ron remillard kavli center for astrophysics and space research
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INPE Advanced Course on Compact Objects Course IV: Accretion Processes in Neutron Stars & Black Holes. Ron Remillard Kavli Center for Astrophysics and Space Research Massachusetts Institute of Technology http://xte.mit.edu/~rr/inpe_IV.5.ppt. - PowerPoint PPT PresentationTRANSCRIPT
INPE Advanced Course on Compact Objects
Course IV: Accretion Processes in Neutron Stars & Black Holes
Ron RemillardKavli Center for Astrophysics and Space ResearchMassachusetts Institute of Technology
http://xte.mit.edu/~rr/inpe_IV.5.ppt
IV.5 Variability in X-ray Binary Systems
msec X-ray Pulsars Sources and Significance Timing and Spectral Properties
Aperiodic Variability in Accreting Neutron Stars Type I X-ray Bursts Type II X-ray Bursts Superbursts kHz QPOs
Aperiodic Variability in Black Holes Impulsive Relativistic Jets Weaker Types of Impulsive Jets Wild Instability Cycles in GRS1915+105
Msec X-ray PulsarsSource Spin (Hz) Orbit (hr) Bursts (Hz)
IGR J00291+5934 599 2.45
XTE J0929-314 185 0.73
XTE J1751-305 435 0.70
XTE J1807-294 191 0.58
SAX J1808.4-3658 401 2.00 bursts (401)
XTE J1814-338 314 4.27 bursts (314); not wd?
HETE J1900.1-2455 377 1.39 bursts
Swift J1756.9-2508 182 0.90
Characteristics:• Extremely compact binaries; wd companion (Rc~0.05 Ro; Mc~0.02 Mo)• Tip of reservoir of accretion-spun-up pulsars visible in X-rays• Key to spin-ID of burst oscillations • Key to inventory of spin distributions • Key toward a model for kHz QPOs
Msec X-ray Pulsars
XTE J0929-314: typical, faint transient peak ~ 30 mCrab (1.5-12 keV) outburst duration ~65 days
HETE J1900.1-2455: transient persists for 2+ years; brief turnoff ; early end of msec pulsations (Aug. 19, 2005)
Energy Spectra & Power Spectra of msec Pulsarsmsec X-ray pulsars resembleAtoll sources in hard state.
So why don’t atolls pulse(burst oscillations similar spin frequencies)
• B ranges different?• accretion plasma buries B?• HETEJ1900 may inform us!
Type I X-ray Bursts
Number of bursters ~80
Science Applications: Neutron-star finder Burst oscillations ( spin) Radius-expansion bursts
( distance estimate)
Redshifted abs. lines?(Cottam et al, 2003: 1? Case)
Test burst models Trace dM/dt at NS surface? Topic for BH event horizon
test (lack of bursts in BH)
Type I X-ray Bursts
Burst Oscillationse.g., Strohmayer
& Markwardt 1999
14 sources of BOs
max = spin
range: 45, 270-619 Hz
some frequency profiles are shorter or spotted (on/off)
amplitudes increase with energy (Muno et al. 2003)
Type I X-ray Bursts
Burst Oscillations
multiple max measures
From the same source give consistent results
Muno et al. 2002
Msec X-ray Pulsars and Burst Oscillations
Frequency (Hz)
Spin Distribution
Neutron Star Speed limit ~730 Hz(burst oscillations, radio pulsars, X-pulsars; Chakrabarty et al. 2003)
Why is limit < breakup freq.
