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X-rays from Magnetic Cataclysmic Variables and ASTROSAT. K.P SinghTata Institute of Fundamental ResearchMumbai, India. Talk Outline. Introduction to CVs Types and classes of CVs Non-magnetic systems Magnetic systems: Polars and Intermediate Polars X-ray Light Curves of Polars and IPs - PowerPoint PPT Presentation
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X-rays from Magnetic Cataclysmic Variables and ASTROSAT
K.P Singh Tata Institute of Fundamental ResearchMumbai, India
2
Talk Outline
• Introduction to CVs
• Types and classes of CVs
• Non-magnetic systems
• Magnetic systems: Polars and Intermediate Polars
• X-ray Light Curves of Polars and IPs
• Wide-Band, Low-Resolution X-ray spectra
• ASTROSAT
• Conclusions
18 Feb 2012 HEAP12- HRI (KP Singh)
3
CVs: what are they?• Cataclysmic Variables are
– semi-detached binaries accreting
– from a red dwarf red dwarf main-sequence-like secondary star
– to a more massive white dwarf white dwarf primary star
• Binary: Roche potential: the gravitational potential around two orbiting point masses – resultant force on a test mass:
credit: csep10.phys.utk.edu
F tot = F M1(grav )+ F M
2(grav )+ FCoM ( centrifugal)
Centre of Mass
2
18 Feb 2012 HEAP12- HRI (KP Singh)
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Roche Lobe Overflow• Semi-detached secondary star fills its Roche
lobe so that it is distorted into a pear shape.
• At Lagrangian 1 (L1) point, gravitational and centrifugal forces cancel and material is lost from the secondary star into the primary Roche lobe.
• Material falls towards the white dwarf in a stream
• The 4 other stationary pointsL2 – L5 are important for orbit theory
2
credit: csep10.phys.utk.edu
credit: www.genesismission.org
18 Feb 2012 HEAP12- HRI (KP Singh)
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The CV Zoo: subtypes• Cataclysmic Variables (non-magnetic)
– Novae large eruptions 6–9 magnitudes
– Recurrent Novae previous novae seen to repeat
– Dwarf Novae regular outbursts 2–5 magnitudes
› SU UMa stars occasional Superoutbursts
› Z Cam stars show protracted standstills
› U Gem stars all other DN
– Nova-like variables
› VY Scl stars show occasional drops in brightness
› UX UMa stars all other non-eruptive variables
• Intermediate Polars/DQ Her stars
• Polars/AM Her stars
magnetic systems
18 Feb 2012 HEAP12- HRI (KP Singh)
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(1) Non-Magnetic CVs
• magnetic field on primary <106 G (100 T) non-magnetic CV
• accretion takes place through a disk
• via boundary layer on white dwarf
18 Feb 2012 HEAP12- HRI (KP Singh)
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(2) Magnetic CVs: Polars
• NO DISK: accretion takes place via a stream and accretion column directly onto white dwarf
• Largest circular polarization varying with the orbital period: magnetic field > 107 G (1000 T) polar/AM Her system
• the magnetic field controls the flow fromsome threading region
18 Feb 2012 HEAP12- HRI (KP Singh)
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Polars: Synchronisation
• All of the variability in Polars occurs at a single period: the orbital period
– radial velocity curves of the secondary
– X-ray light curves from the primary
– polarisation variations
the white dwarf/red dwarf are locked into the same orientation: synchronised rotation
• The mechanism for synchronisation is the dissipation due to the magnetic field of the primary being dragged through the secondary
• As relative spin rate of primary decreases, locking can occur due to the dipole-dipole magnetostatic interaction between primary and (weaker) secondary magnetic field
• Some Polars not quite in synchronism; in these systems it typically takes 5–50 days for white dwarf orientation to repeat itself
• Very useful systems to study the effect of orientation of magnetic field on the accretion process
18 Feb 2012 HEAP12- HRI (KP Singh)
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Polars: Radial Accretion
• Infalling material is forced to follow the magnetic field lines
• Gas is initially in free-fall but then it encounters a shock front
