On Some Prospects of the LOFT Mission: QPO Models Institute of Physics, Silesian University in Opava Gabriel Török CZ.1.07/2.3.00/20.0071 Synergy, GAČR.

Slides:



Advertisements
Similar presentations
Observing Orbital Motion in Strongly Curved Spacetime Institute of Physics, Silesian University in Opava Gabriel Török CZ.1.07/2.3.00/ Synergy,
Advertisements

Gabriel Török 3:2 ratio in NS X-ray observations: summary of recent progress The presentation draws mainly from the collaboration with M.A. Abramowicz,
Energy spectra of X-ray quasi- periodic oscillations in accreting black hole binaries Piotr Życki & Małgorzata Sobolewska § Nicolaus Copernicus Astronomical.
Neutron Stars and Black Holes Please press “1” to test your transmitter.
Accretion in Binaries Two paths for accretion –Roche-lobe overflow –Wind-fed accretion Classes of X-ray binaries –Low-mass (BH and NS) –High-mass (BH and.
Mass transfer in a binary system
Faculty of Science Department of Physics Field Line Resonances in the Earth’s Magnetosphere and Astrophysical Plasmas 1 J. C. Samson
Ron Remillard, MIT Primary Collaborator, Jeff McClintock CfA
Pavel Bakala Eva Šrámková, Gabriel Török and Zdeněk Stuchlík Institute of Physics, Faculty of Philosophy and Science, Silesian University in Opava, Bezručovo.
Gabriel Török* 3:2 controversy …hope for underlying QPO physics ? *Institute of Physics, Faculty of Philosophy and Science, Silesian University in Opava,
1 Astrophysical black holes Chris Reynolds Department of Astronomy.
Vznik této prezentace byl podpořen projektem CZ.1.07/2.3.00/ Tato prezentace slouží jako vzdělávací materiál.
Institute of Physics, Silesian University in Opava Gabriel Török GAČR 209/12/P740, CZ.1.07/2.3.00/ Synergy, GAČR G, SGS ,
A toy model for HFQPOs in XRBs Ye Yong-Chun ( 叶永春 ), Wang Ding-Xiong( 汪定雄 ) Department of Physics, Huazhong University of Science and Technology, Wuhan,
Lecture 4a. Blackbody Radiation Energy Spectrum of Blackbody Radiation - Rayleigh-Jeans Law - Rayleigh-Jeans Law - Wien’s Law - Wien’s Law - Stefan-Boltzmann.
In collaboration: D. Barret (CESR), M. Bursa & J. Horák (CAS), W. Kluzniak (CAMK), J. Miller (SISSA). We acknowledge the support of Czech grants MSM ,
Gabriel Török* Relating high-frequency QPOs and neutron-star EOS *Institute of Physics, Faculty of Philosophy and Science, Silesian University in Opava,
Vznik této prezentace byl podpořen projektem CZ.1.07/2.3.00/ Tato prezentace slouží jako vzdělávací materiál.
Reverberation effect in Quasi Periodic Oscillations in Black Hole Candidates. Nikolai Shaposhnikov 1,2,3 1 University of Maryland, Astronomy Department.
BLACK HOLES: FROM STARS TO GALAXIES – ACROSS THE RANGE OF MASSES Felix Mirabel European Southern Observatory. Chile (on leave from CEA. France) In last.
Scientific objectives for XEUS: Galaxies Groups and Clusters at z~2 Study of the Evolution of clusters in the mass range kT > 2 keV up to z=2. Dynamics,
Einstein’s elusive waves
Gravitational waves and neutrino emission from the merger of binary neutron stars Kenta Kiuchi Collaboration with Y. Sekiguchi, K. Kyutoku, M. Shibata.