• magnetic-accretion spin equilibrium? • Gravitational waves? (Wagoner 1984; Bildsten 1998)
Type I X-ray Bursts
Radius Expansion Burstse.g., Z-transient XTE J1701-462
Isolate burst spectrum(t)
Fit spectra to blackbody (R,t)
See R expansion
+ dip in T evolution
Eddinton Lx
distance estimate
(assume Mx, layer composition)
Look for consistent results
Rudimentary Elements of Bursts Models
Paradigm: thermonuclear explosion of H, He from accumulated, accreted matter on NS surface
Use Lx as a scale for dM/dt
Assume (vary) MNS and RNS
Assume (vary) composition Calculate (vary) T of subsurface layer (NS cooling model) Compute hydrostatic equilibrium Monitor (, T) for detonation conditions
Many complexities, e.g. differential rotation and turbulent mixing in surface layer (Prio & Bildsten 2007)
Bursts Models
Status of burst models(see Strohmayer & Bildsten 2006
many bursters on fast and slow side of burst rate expectations
Burst Oscillation Models
spot evolution
ray tracing for osc. amplitude(t))
Spitkovsky et al 2002, ApJ, 566, 1018
Type I bursts: huge science comeback; 1990s poster-child for “old and boring”
Type II X-ray Bursts
Number of sources 2 ; events are NOT thermal4U1730-33 (rapid burster + type I) ; GRO J1744-28 (bursting pulsar)
Linear E vs. t accretion instability
Cause unknown (magnetic?; high-rate ADAF?)
0 300 600Time (s)
Count rate
Rapid Burster; Inoue 2004, Adv. Sp. Res., 34, 2550
SuperBursts in Accreting Neutron Stars
Number of sources 8
duration: few to 10 hrtriggered by a type I burst
recurrence rate: year(s)
can excite transient pulsar at spin rate (1636-53)
model: C detonation in accretion/burst residue in subsurface layers
kHz QPOs
Number of sources 26 atolls 16
Z-type 8
msec pulsars 2
Properties• move in frequency (300-1200 Hz)• often twin, sometime solo• separation of twins varies slowly
kHz QPOs
QPO Scales
van der Klis 2006
Plot everything vs.upper kHz QPO
interpretationscontroversial
Upper kHz QPO
kHz QPOs
Current kHz QPO Models
Beat frequency model (Miller & Lamb)• twin peaks: Keplerian vs. NS surface footprint with RNS < RISCO
• twin peak separation interpreted as spin
• However, twin peak separation is spin or 0.5 spin
Disk Resonance (Abramowicz & Kluzniak)• TypIcial twin peaks are 600, 900 Hz 3:2 ratio• Resonance model for NS disks
Impulsive, Relativistic Jets in BH Binaries
GRS1915+105 jets
v > 0.9 c (Mirabel & Rodriguez 1994;
Fender et al. 1999)
Also GRO J1655-40, Cyg X-3,
XTE J1550-564 (see Fender 2006)
Special relativity demo; nut beware of assumption of bipolar symmetry
Ejection moment not observed
in X-rays
Black Holes in the Milky Way
Relativistic jets imaged in radioand also in X-rays (Chandra).
(Hannikainen et al. 2001; Corbel et al. 2002).
Baryonic content of MQ jets still uncertain,except for SS433
Impulsive, Relativistic Jets in BH Binaries
Small-scale impulsive jets• B-cycles of GRS1915+105 (Eikenberry et al. 1998; Fender + Pooley 1998)• strong evidence for disk:jet connection• other LC types (Eikenberry et al. 2007; Rodriguez et al. 2007)
More Complications: Fast X-ray Novae
SAX J1819.3-2525
(V4641 Sgr)
black hole binary
+ relativistic radio jets
‘Fast X-ray Nova’
20 min light curve,
Sept 15, 1999 (RXTE)
RXTE Observations of GRS1915+105
1996 – 2006: 1351 obs. (public data; 4.77 Ms)
785 data intervals (4.43 Ms)
Quasi-steady 428(rms < 16%; 1 s bins;
307 hard; 121 soft)
Variable Light Curves 357(rms > 16%)
