TY - JOUR
T1 - Proper motion, spectra, and timing of PSR J1813−1749 using Chandra and NICER
AU - Ho, Wynn C. G.
AU - Guillot, Sebastien
AU - Parkinson, P. M. Saz
AU - Limyansky, B.
AU - Ng, C.-Y
AU - Bejger, Michał
AU - Espinoza, Cristóbal M.
AU - Haskell, B.
AU - Jaisawal, Gaurava K.
AU - Malacaria, C.
PY - 2020
Y1 - 2020
N2 - PSR J1813-1749 is one of the most energetic rotation-powered pulsars known,
producing a pulsar wind nebula (PWN) and gamma-ray and TeV emission, but whose
spin period is only measurable in X-ray. We present analysis of two Chandra
datasets that are separated by more than ten years and recent NICER data. The
long baseline of the Chandra data allows us to derive a pulsar proper motion
mu_R.A.=-(0.067"+/-0.010") yr^-1 and mu_decl.=-(0.014"+/-0.007") yr^-1 and
velocity v_perp~900-1600 km/s (assuming a distance d=3-5 kpc), although we
cannot exclude a contribution to the change in measured pulsar position due to
a change in brightness structure of the PWN very near the pulsar. We model the
PWN and pulsar spectra using an absorbed power law and obtain best-fit
absorption NH=(13.1+/-0.9)x10^22 cm^-2, photon index Gamma=1.5+/-0.1, and
0.3-10 keV luminosity Lx~5.4x10^34 erg/s (d/5 kpc)^2 for the PWN and
Gamma=1.2+/-0.1 and Lx~9.3x10^33 erg/s (d/5 kpc)^2 for PSR J1813-1749. These
values do not change between the 2006 and 2016 observations. We use NICER
observations from 2019 to obtain a timing model of PSR J1813-1749, with spin
frequency nu=22.35 Hz and spin frequency time derivative
nudot=(-6.428+/-0.003)x10^-11 Hz/s. We also fit nu measurements from 2009-2012
and our 2019 value and find a long-term spin-down rate
nudot=(-6.3445+/-0.0004)x10^-11 Hz/s. We speculate that the difference in
spin-down rates is due to glitch activity or emission mode switching.
AB - PSR J1813-1749 is one of the most energetic rotation-powered pulsars known,
producing a pulsar wind nebula (PWN) and gamma-ray and TeV emission, but whose
spin period is only measurable in X-ray. We present analysis of two Chandra
datasets that are separated by more than ten years and recent NICER data. The
long baseline of the Chandra data allows us to derive a pulsar proper motion
mu_R.A.=-(0.067"+/-0.010") yr^-1 and mu_decl.=-(0.014"+/-0.007") yr^-1 and
velocity v_perp~900-1600 km/s (assuming a distance d=3-5 kpc), although we
cannot exclude a contribution to the change in measured pulsar position due to
a change in brightness structure of the PWN very near the pulsar. We model the
PWN and pulsar spectra using an absorbed power law and obtain best-fit
absorption NH=(13.1+/-0.9)x10^22 cm^-2, photon index Gamma=1.5+/-0.1, and
0.3-10 keV luminosity Lx~5.4x10^34 erg/s (d/5 kpc)^2 for the PWN and
Gamma=1.2+/-0.1 and Lx~9.3x10^33 erg/s (d/5 kpc)^2 for PSR J1813-1749. These
values do not change between the 2006 and 2016 observations. We use NICER
observations from 2019 to obtain a timing model of PSR J1813-1749, with spin
frequency nu=22.35 Hz and spin frequency time derivative
nudot=(-6.428+/-0.003)x10^-11 Hz/s. We also fit nu measurements from 2009-2012
and our 2019 value and find a long-term spin-down rate
nudot=(-6.3445+/-0.0004)x10^-11 Hz/s. We speculate that the difference in
spin-down rates is due to glitch activity or emission mode switching.
U2 - 10.1093/mnras/staa2653
DO - 10.1093/mnras/staa2653
M3 - Journal article
C2 - 33204043
SN - 0035-8711
VL - 498
SP - 4396
EP - 4403
JO - Monthly Notices of the Royal Astronomical Society
JF - Monthly Notices of the Royal Astronomical Society
ER -