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Accreting neutron star spins and the equation of state

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Title: Accreting neutron star spins and the equation of state


1
Accreting neutron star spins and the equation of
state
  • Duncan Galloway
  • Monash University
  • Deepto Chakrabarty
  • Center for Space Research, MIT
  • Andrew Cumming
  • McGill University, Canada

MAD 07, November 2007
2
What is a neutron star made of?
  • Theory predicts in detail the likely structure in
    outer layers
  • Crust (1-2km) nuclei (mainly 56Fe) plus neutrons
    (1S0 superfluid?)
  • Composition of inner outer cores (up to 99 of
    mass) however EXTREMELY uncertain Hyperons?
    Pions? Kaons? Quark matter?
  • How can we find out?
  • (Figure courtesy D. Page)

3
Constraining the equation of state
  • Basically we want a simultaneous mass and radius
    measurement from a neutron star
  • This can be achieved by
  • Detection of rapidly-rotating neutron stars (in
    LMXBs or elsewhere)
  • Measurements of the neutron-star radius from the
    spectrum of thermonuclear (type-I) burst tails
  • Measurement of the Eddington limit from
    radius-expansion bursts
  • Detecting discrete spectral features from the
    neutron star surface
  • Measurement of the heat flux from the crust via
    thermonuclear burst recurrence times energetics

?
4
Low-mass X-ray binaries
5
(Some) present-day instruments
RXTE, launched 1995 (NASA) large effective area
and very high timing resolution but no imaging
capability 2-200 keV Chandra, launched 1999
(NASA), small effective area but very high
spatial and spectral resolution (courtesy
transmission gratings) 0.5-10 keV XMM-Newton,
launched 1999 (ESA), moderate effective area,
spatial and spectral resolution (reflection
gratings) optical monitor 0.5-10
keV INTEGRAL, launched 2002 (ESA), primarily
gamma-ray instrument but also wide-field X-ray
and optical capability 4 keV - 10 MeV
6
Constraints via rapid spin
  • Allowed region is to the left of the dashed
    curves
  • While the robust maximum spin rate is still 716
    Hz
  • a neutron star spinning at 1122 Hz or faster
    would rule out many EOSs

Lattimer Prakash 2007
  • So its not enough to find neutron stars spinning
    above the present maximum we really want to be
    well above 1000 Hz
  • Given the present limit of 716 Hz, this seems
    unlikely

7
Gravitational wave observatories
  • There are currently 4 interferometric
    gravitational wave observatories operational
    worldwide
  • Candidate sources include binary inspirals,
    stochastic background and rapidly rotating
    neutron stars
  • Hotly anticipated first detection of
    gravitational waves, perhaps within the next
    decade!
  • http//www.ligo.caltech.edu

8
Examples of X-ray bursts from RXTE
9
Constraints from thermonuclear bursts
  • We can measure the radius of the neutron star
    from the (blackbody) emission in the burst tail
  • Burst recurrence time depends on the heat flux
    from the interior -gt composition
  • We have lots of good quality (archival) data!
    (RXTE catalog, MINBAR project)

10
For more high-energy fun
  • Monthly High-Energy Astrophysics Teleconference
    (HEAT) http//users.monash.edu.au/dgallow/heat
    email Stephen Ng (ncy_at_physics.usyd.edu.au) to
    join the mailing list
  • High-energy Astrophysics Workshop, Kialoa, NSW,
    April 20-22 details TBA
  • http//www.physics.monash.edu.au/research/astronom
    y research areas honours/PhD projects
  • http//users.monash.edu.au/dgallow
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