ParametersChapter 3: The parameter files3.1 The basic timing model parametersThe parameter files (that contain the pulsar timing model and various instructions for the tempo2 fitting routines) have the same form as in the earlier tempo implementation. Each of the pulsar parameters has a label, a value and may have an uncertainty on the value and a flag indicating whether tempo2 should fit for this parameter or whether the parameter should be held constant (0 = default = hold constant; 1 = fit). The parameters labels are described in Table 3.1 at the bottom of this page. An example of a parameter file for PSR J0437-4715 taken from the ATNF pulsar catalogue (by selecting the ephemeris option): PSRJ J0437-4715
RAJ 04:37:15.7865145 1 7.000e-07
DECJ -47:15:08.461584 1 8.000e-06
DM 2.6469 1.000e-04
PEPOCH 51194.000
F0 173.6879489990983 1 3.000e-13
F1 -1.728314E-15 1 1.600e-20
PMRA 121.438 6.000e-03
PMDEC -71.438 7.000e-03
BINARY DD
PB 5.741046 1 3.000e-06
ECC 1.9186E-5 1 5.000e-09
A1 3.36669157 1 1.400e-07
T0 51194.6239 1 8.000e-04
OM 1.20 1 5.000e-02
OMDOT 0.016 1.000e-02
START 50640.928
FINISH 52088.897
CLK UTC(NIST)
EPHEM DE200
PBDOT 3.64E-12 2.000e-13
TZRMJD 51204.64376750220085
TZRFRQ 1413.400
TZRSITE 7
RM +1.5 5.000e-01
PX 7.19 1.400e-01
SINI 0.6788 1.200e-03
M2 0.236 1.700e-02
This indicates to tempo2 that all parameters should be held fixed except for the astrometric parameters (RAJ, DECJ), pulse parameters (F0, F1) and the Keplerian orbital parameters (PB, ECC, A1, T0 and OM). Uncertainties are given on many of the parameters. In more detail, a pulsar which has a spin period of P0=1.23456 s and no fitting is required then use: P0 1.23456 To request that tempo2 fits for this parameter: P0 1.23456 1 or to include an uncertainty on the measurement (which is ignored by the main tempo2 software) P0 1.23456 1 0.00003 Other commands may be given in parameter files that control the algorithms used by tempo2. Tempo2 only required the following parameters: PSRJ, DM, F0, PEPOCH, RAJ and DECJ. It is also possible to provide the pulsar parameters in the old-style tempo format where the arrival times and the parameters are given in the same file. Details of this mode (which we do not recommend) are given here. 3.2 Phase jumpsIt is often necessary to fit for a constant offset between two sets of arrival times. For instance, the templates used to determine arrival times at different observatories may be perfectly aligned. The command "JUMP" in the parameter file can be used to define such jumps:
JUMP -i PKS_DFB 0.234 1 JUMP FREQ 1400 1500 0 1 JUMP TEL PKS 0.342 which would initialise a jump for all observations with the "-i" flag set to "PKS_DFB" with the value of 0.234 and then fit for the jump. A jump would be included (and fitted) for all observations with frequencies between 1400 and 1500 MHz and a set (i.e. not fitted) jump would be included on all data observed using the "PKS" telescope. 3.3 Removing timing noiseEven with accurate spin and positional parameters, the timing residuals for some (particularly the young) pulsars contain remnant structures. Some of these structures are understood; cusps, for instance, signify sudden changes in the pulsar's spin rate during a glitch, sinusoidal oscillations can represent unmodelled companions (such as planets) or the pulsar precessing. However, many of the structures seen in the residuals are still not understood and are known as "timing noise". To obtain the most accurate pulsar's positional and proper motion parameters (and dispersion measure) it is essential to remove this timing noise. Traditionally this has been carried out by fitting higher order pulsar rotational derivative terms. However, Hobbs et al. (2004) described an improved method that used the fitting of harmonically related sinusoids. Such sinusoidal terms can be included in tempo2 parameter files. WAVE_OM 0 1 WAVE1 0 0 WAVE2 0 0 WAVE3 0 0 would allow tempo2 to select the fundamental frequency for the sinuosoids based on the data-span (see the algorithm described in Hobbs et al. 2004) and subsequently fit for 3 sine and cosine waves. Table 3.1: Pulsar parameters than can be entered in a parameter file
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