Light Curve Types: Steady Variable
hard-steady 304 23 (-var )
soft-steady 64 0
soft-rolling 36 20
soft+dips 21 10
fast flare sequence + long min. 3 20
hard dip + trigger + soft spike 0 33
square waves 0 20
steady-flicker-dip sequence 0 5
flicker steady switching 0 16
flare-dip sequence + long min. 0 42
heartbeats (50 s) 0 89
dropouts to soft and variable 0 44
….new or inter- combinations 0 35 _______ _______
428 357
Steady Conditions: Color-Color Diagrams
Steady Conditions & Radio Flux
GRS1915+105: coded for radio flux (Ryle telescope, 15 GHz): (x x S < 5 mJy; 5 < S < 25; 25 < S < 75; S > 75 mJy ;
BHB Color-Intensity Diagrams
GRS1915+105/steady H1743-322 GX339-4
Fast QPOs in GRS1915+105
67 Hz: 28 (of 785) QPO detections ( > 4):
Sample: 67.37 Hz <Q> = 30.2
LC Type Detect (total) Frequency Q (freq./FWHM)
2 (64) 66.23 (0.34) 16
8 (56) 65.85 (0.24) 14
13 (31) 66.72 (0.21) 11
4 (16) 66.92 (0.70) 24
1 (20) 68.60 (0.93) 20
QPO Frequencies: 41, 67, 113, 165 Hz
67 Hz in “agitated soft state” or thermal:SPL intermediate
QPO near 67 Hz in type-averaged PDS[64][56][31]
QPOs in Variable States (avg. PDS; 2-40 kev)
[42] [89] [44]
GRS1915+105 Light Curves: Type
bright-hard zone contains a high-frequency QPO
GRS1915+105 : theta-blue
Power Density Spectra, blue regionQPO (9 ) at 165 +- 3 Hz; harmonic (330 Hz; 3.7 )
Q = 5, ampl = 2% (13-30 keV)
Colors resemble steep power-law state
GRS1915+105 Light Curves: Type
Long exposures, July 16-18, 2001. bright-hard zone: 113 Hz QPO at 6-40 keV
High Frequency QPOs from GRS1915+105
Type : bright-hard zone; 15-40 keV
Data Frequency Q (freq./FWHM)1997 Sept. 5-29 Remillard et al. 2002 165 (3) 5
1997 June - Oct. Belloni et al. 2006 166 (7) 2
All Type [44] (all HID zones) 165 (3) 4.7 (0.5)
Type : bright-hard zone; 6-40 keV
Data Frequency Q (freq./FWHM)2001 July 16-18 Remillard et al. 2004 113 (5) 2
All Type [42] (all HID zones) 112 (4) 2.2 (0.4)
GRS1915+105 Light Curves: Type
Profile variations within the group.
MIT undergraduate thesis: J. Z. Gazak
GRS1915+105 Light Curves: Type
Recurrence time and flare fractions for the group.
MIT undergraduate thesis: J. Z. Gazak
GRS1915+105 Light Curves: Type
Cycle zones for the group.
MIT undergraduate thesis: J. Z. Gazak
GRS1915+105 Light Curves: Type [82]
67 Hz in zone1
151 (4) Hz QPO
in zone 3
7 ; Q = 3.2
(8 +/- 3 % below 165 Hz)
keV: 2-40 6-40 15-40
QPOs in Variable States (avg. PDS; 2-40 kev)[42] [89] [44]
6-40 keV 6-40 keV 15-40 keV
MIRAX Support of Astrophysics
Properties Physical Models MIRAX Observations
Black Holes: mass Binary dynamics locate transients; optical teams
spin GR disk spectra thermal state measures & alerts
GR resonance (high-n QPOs) SPL state transitions and alerts
event horizon Type I burst models deep limits for burst function
jets Blandford-Znajek obs. moment of ejection; hard
GR MHD? Vertical B? state transitions; radio teams
accretion structures GR MHD (Prad regime) measure SPL high-Lx flares
MIRAX Support of Astrophysics
Properties Physical Models MIRAX Observations
Neutron Stars: mass Binary dynamics locate NS transients
radius kHz QPO models? bursts; atoll specra?
spin Binary evolution theory locate msxp transients
burst osc.; superburst osc.
magnetic field Mag. evol. models? pulsar cyclotron lines
SGR bursts; AXP bursts
internal structure NS structure models SGR oscillations
& crust Burst Models? Burst and superburst archive
jets MHD? hard state; transit.; radio team