pulsar timing - Australia Telescope National Facility

Pulsar Timing at Parkes
George Hobbs
CSIRO Australia Telescope National Facility
[email protected]
Purpose of talk
• Highlight some recent results relating to pulsar timing and the
Parkes Observatory
• Time constraints => will mainly concentrate on work that I’ve
been involved in
Large number of collaborators including: CASS pulsar group,
PPTA team, Chinese pulsar community ….
CSIRO. Gravitational wave detection
Pulsar timing
Slide from D. Champion
Fold
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Model
TOA (measured using the observatory clock)
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Residual
A few simulations
GW background
Spin-down irregularities
Clock noise
• With one pulsar you cannot (normally) tell what unmodelled
physical effect is causing the residuals
Simulated data
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Spin-down irregularities
No angular signature
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Terrestrial time standard irregularities
Monopolar signature
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Errors in the planetary ephemerides - e.g.
error in the mass of Jupiter
Dipolar signature
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What if gravitational waves exist?
Quadrapolar signature
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Studying individual pulsars using Parkes data
• M. Yu et al. (in preparation) – detection of 105 glitches in 36
pulsars observed at Parkes
• X. You et al. (in preparation) – analysis of the Solar Wind
magnetic field and electron density using PPTA observations of
J1022+1001
• Manchester et al. (2010) – relativistic spin precession in PSR
J1141-6545
• Weltevrede et al. (2010) – Pulsar timing for the Fermi mission
• Verbiest et al. (2008) - Limits on the variation of the
gravitational “constant”
• You et al. (2007) - Studies of the interstellar medium
• ….
• - concentrate in this talk on looking for correlations between
timing residuals ….
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Developing a pulsar-based time standard
Parkes data + Arecibo
Best time
standard
w.r.t. TT(TAI)
Pulsar time
standard w.r.t
TT(TAI)
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Measuring planetary masses
• Use International Pulsar Timing Array data
from Parkes, Effelsberg, Nancay and Arecibo.
• Champion et al. 2010, ApJ.
• A planetary mass error will lead to incorrect
determination of the Solar System barycentre
=> correlated pulsar timing residuals
• Can fit to multiple pulsars simultaneously to
search for such a signal
CSIRO. Gravitational wave detection
Measuring planetary mass
• Champion, Hobbs, Manchester et al. (2010), ApJ, 720, 201
• Use data from Parkes, Arecibo, Effelsberg and Nancay
MSun
Best Published
This work
Mercury
1.66013(7)x10-7
1.660(2)x10-7
Venus
2.4478686(4)x10-6
2.44782(10)x10-6
Mars
3.227151(9)x10-7
3.2277(8)x10-7
Jupiter*
9.547919(8)x10-4 -4
9.54791915(11)x10
2.85885670(8)x10-4
9.547916(4)x10-4
Saturn
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2.858858(14)x10-4
Published limits on gravitational wave
background (95% confidence)
Poor choice of pulsar?
All use the
same
Kaspi et
al. (1994)
data set
Tentative
new
bound
Incorrect algorithm?
Use same data set
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Pulsar navigation: assume that you are on the
Earth’s surface
• PULSE@Parkes observations
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Pulsar navigation: assume that you are on the
Earth’s surface
• Parkes observations
CSIRO. Gravitational wave detection
Pulsar navigation: assume that you are on the
Earth’s surface
• Parkes observations
CSIRO. Gravitational wave detection
Pulsar navigation: assume that you are on the
Earth’s surface
• Parkes observations
CSIRO. Gravitational wave detection
Pulsar navigation: assume that you are on the
Earth’s surface
• Parkes observations … correct to within a few kilometres
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Pulsar navigation: in 3D
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Conclusion
• Can distinguish between many phenomena by looking for
correlated timing residuals between pulsars
• Have improved understanding of individual pulsars
• Have developed a pulsar-based time standard
• Have the most precise, published, mass estimate for the Jovian
system
• Have not detected gravitational waves, but getting closer
• Can reverse the timing procedure to determine our position.
CSIRO. Gravitational wave detection