Black Holes Escape velocity Event horizon Black hole parameters Falling into a black hole.
International Workshop on Astronomical X-Ray Optics Fingerprints of Superspinars in Astrophysical Phenomena Zdeněk Stuchlík and Jan Schee Institute of.
On some prospects of the LOFT mission Institute of Physics, Silesian University in Opava Astronomical Institute, Prague Gabriel Török, Pavel Bakala, Vladimír.
Timing and Spectral Properties of Neutron Star Low-Mass X-ray Binaries Sudip Bhattacharyya Department of Astronomy and Astrophysics Tata Institute of Fundamental.
Some Comments on Results Achieved within the Students Project SGS 01/2010 and CZ.1.07/2.2.00/ (Bachelors and Masters Theses 2011) Institute of Physics,
KERR SUPERSPINARS AS AN ALTERNATIVE TO BLACK HOLES Zdeněk Stuchlík Institute of Physics, Faculty of Philosophy and Science, Silesian university in Opava.
A physical interpretation of variability in X-ray binaries Adam Ingram Chris Done P Chris Fragile Durham University.
Discovery of powerful millisecond flares from Cyg X-1 Marek Gierliński University of Durham, England Andrzej Zdziarski N. Copernicus Astronomical Center,
Ramesh Narayan (McClintock, Shafee, Remillard, Davis, Li)
MEASUREMENT OF BRANY BLACK HOLE PARAMETERS IN THE FRAMEWORK OF THE ORBITAL RESONANCE MODEL OF QPOs MEASUREMENT OF BRANY BLACK HOLE PARAMETERS IN THE FRAMEWORK.
Death of Stars III Physics 113 Goderya Chapter(s): 14 Learning Outcomes:
Observing Orbital Motion in Strongly Curved Spacetime Institute of Physics, Silesian University in Opava Gabriel Török CZ.1.07/2.3.00/ Synergy,
Black Hole Accretion Theoretical Limits And Observational Implications Dominikus Heinzeller Institute for Theoretical Astrophysics Center for Astronomy.
A Toy Model for 3:2 HFQPO Pairs in Black Hole Binaries XTE J and GRO J Ding-Xiong WANG( 汪定雄 ), Zhao-Ming GAN (speaker, 甘朝明 ), Chang-Yin.
Pavel Bakala Martin, Urbanec, Eva Šrámková, Gabriel Török and Zdeněk Stuchlík Institute of Physics, Faculty of Philosophy and Science, Silesian University.
Pavel Bakala Eva Šrámková, Gabriel Török and Zdeněk Stuchlík Institute of Physics, Faculty of Philosophy and Science, Silesian University in Opava, Bezručovo.
Page 1 HEND science after 9 years in space. page 2 HEND/2001 Mars Odyssey HEND ( High Energy Neutron Detector ) was developed in Space Research Institute.
Zdeněk Stuchlík Gabriel Török, Petr Slaný, Andrea Kotrlová, Jiří Kovář Multi-resonant models of quasi-periodic oscillations in black hole and neutron star.
Timing Features of XTE J in 2003 March outburst Fan Zhang et al. (astro-ph/ ) --Possible Evidence for Accreting Blobs.
Pavel Bakala Gabriel Török, Zdeněk Stuchlík, Eva Šrámková Institute of Physics Faculty of Philosophy and Science Silesian University in Opava Czech Republic.
Pavel Bakala,Gabriel Török, Zdeněk Stuchlík and Eva Šrámková Institute of Physics, Faculty of Philosophy and Science, Silesian University in Opava, Bezručovo.
Black holes and accretion flows Chris Done University of Durham.