• Shock converts kinetic energy into thermal energy (bulk motion into random motion) temperature increases to ~50 keV
• Velocity drops by 1/4 and density increases by 4
• Material radiates by cyclotron and bremsstrahlung and gradually settles on white dwarf
hard X-rays
white dwarf
shock
cold
supersonic
flow
hot
postshock
flow
soft X-ra
ys/
extreme UV
optical/IR
cyclotron
radiation
18 Feb 2012 HEAP12- HRI (KP Singh)
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X-ray Spectrum
• Polars/AM Her stars were found to be strong soft X-ray emitters (~1033 erg/s) in early surveys
• X-ray emission characterized by thermalized free-fall velocities from a white dwarf so emission is from a hot region close to the white dwarf surface: post-shock
• Cyclotron emission must also be from a hot region (otherwise narrow cyclotron emission lines rather than continuum)
AM Her
Rothschild et al (1981)
18 Feb 2012 HEAP12- HRI (KP Singh)
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Polars: Spectral Energy Distribution
• Most of the energy from these systems is a result of accretion
• 3 main components:cyclotron radiation from accretion column
hard X-ray emission, also from accretion column
soft X-ray emission, from heated surface of primary
Beuermann (1998)18 Feb 2012
12
XMM-Newton Spectrum of V1432 Aql
Model Compenents:
•Black body emission (88±2 eV)•Absorbers:1.7±0.3 x 1021 cm-2, fully covering the source & 1.3 ±0.2 x 1023 cm-2, covering 65% •Multi-temperature plasma model•Gaussian for 6.4 keV line emission
Absorption due to ISM = 4.5 x 1020 cm-2 (fixed from ROSAT Obs; Staubert et al. 1994)
18 Feb 2012 HEAP12- HRI (KP Singh)
XMM: Rana, Singh et al. 2005, ApJ
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RXTE Spectrum of V1432 Aql
Model = Absorption (Multi-temperature Plasma + Gaussian)
• Bremsstrahlung model (temperature of >90 keV ; highest in Polars and IPs)• Mass of the WD related to the shock temperature • Mass of the WD in V1432 Aql is 1.2±0.1 solar mass.
18 Feb 2012 HEAP12- HRI (KP Singh)
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AM Her (Polar) Pspin (X-ray)=11139 sGirish, Rana & Singh 2007
Two-pole accretion based on opticalPolarizationInclination=52+-5 degrees
18 Feb 2012 HEAP12- HRI (KP Singh)
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UZ For (Eclipsing Polar): P=7591.8 s
• Two accretion regions evident
• Weak accretion stream
UZ For
STJ photometry: Perryman et al (2001)
Sky
18 Feb 2012 HEAP12- HRI (KP Singh)
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(3) Magnetic CVs: Intermediate Polars• magnetic field ~106 G intermediate polar/DQ Her system
• accretion takes place through a hollowed-out disk and then via accretion columns onto the white dwarf
• magnetic field controls the flow in the final stages
18 Feb 2012 HEAP12- HRI (KP Singh)
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Intermediate Polars: models• Intermediate Polars spin variability can be explained in
several ways
– visibility of the accretion region on the white dwarf
– visibility of the accretion “curtains”
– reprocessing of flux on the disk (optical/UV)
• From studies of the relative phasing in different wavelength bands and including the absorption effects now known to be a combination of the above models leading to the complex behavior in Intermediate Polar light curves
stream
Adapted from Hellier (2001)
18 Feb 2012 HEAP12- HRI (KP Singh)
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AO Psc (Intermediate Polar)
AO Psc
• AO Psc: Optical spectrum like that of Polars, but without any identifiable polarisation
• Variability on three different timescales now known to be
– the orbital 3.591 h,
– the spin period of the white dwarf 805.4 s
– the mixture of the two (beat/synodic period)
Cropper et al (2002)
18 Feb 2012 HEAP12- HRI (KP Singh)
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AO Psc (IP) Power Spectra
• By performing a Fourier Transform of the previous data, the main periodicities can be identified
– orbital period
– white dwarf spin
– beat (very faint in this system)
• Also evident are harmonics when the variations are non-sinusoidal (2, 3, 2)
Ginga:Norton et al.
