what’s the deal with psr j1022+1001?
TRANSCRIPT
What’s the deal with PSR J1022+1001?
Parkes Pulsar Timing Array Discussion 5 September 2012
Willem van Straten
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PSR J1022+1001 profile
PSR J1022+1001
Camilo, F., Nice, D. J., Shrauner, J. A., & Taylor, J. H. 1996, ApJ, 469, 819
• using Arecibo and Greenbank • first observed profile shape variations
“on a timescale of minutes” • limit to timing precision
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PSR J1022+1001
Kramer, M., Xilouris, K. M., Camilo, F., Nice, D., Lange, C., Backer, D. C., & Doroshenko, O. 1999, ApJ, 520, 324
• using Effelsberg • observed profile shape variations in
both time and frequency • EQUAD ~ 10 µs
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Xilouris, K. M. 1991, A&A, 248, 323
Result in boost ~ 0.1
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PSR J1022+1001
Ramachandran, R. & Kramer, M. 2003, A&A, 407, 1085
• using Westerbork = equatorial mount • therefore, no parallactic angle variation • does not imply instrumental stability!
– automatic gain controllers – phase drift
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PSR J1022+1001
Hotan, A. W., Bailes, M., & Ord, S. M. 2004, MNRAS, 355, 941
• using Parkes • no evidence for shape variations • timing r.m.s ~ 2.2 µs • χ2/Nfree ~ 1.4
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Template Matching
ϕ P(φ) = aS(φ+ ϕ) + b
P(ν) = aS(ν)e-i2πϕν + δ(ν)b
FFT
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Arrival Time Comparison
• 278 TOAS spanning 6.9 years 13