Gabriel Török, P.Bakala, E. Šrámková, Z. Stuchlík, M. Urbanec Mass and spin of NS implied by models of kHz QPOs *Institute of Physics, Faculty of Philosophy.
Figs on this page: nasa.gov. Outline 1. Introduction: Quasi-periodic oscillations (QPOs) - Black-hole and neutron star binaries, accretion disks and QPOs.
Abbas Askar University of Belgrade 12 th November 2011 Astronomy Workshop Presentation Belgrade, Serbia.
Gabriel Török* On orbital models of kHz QPOs in neutron star binaries *Institute of Physics, Faculty of Philosophy and Science, Silesian University in.
Paczyński Modulation: Diagnostics of the Neutron Star EOS? Institute of Physics, Silesian University in Opava Gabriel Török, Martin Urbanec, Karel Adámek,
Measuring the SPIN of Black Holes
MIT Workshop on QPOs Oscillation Modes of the Inner Torus in MHD Simulations of Black-Hole Accretion Disks Collaborators: Omer Blaes (UCSB), Phil.
Transient response of the ionosphere to X-ray solar flares Jaroslav Chum (1), Jaroslav Urbář (1), Jann-Yenq Liu (2) (1) Institute of Atmospheric Physics,
Gabriel Török* On orbital models of kHz QPOs *Institute of Physics, Faculty of Philosophy and Science, Silesian University in Opava, Bezručovo nám. 13,
Institute of Physics, Silesian University in Opava Gabriel Török GAČR 209/12/P740, CZ.1.07/2.3.00/ Synergy, GAČR G, SGS ,
Global Simulations of Time Variabilities in Magnetized Accretion Disks Ryoji Matsumoto (Chiba Univ.) Mami Machida (NAOJ)
Exploring an evidence of supermassive black hole binaries in AGN with MAXI Naoki Isobe (RIKEN, ) and the MAXI
Gabriel Török* 3:2 controversy …hope for underlying QPO physics ? *Institute of Physics, Faculty of Philosophy and Science, Silesian University in Opava,
STRONG RESONANT PHENOMENA IN BLACK HOLE SYSTEMS Institute of Physics, Faculty of Philosophy and Science, Silesian University in Opava, Bezručovo nám. 13,
Genetic Selection of Neutron Star Structure Matching the X-Ray Observations Speaker: Petr Cermak The Institute of Computer Science Silesian University.
Global MHD Simulations of State Transitions and QPOs in Black Hole Accretion Flows Machida Mami (NAOJ) Matsumoto Ryoji (Chiba Univ.)
Reverberation mapping with eXTP
Soichiro Isoyama Collaborators : Norichika Sago, Ryuichi Fujita, and Takahiro Tanaka The gravitational wave from an EMRI binary Influence of the beyond.
Why is the BAT survey for AGN Important? All previous AGN surveys were biased- –Most AGN are ‘obscured’ in the UV/optical –IR properties show wide scatter.
Overview on XTP sciences Zhang Shu (on behalf of the XTP science team) Institute of High Energy Physics.
Gravitational Waves What are they? How can they be detected?
Zdeněk Stuchlík, Gabriel Török, Petr Slaný Multi-resonant models of quasi-periodic oscillations Institute of Physics, Faculty of Philosophy and Science,
The X-ray Universe Granada
Evidence for an Intermediate Mass Black Hole in NGC 5408 X-1
General Relativity in X-ray Astronomy Astrosat and Future Experiments
Presentation transcript:

On Some Prospects of the LOFT Mission: QPO Models Institute of Physics, Silesian University in Opava Gabriel Török CZ.1.07/2.3.00/ Synergy, GAČR 209/12/P740, 202/09/0772, SGS ,

density comparable to the Sun mass in units of solar masses temperature ~ roughly as the T Sun more or less optical wavelengths MOTIVATION Companion: Compact object: - black hole or neutron star (>10^10gcm^3) >90% of radiation in X-ray LMXB Accretion disc Observations: The X-ray radiation is absorbed by the Earth atmosphere and must be studied using detectors on orbiting satellites representing a rather expensive research tool. On the other hand, it provides a unique chance to probe effects in the strong-gravity-field region (GM/r~c^2) and test extremal implications of General Relativity (or other theories). T ~ 10^6K Figs: space-art, nasa.gov 1. Introduction LMXBs

Fig: nasa.gov LMXBs short-term X-ray variability: peaked noise (Quasi-Periodic Oscillations ) Low frequency QPOs (up to 100Hz) hecto-hertz QPOs ( Hz),... HF QPOs (~ Hz): Lower and upper QPO feature forming twin peak QPOs frequency power Sco X-1 The HF QPO origin remains questionable, it is most often expected that it is associated to orbital motion in the inner part of the accretion disc. Individual peaks can be related to a set of oscillators, as well as to time evolution of a single oscillator. 1. Introduction MOTIVATION

2. LOFT LOFT is specifically designed to exploit the diagnostics of very rapid X-ray flux and spectral variability (already known to exist) that directly probe the motion of matter down to distances very close to black holes and neutron stars. Its factor of ~20 larger effective area than RXTE’s PCA (the largest area X-ray instrument ever flown) is crucial in this respect. (from LOFT webpage)

2. LOFT LOFT/LAD’s much improved energy resolution (better than 260 eV) compared to that of RXTE/PCA will also allow the simultaneous exploitation of spectral diagnostics, in particular the relativistically broadened 6-7 keV Fe-K lines. The timescales that LOFT will investigate range from submillisecond quasi-periodic oscillations (QPOs) to years long transient outbursts. LOFT is required to answer two fundamental questions of ESA's Cosmic Vision Theme Matter under extreme conditions: Does matter orbiting close to the event horizon follow the predictions of general relativity? What is the equation of state of matter in neutron stars? (from LOFT webpage)

3. LOFT & QPO Models (SFG1 Group Goals) (Several of) Competing models variously identify observed QPOs with the relativistic radial and vertical epicyclic frequencies or relativistic nodal and periastron precession. Very high-signal-to-noise LOFT/LAD measurements of the QPOs will unambiguously discriminate between such interpretations and in the process tease out yet untested general relativistic effects such as frame dragging, strong-field periastron precession, and the presence of an innermost stable orbit. Crucially, LOFT will provide access for the first time to types of information in these signals that are qualitatively new due to the capability to measure dynamical timescale phenomena within their coherence time, where so far only statistical averages of signals were accessible. This will allow studies that directly witness QPO formation and propagation and tie in with what state-of- the-art numerical work is just beginning to address. (from LOFT webpage)

Very high-signal-to-noise LOFT measurements of the QPOs will unambiguously discriminate between QPO interpretations. “ Models predict frequencies but give very little insights on amplitude - It is however likely that we see the tip of the iceberg (the fundamental, which is actually close to the PCA sensitivity) and that the clue is in the harmonic content of the signal, and this is a problem, because we don't know at which amplitude levels they will show up.” (from SFG1 materials) 3. LOFT & QPO Models (SFG1 Group Goals)

Very high-signal-to-noise LOFT measurements of the QPOs will unambiguously discriminate between QPO interpretations. Lightcurves corresponding to different disc oscillation modes and lightcurves corresponding to hot-spot models should be modelled including both the current models and the process of observation in order to obtain relevant PDS. 3. LOFT & QPO Models (SFG1 Group Goals)

4. Lightcurve Modelling: Implementation Basis & “Reverse Engineering” COLLABORATION: Pavel Bakala, Vladimír Karas, Michal Dovčiak, Martin Wildner, Dalibor Wzientek, Marek Abramowicz, Eva Šrámková, Kateřina Goluchová, Frederic Vincent, Grzegorz Mazur  Institute of Physics, Silesian University in Opava, CZ  Astronomical Institute, Prague, CZ  Copernicus Astronomical Center, Warszawa, PL  Institute for Theoretical Physics, University of Warsaw,PL  Laboratoire AstroParticule et Cosmologie, CNRS, Universite Paris Diderot, FR

4. Lightcurve Modelling: Implementation Basis & “Reverse Engineering” Global Empirical Model of Variability and Spectra (GRS , SPL State) + QPO MODEL TOTAL SOURCE FLUX MODEL