18 Feb 2012 HEAP12- HRI (KP Singh)
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TV Col (Intermediate Polar) =1909.7s =5.5 h
Rana, Singh et al. 2004, AJ, 127, 489
First clear detection of Orbital modulation
18 Feb 2012 HEAP12- HRI (KP Singh)
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TV Col (IP): Spin and Orbital Phase LCs
Rana, Singh et al. 2004, AJ, 127, 489
Absorption Dips due to stream
18 Feb 2012 HEAP12- HRI (KP Singh)
INTEGRAL Discovered IP: IGR J17195-4100
18 Feb 2012 HEAP12- HRI (KP Singh)
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New spin period: 1053.9 sNew Binary Orbital period: 3.5 hoursGirish & Singh, MNRAS, 2012
Multi-temperature plasma, partial absorber and flourescence – sometimes a weak soft X-ray component. Accretion Curtain but perhaps no disc in this IP !Girish & Singh, MNRAS, 2012
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X-ray Spectrum: EX Hya (IP)• X-ray spectra of Intermediate Polars generally show
just the multi-temperature thermal bremsstrahlung component from the hot radial accretion flow – no soft reprocessed component from the white dwarf
• Main explanation is likely to be the larger area over which accretion takes place, but also photoelectric absorption is important
Fujimoto & Ishida 1997
18 Feb 2012 HEAP12- HRI (KP Singh)
ASTROSAT (1.55 tons; 650 kms, 8 deg inclination orbit by PSLV. 3 gyros and 2 star trackers for attitude control by reaction wheel system with a Magnetic torquer ) Launch: end of 2012
Soft X-ray Telescope
3 Large Area Xenon Proportional Counters
2 UV(+Opt ) Imaging Telescopes
CZTI
SSM (2 – 10 keV)
Folded Solar panels
Radiator PlatesFor SXT and CZT
Scanning Sky Monitor (SSM)
Feb 13, 2012K.P. Singh
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UVIT: Two Telescopes• f/12 RC Optics
• Focal Length: 4756mm
• Diameter: 38 cm
• Simultaneous Wide Angle ( ~ 28’) images in FUV (130-180 nm) in one and NUV (180-300 nm) & VIS (320-530 nm) in the other
• MCP based intensified CMOS detectors
• Spatial Resolution : 1.8”
• Sensitivity in FUV: mag. 20 in 1000 s
• Temporal Resolution ~ 30 ms, full frame ( < 5 ms, small window )
• Gratings for Slit-less spectroscopy in FUV & NUV
• R ~ 100
Energy Range : 3-80 keV ( 50 Mylar window, 2 atm. of 90 % Xenon + 10 % Methane )
Effective Area : 6000 cm² (@ 20 keV)
Energy Resolution : ~10% FWHM at 22 keV
Onboard purifier for the xenon gas
Field of View : 1° x 1° FWHM (Collimator : 50µ Sn + 25µ Cu + 100µ Al )Blocking shield on sides and bottom : 1mm Sn + 0.2 mm Cu
Timing Accuracy : 10 μsec in time tagged mode
(oven-controlled oscillator).
Large Area Xenon Proportional Counter (LAXPC): Characteristics
Feb 13, 2012 K.P. Singh
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LAXPC: Effective Area
CZT Imager characteristics
Area 1024 cm 2
Pixels 16384
Pixel size 2.4 mm X 2.4 mm (5 mm thick)
Read-out ASIC based (128 chips of 128 channels)
Imaging method Coded Aperture Mask (CAM)
Field of View 17 X 17 deg2 (uncollimated)6 X 6 (10 – 100 keV) – CAM
Angular resolution 8 arcmin
Energy resolution 5% @ 100 keV
Energy range 10 – 100 keV - Up to 1 MeV (Photometric)
Sensitivity 0.5 mCrab (5 sigma; 10 4 s)
Feb 13, 2012 K.P. Singh
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SXT Characteristics
Telescope Length: 2465 mm (Telescope + camera + baffle + door)Top Envelope Diameter: 386 mm Focal Length: 2000 mmEpoxy Replicated Gold Mirrors on Al substrates in conical Approximation to Wolter I geometry.Radius of mirrors: 65 - 130 mm; Reflector Length: 100 mmReflector thickness: 0.2 mm (Al) + Epoxy (~50 microns) + gold (1400 Angstroms)Reflector Smoothness: 8 – 10 AngstromsMinimum reflector spacing: 0.5 mmNo. of reflectors: 320 (40 per quadrant) Detector : E2V CCD-22 (Frame-Store) 600 x 600
Field of view : 41.3 x 41.3 arcmin
PSF: ~ 4 arcminsSensitivity (expected): 15 Crab (1 cps/mCrab)
SXT Effective Area vs. Energy (after subtraction of shadowing effects due to holding structure)
February 13, 2012
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Scanning Sky Monitor (SSM)
• Detector : Proportional counters with resistive anodes
• Ratio of signals on either ends of anode gives position.
