Title: Thermonuclear Xray bursts as science driver
1Thermonuclear X-ray bursts asscience driver
Jean in t Zand
2X-ray bursts science driver requirements,
briefly
One of 12 Scientific Questions in ESAs Cosmic
Vision
- X-ray bursts are most luminous phenomenon nearest
to the densest matter of the visible universe - X-ray bursts are most luminous phenomenon from
the strongest gravitation fields in the visible
universe
- X-ray bursts are transient and the most
interesting ones are rather unpredictable ? need
monitor quick slewing
3Determine nature of NS matter
- By constraining M/R relation
- Through measurement of M and R
- M determined accurately in 20 cases (pulsars in
binaries) - Radius is difficult to measure accurately, let
alone for those systems which have accurate mass
measurements - From thermal radiation Fsigma (R/d)2 Teff4
- Through measurement of M/R, M/R2
- By gravitationally redshifted lines from NS
surface - By pressure-broadened lines (Stark effect)
- By rotationally broadened lines
- By measuring NS cooling curves (after SN, SXT or
XRB) - Amount of cooling set by amount of neutrino
emission which is dependent on nature of matter
4Slide from Deepto Chakrabarty
5Slide from Deepto Chakrabarty
6What are X-ray bursts?
7X-ray bursts thermonuclear flashes on neutron
stars
(Courtesy Andrew Cumming)
- Most luminous emission from surface of low-B NS,
albeit short
8Fuel accumulation and ignition
- Local accretion rate in low-B NSs 10 to 105 gr
s-1 cm-2 - After hours to days, accumulate columns of
y106-8 gr cm-2 - Pressure (yg) builds up to ignition condition
for nuclear fusion processes like CNO cycle,
triple-alpha, rp-capture etc - CNO often stable, triple-alpha not ?
thermonuclear shell flash ? X-ray burst
9X-ray burst movie of abundance evolution(Schatz
2003)
10Nuclear burning stability versus accretion rate
Heger et al. 2006
11X-ray burst phenomenology
12Burst profiles
2S 0918-549/WFC
GX 31/WFC
4U 1812-12 / HETE-WXM
GS 1826-24/WFC
Den Hartog et al. 2003 Nakagawa et al. 2004 in
t Zand et al. 2005
13Superburst profiles
Strohmayer Bildsten 2006
in t Zand, Cornelisse Cumming 2004
14lt- intermediate bursts
lt- superbursts (carbon)
He bursts -gt
mixed H/He bursts -gt
15Spectra with RXTE
- Black body to a high degree of accuracy
- kT 0.5-2.5 keV
- Fe-K line and edge at 6 and 9 keV
16Photospheric radius expansion
RXTE work by Galloway et al. (submitted)
Ginga result by Van Paradijs et al. 1990
1782 Galactic X-ray bursters (as of September 2006)
45
In t Zand et al. 2004 Galloway et al. 2005
Vanderspek 2005 Brandt et al. 2006
http//www.sron.nl/jeanz/bursterlist.html
18All 10 superbursters known sofar (Sep 06)
Purple uncertain detection Probably we have
detected already the majority of superbursters
19Map of X-ray bursters
Version 2001
20One classification of X-ray bursts that is useful
now
21Motivation EXO 0748-676
22Where it all seems to come together EXO 0748-676
Villarreal Strohmayer 2005
Cottam, Paerels Mendez 2002
Wolff et al. 2005
Oezel 2006
23Slide from Mariano Mendez
24Pursuit of confirmation of EXO results
- 2003 XMM-Newton obs. of EXO 0748-676 (570 ksec
76 bursts no full confirmation) - 2003 Chandra HETG obs. of EXO 0748-676 (300 ksec
no confirmation) - 2003 XMM-Newton obs. of GS 1826-24 (110 ksec no
confirmation) - 2006 Chandra obs. of GS 1826-24 (240 ksec
unsuccesful) - 2006 Chandra obs. of GX 354-0 (240 ksec
performed, no results yet) - XMM-Newton TOOs of superbursts(2 x 25 ksec
waiting for triggers from INTEGRAL and Swift) - Chandra TOO of one of brightest bursters 4U
1812-12 (90 ksec waiting for a trigger)
- Results on non-PRE burst negative, pursuit is now
for - features in PRE bursts and superbursts
25Weinberg, Bildsten Schatz (2006) dredging up
the ashes through convection in PRE bursts ?
touches on ISM pollution
26Observatory requirements
27General requirements for X-ray burst studies
- Need triggers ? need monitoring device
- monitor sensitivity should be able to detect 2
keV black body spectrum with bolometric flux of
10-8 erg s-1 cm-2 within 1 s, e.g. 100 cm2 at 40
x 40 sq deg - Have X-ray bursters in field of view, for
instance through considerable exposure on
Galactic center - Fast slew to target ? between 1 s and 1 hour. If
slew is slower than 1 min, one looses out on gt99
of all bursts. With 10 s one will detect at least
10 of all fluence ? carry out Galactic center
campaign to get sufficient triggers and
decrease slew time - NFI sensitivity. Best instrument sofar
XMM-Newton 100 cm2 for RGS 1500 cm2 for EPIC
PNMOS. Say this is threshold for EXO result on
28 bursts, one would need 500 cm2 _at_ 1 keV for
science in 1 burst.
28Specific requirements
- Monitor bandpass down to at least 5 keV
- Monitor spectral resolution 20 FWHM
- Monitor area few hundred cm2
- Monitor field of view 60 degrees FWZR
- Monitor angular resolution few arcminutes
- Slew speed few degrees per second, in
combination with dedicated observation program on
Gal. Center - NFI bandpass 0.3-10 keV
- NFI spectral resolution 3 eV _at_ 1 keV
- NFI area as large as possible but at least..
- NFI maximum countrate 10,000 (pile up?)
- NFI field of view none
- NFI angular resolution none
- NFI time resolution ?
29Finally points of concern..
- A confirmation of the EXO result would make for a
much stronger science case. So far, not so. Final
results probably within a year - All other bursters have fast rotation frequencies
(1 at 95 Hz 16 at gt270 Hz) line broadening
diminishes detection possibilities considerably
To be done..
- Model burster population more accurately and
determine possible trigger rates - Model spectra and predict resulting constraints
- Refine requirements