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Table 1

Setup used to generate various datasets used in the current paper.

Dataset Central frequency Bandwidth Length of sub-integration (s) Template PSR ephemeris
(MHz) (MHz)
Setting 1 452 100 10 J0737−3039A J0737−3039A

Setting 2a 815 490 10 J0737−3039A/ J0737−3039A/
broad Gaussian/ eccentric (e=0.6)/
narrow Gaussian circular (e=0)

Setting 2b (SKA-Low) 200 300 2 J0737−3039A circular (e=0)

Setting 2c (SKA-Mid) 900 1100 10 J0737−3039A circular (e=0)

Setting 3a 815 490 10 J0737−3039A J0737–3039A/
Pb = 1 h/
Pb = 3 h/
Pb = 4.5 h

Setting 3b 7000 100 1 J0737−3039A J0737−3039A/
Pb = 4.5 h

Notes. Settings 1, 2a/b/c, and 3a/b are used to probe the pulsar orbital Doppler effect (Section 4.1), orbital profile smearing effect (Section 4.2.1), and folding issues with ‘polyco’ (Section 6), respectively. Number of frequency channels for all the setups is 200. For Settings 1, 2 and 3a the TZNSPAN parameter, which characterises the time resolution of the polynomial prediction, is fixed to 3 min. For Setting 3b TZNSPAN is 1 min. The template profile of J0737−3039A is constructed from the MeerKAT observations at L-band with a central frequency of 1283.582 MHz. Narrow and broad Gaussian profiles are simulated with width-period ratio (duty cycle) of 0.006 and 0.1, respectively. The parameter file of PSR J0737−3039A adopts measurements from Hu et al. (2022). To investigate how systematic error behaves under varying conditions, the PSR J0737−3039A ephemeris are modified as follows. Specifically, we alter the original orbital period (Pb = 2.45 h) and the eccentricity (e = 0.088) for a series of tests with the values listed in the table.

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