• Energy Range : 2 - 10 keV
• Position resolution : 1.5 mm
• Field of View : 10 x 90 (degs) (FWHM)
• Sensitivity : 30 mCrab (5 min integration)
• Time resolution : 1 ms
• Angular resolution : ~ 10 arc min
Feb 13, 2012 K.P. Singh
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ASTROSAT – Key Strengths
Simultaneous UV to hard X-ray continuum (pure continuum) measurements
Large X-ray bandwidth, better hard X-ray sensitivity with low background
UV imaging capability better than GALEX
Simultaneous UV to hard X-ray spectral measurements with ASTROSAT : MCVs
Objectives
• Resolving all the spectral components (continuum):
UV and soft X-rays (thermal) from accretion disk, hard
X-ray reflection component, intrinsic power-law comp• Variability:
• WD Rotation Period• Binary Periods• Eclipses• Absorption Dips
• Shock Temperatures and Mass of the WD
Cataclysmic Variables with Astrosat
SXT
LAXPC
C
36
CVs: Open Issues• Many aspects deserve further investigation: here are some
– boundary layer in non-magnetics– the base of the post-shock accretion flow in magnetics and
the way this diffuses into the white dwarf– heating of the atmosphere around the accretion region in
magnetics, and effect on overall energy distribution– low accretion rate regimes in magnetics, whether this
results in a bombardment solution (no shock)– disk-magnetosphere interaction in IPs: important in a number
of contexts– disk-stream interactions in non-magnetics– magnetosphere-stream interactions in Polars– irradiation of the stream and secondary by X-ray flux– more astrophysics in the post-shock flow models (such as the
separation of electron and ion fluids)
• Combinations of high quality data (e.g. eclipse mapping of spectra) and new astrophysical fluid computations will transform the field and allow ever more intricate understandings of accretion phenomena to be achieved
18 Feb 2012 HEAP12- HRI (KP Singh)
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CVs in the grander scheme of things
• Cataclysmic variables are fairly common systems.
• CVs produce the low-level background of discrete sources in galactic X-ray emission – fainter but much more numerous than neutron-star or Black hole X-ray binaries
• They are highly important laboratories for studies of accretion
– disk behaviour › instabilities, › stream impacts, › warps, › tidal resonances, › spiral waves etc.
– magnetically dominated accretion › accretion columns, › emission from post-shock flow, › shocks, instabilities etc.
• Multi-wavelength emission (polarized in many cases) allows a multi-wavelength approach, providing very strong observational constraints on the interpretation of data
18 Feb 2012 HEAP12- HRI (KP Singh)
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CVs in the grander scheme of things (contd.)
• Important for investigations on how material interacts with a magnetic field:– threading region in Polars, – inner region of disk in Intermediate Polars, – Dwarf Nova oscillations in non-magnetic CVs
• In general, the balance of: – visibility of underlying system &– the emission (X-ray, optical) has been fundamental to making
enormous progress in understanding a wide range of astrophysics
• It is a field which incorporates fluid dynamics, MHD, a full range of emission processes, stellar evolution, gravitational radiation etc.
• A large number of important observational techniques have been developed in the context of CVs and then used elsewhere:– Doppler tomography, – eclipse mapping of disks and streams, – Stokes imaging, – timing analyses
• Progenitors of Type I Supernovae – Cosmological Distance Ladder
18 Feb 2012 HEAP12- HRI (KP Singh)
Feb 13, 2012 K.P. Singh
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Thank you !