207, 621
Skinner G.K. 1980, Nature, 288, 141
Skinner G.K., Bedford D.K., Elsner R.F., et al. 1982, Nature, 297, 568
White N.E., Carpenter G.F. 1978, MNRAS, 183, 11P
|
K5 A 0535+26 — A Be/Xray binary pulsar
|
A 0535+26 — d = 2 kpc — a major X-ray outburst in May/June 2005 — optical and IR flux |
 |
Authors: M.J. Coe, P. Reig, V.A. McBride, J.L. Galache, J. Fabregat |
 |
Journal-ref: MNRAS 368 (2006) 447-453 [astro-ph/0602115 ] |
 |
Title: A 0535+26: Back in business |
Image credit:
Figure 8. Estimate of the radius of the Ha emitting region of the
circumstellar disk compared to the neutron star orbit (solid black
line). The three sizes of disk shown correspond to the following
radii values :
(a) 4.8×1012 cm, (b) 6.8×1012 cm and (c) 10.7×1012 cm.
The dashed circles are 4 truncation radii: from inside out they are
7:1, 5:1, 4:1 and 3:1.
|
Abstract:
In May/June 2005, after 10 years of inactivity, the Be/X-ray binary system A 0535+26 underwent a major X-ray
outburst. In this paper data are presented from 10 years of optical, IR and X-ray monitoring showing the
behaviour of the system during the quiescent epoch and the lead up to the new outburst. The
results show the system going through a period when the Be star in the system
had a minimal circumstellar disk and then a dramatic disk recovery leading,
presumably, to the latest flare up of X-ray emission. The data are interpreted
in terms of the state of the disk and its interaction with the neutron star companion.
INTRODUCTION AND BACKGROUND
The Be/X-ray systems represent the largest sub-class of massive X-ray binaries. A survey of the literature reveals
that of the 115 identified massive X-ray binary pulsar systems (identified here means exhibiting a coherent X-ray
pulse period), most of the systems fall within this Be counterpart class of binary. The orbit of the Be star and
the compact object, presumably a neutron star, is generally wide and eccentric. X-ray outbursts are normally
associated with the passage of the neutron star close to the circumstellar disk.
A 0535+26 was discovered by Ariel V during a Type II outburst in 1975. The primary is an O9.7IIIe star
and its optical and infrared (IR) emission has been the subject of many papers in an attempt to decode the
behavioural patterns of this system.
Throughout the last decade (1995-2004) there have been no reported detections of the source at X-ray
wavelengths. However, in May/June 2005 the source was detected undergoing significant X-ray activity by the
SWIFT and RHESSI observatories.
In this paper we report on the recent developments in the optical and IR fluxes in the context of the
re-emergence of A 0535+26 as an active X-ray source.
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A 0535+26 — giant outburst in 1994 — LX = 1038 erg s-1 |
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Authors: M. Maisack, J.E. Grove, E. Kendziorra, P. Kretschmar, R. Staubert, M.S. Strickman |
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Journal-ref: A&A 325 (1997) 212 [astro-ph/9703135 ] |
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Title: Pulse Phase Spectroscopy of A 0535+26 during its 1994 giant outburst observed with OSSE |
Abstract:
We present pulse phase spectroscopy of A 0535+26 in the energy range 35-200
keV from OSSE observations of its giant outburst in 1994.
We discuss the phase dependence of the continuum parameters and the cyclotron resonance feature
(CRF) at 110 keV already found in the phase averaged spectrum. We find that a
CRF is required at every phase. The behaviour of the line parameters with phase
and the pulse shape indicate that the emission occurs in a pencil-beam geometry.
INTRODUCTION
In Be X-ray binaries (BeXRB) with a neutron star as the compact object, mass transfer is mediated via a
circumstellar disk around the companion. The companions are O or B stars with high rotational velocities which
are responsible for the loss of material in the equatorial plane.
The material in this disk, which may be present or absent for extended periods, flows out rather slowly
(velocities of several tens of km/s) compared to the fast B star wind outside the equatorial plane. In fact, the
dynamics of the material in this circumstellar disk may be dominated by Keplerian motion.
Be-XRB undergo dramatic increases in X-ray flux when the neutron star passes through the dense regions of the
circumstellar disk near periastron passage and enhanced mass accretion sets in. Outbursts with luminosities in
excess of LX = 1038 erg s-1
can be observed in these systems at these times, while the X-ray luminosity during quiescence
is LX = 1033 erg s-1 and below.
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Literatur zu
"Gamma-Ray Giant Flares / X-ray Transients"
"SGR 1806-20"
(I)
(II)
(III)
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| Schwartz, S., Silvia Zane, Robert J. Wilson, et al. | 2005 | ApJ 627, L129-L132 |
"The Gamma-Ray Giant Flare from SGR 1806-20: Evidence of Crustal Cracking via Initial Timescales"
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| Hurley, K. , S.E. Boggs, D. M. Smith et al. | 2005 | Nature 434, 1098-1103 |
"An exceptionally bright flare from SGR 1806–20 and the origins of short-duration γ-ray bursts"
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| Israel, G. L., T. Belloni, L. Stella, et al. | 2005 | ApJ 628, L53–L56 |
"Discovery of rapid X-ray oscillations in the tail of the SGR 1806-20 hyperflare "
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D.M. Smith, W.A. Heindl, C.B. Markwardt, J.H. Swank, I. Negueruela, T.E. Harrison,
L. Huss | 2006 | ApJ 638, 974-981 |
"XTE J1739-302 as a supergiant fast X-ray transient"
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| Negueruela, I.; Smith, D.M.; Harrison, T.E.; Torrejón, J.M. | 2006 | ApJ 638, 982 |
"The Optical Counterpart to the Peculiar X-Ray Transient XTE J1739-302"
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| M.J. Coe, P. Reig, V.A. McBride, J. L. Galache, J. Fabregat | 2006 | MNRAS 368, 447-453 |
"A 0535+26: Back in business"
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| P. Kaaret, Z. Prieskorn, J.J.M. in 't Zand, et al. | 2007 | ApJ 657, L97 |
"Discovery of 1122 Hz X-Ray Burst Oscillations from the Neutron-Star X-Ray Transient XTE J1739-285"
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| Negueruela, I., Smith, D.M., Reig, P., et al. | 2007 | ESASP 604, 165 |
"SFXTs: A new class of high mass X-ray binaries unveiled by INTEGRAL"
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 | H. Heintzmann | ( Eintrag vom 15.8.2008) |
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