4. Lightcurve Modelling: Implementation Basis & “Reverse Engineering” Global Empirical Model of Variability and Spectra (GRS , SPL State) + TOTAL SOURCE FLUX MODEL QPO MODEL

4. Lightcurve Modelling: Implementation Basis & “Reverse Engineering” Global Empirical Model of Variability and Spectra (GRS , SPL State) Response Matrices (Detector) “DATA” Time and Spectral Distribution of Detected Counts TIMING ANALYSIS RESULTS TOTAL SOURCE FLUX MODEL + QPO MODEL

5. Some Results: Signal Strength Model: Single spot orbiting close to inner edge of the accretion disc (simulation using KY Spot code). Expectation: Keplerian frequency + harmonics

5. Some Results: Signal Strength Signal Strength (relative hot-spot brigthness) Model: Single spot orbiting close to inner edge of the accretion disc (simulation using KY Spot code). [ ~ 1Crab source countrate] Expectation: Keplerian frequency + harmonics

5. Some Results: Signal Strength Signal Strength Model: Single spot orbiting close to inner edge of the accretion disc (simulation using KY Spot code). [ ~ 1Crab source countrate] Expectation: Keplerian frequency + harmonics

5. Some Results: Signal Strength Model: Single spot orbiting close to inner edge of the accretion disc (simulation using KY Spot code). [ ~ 1Crab source countrate] Expectation: Keplerian frequency + harmonics

5. Some Results: Signal Strength Model: Single spot orbiting close to inner edge of the accretion disc (simulation using KY Spot code). [ ~ 1Crab source countrate] Expectation: Keplerian frequency + harmonics

5. Some Results: Signal Strength Model: Single spot orbiting close to inner edge of the accretion disc (simulation using KY Spot code). [ ~ 1Crab source countrate] Expectation: Keplerian frequency + harmonics

5. Some Results: Signal Strength Current BH status: weak signal with sporadic RXTE QPO detections - The applied simple model clearly illustrates the LOFT capability in such situation.

5. Some Results: Comparison Between QPO Models Frequency Power RXTE simulationsLOFT simulations Torus (Epicyclic Modes) SPOTS (ISCO, nurmax) Multiple spost created around two preferred radii (using KY Spot code). The m=0 epicyclic oscillations of the optically thin torus drifting through the resonant radius. M = 11M ⊙, D = 65°, a = 0, R1= 6M, R2=8M, n=0.1. M = 5.6M ⊙, D = 65°, a = 0, R0= 10.8M, n=0.1. Power Torus (Epicyclic Modes) Frequency Power SPOTS (ISCO, nurmax)

Frequency Power RXTE simulationsLOFT simulations Torus (Epicyclic Modes) SPOTS (ISCO, nurmax) Multiple spost created around two preferred radii (using KY Spot code). The m=0 epicyclic oscillations of the optically thin torus drifting through the resonant radius. M = 11M ⊙, D = 65°, a = 0, R1= 6M, R2=8M, n=0.1. M = 5.6M ⊙, D = 65°, a = 0, R0= 10.8M, n=0.1. Frequency Power Torus (Epicyclic Modes) Power SPOTS (ISCO, nurmax) 5. Some Results: Comparison Between QPO Models

RXTE simulationsLOFT simulations Frequency Power Torus (Epicyclic Modes) SPOTS (ISCO, nurmax) Frequency Power Torus (Epicyclic Modes) Power SPOTS (ISCO, nurmax) 5. Some Results: Comparison Between QPO Models

RXTE simulationsLOFT simulations GR Power Frequency Torus (Epicyclic Modes) SPOTS (ISCO, nurmax) Frequency Power Torus (Epicyclic Modes) Power SPOTS (ISCO, nurmax) 5. Some Results: Comparison Between QPO Models

END Thank you for your attention…