Transcript Document

ULXs and Evidence for Two IMBHs in M82
Hua Feng
Tsinghua University
Collaborators: Phil Kaaret (Iowa), Fengyun Rao (Tsinghua),
Jing Jin (Tsinghua)
XMM-Newton 2010 Science Workshop, Madrid, Spain
M82 – a nearby starburst galaxy
Three ULXs in M82
X42.3+59
X41.4+60; X-1

X37.8+54
X41.4+60: 62-day X-ray periodicity
Companion’s density for Roche-lobe overflow system
 = 510-5 g cm-3
a giant or supergiant star
(Kaaret et al. 2006; Kaaret & Feng 2007)
X41.4+60: Low frequency QPOs
Frequency varies from 50-100 mHz
(Strohmayer & Mushotzky 2003; Dewangan et al. 2006;
Mucciarelli et al. 2006; Feng & Kaaret 2007)
Joint Chandra/XMM Observations
2008 Oct 4
2009 Apr 17
2009 Apr 29
Off-axis & subarray configuration to minimize the pileup effect
X41.4+60 was observed at the highest flux on 2008 Oct 4.
XMM-Newton observations:
No QPOs, no timing noise above the Poisson level at > 1mHz
Spectral change: from power-law to disk model
Chandra spectrum on 2008 Oct 4
Multicolor accretion disk model
2/dof = 67.8/70
Power-law model with pileup
2/dof = 201.8/71
Power-law model without pileup
2/dof = 102.1/70
Ldisk  T4
X41.4+60: thermal dominant state
• No QPOs and low timing noise
• Disk model with L  T4
• Emission States
– hard, thermal dominant, steep power-law (Remillard &
McClintock 2006)
Corona
Disk
Thermal dominant state
(Gierlinski & Done 2004)
• L  T4: constant inner radius
• The accretion disk extends all the way to ISCO
• RISCO depends on MBH and Spin
Fitting with a fully relativistic disk model
M = 200-800 Msun
a* > 0.93
i > 60
IMBH with nearly
maximal spinning !
Hard to Thermal transition
Relatively low flux
Hard power-law spectrum
QPOs + flat-top PSD
Three ULXs in M82
X42.3+59
X41.4+60; X-1

X37.8+54
X42.3+59: sometimes brighter than X41.4+60
XMM-Newton
Chandra
15 radius
X42.3+59
X41.4+60
X42.3+59: A transient ULX
Chandra
Chandra
X42.3+59: A transient ULX
(Feng & Kaaret 2007)
> 1000
Stellar mass black hole with massive donor: stable accretion disk
IMBH: unstable accretion disk (Kalogera et al. 2004)
X42.3+59: discovery of QPOs
• Confirmed by simultaneous
Chandra/XMM observations
• Narrow range: 3-4 mHz
• Broad & strong
• No red noise (down to QPO / 100)
• Only appear when LX > ~1040 erg/s
(Feng, Rao, & Kaaret 2010)
Three Types of LFQPOs
XTE J1859+226
GX 339-4; Type B QPOs
(Belloni et al. 2005)
(Casella et al. 2004)
X42.3 QPOs are of Type A or B
Type A/B QPOs: narrow frequency range
(Casella et al. 2005)
X42.3 QPOs: 103 times lower than in stellar mass BHs
X42.3: 104 solar masses; companion star not needed
Three ULXs in M82
X42.3+59
X41.4+60; X-1

X37.8+54
X-ray dips during one outburst
Source spectrum: soft excess + hard component
Soft excess: blackbody emission from a massive outflow (King 2004; Poutanen et al. 2007)
Summary
• X41.4+60: ~102 solar masses
– hard state
• Orbital period of 62 days
• Low frequency QPOs and strong variability
• Power-law spectrum with  = 1.7
– thermal dominant state
• outbursts
• No QPOs, low timing noise
• Thermal spectrum, L  T4
• X42.3+59: ~104 solar masses
– Low frequency type A/B QPOs around 3-4 mHz
– 103 lower than the frequency of the same type QPOs in stellar mass
black holes
• X37.8+54: tens of solar masses
– A thrid, new ULX in M82
– Stellar BH with massive outflow
Feng & Kaaret 2010
Feng, Rao, & Kaaret 2010
Jin, Feng, & Kaaret 2010