2024A&A...686A.101B


Query : 2024A&A...686A.101B

2024A&A...686A.101B - Astronomy and Astrophysics, volume 686A101 (2024/6-1)

A new pulsar timing model for scalar-tensor gravity with applications to PSR J2222-0137 and pulsar-black hole binaries.

BATRAKOV A., HU H., WEX N., FREIRE P.C.C., VENKATRAMAN KRISHNAN V., KRAMER M., GUO Y.J., GUILLEMOT L., McKEE J.W., COGNARD I. and THEUREAU G.

Abstract (from CDS):

Context. Scalar-tensor gravity (STG) theories are well-motivated alternatives to general relativity (GR). One class of STG theories, Damour-Esposito-Farèse (DEF) gravity, has a massless scalar field with two arbitrary coupling parameters. We are interested in this theory because, despite its simplicity, it predicts a wealth of different phenomena, such as dipolar gravitational wave emission and spontaneous scalarisation of neutron stars (NSs). These phenomena of DEF gravity can be tested by timing binary radio pulsars. In the methods used so far, intermediate phenomenological post-Keplerian (PK) parameters are measured by fitting the corresponding timing model to the timing data whose values are then compared to the predictions from the alternative theory being tested. However, this approach loses information between intermediate steps and does not account for possible correlations between PK parameters.
Aims. We aim to develop a new binary pulsar timing model 'DDSTG' (called after Damour, Deruelle and STG) to enable more precise tests of STG theories based on a minimal set of binary parameters. The expressions for PK parameters in DEF gravity are self-consistently incorporated into the model. PK parameters depend on two masses which are now directly fitted to the data without intermediate steps. The new technique takes into account all possible correlations between PK parameters naturally.
Methods. Grids of physical parameters of NSs were calculated in the framework of DEF gravity for a set of 11 equations of state. Automatic differentiation (AutoDiff) technique was employed, which aids in the calculation of gravitational form factors of NSs with a higher precision than in previous works. The pulsar timing program TEMPO was selected as a framework for the realisation of the DDSTG model. The implemented model is applicable to any type of pulsar companions. We also simulated realistic future radio-timing datasets for a number of large radio observatories for the binary pulsar PSR J2222-0137 and three generic pulsar-black hole (PSR-BH) systems.
Results. We applied the DDSTG model to the most recently published observational data for PSR J2222-0137. The obtained limits on DEF gravity parameters for this system confirm and improve previous results. New limits are also the most reliable because DEF gravity is directly fitted to the data. We argue that future observations of PSR J2222-0137 can significantly improve the limits and that PSR-BH systems have the potential to place the tightest limits in certain areas of the DEF gravity parameter space.

Abstract Copyright: © The Authors 2024

Journal keyword(s): gravitation - binaries: close - gravitational waves - pulsars: general - stars: individual: J2222-0137

Simbad objects: 16

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Number of rows : 16
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 PSR J0514-4002A Psr 05 14 06.6927 -40 02 48.897           ~ 69 1
2 NGC 1851 GlC 05 14 06.76 -40 02 47.6           ~ 1529 0
3 PSR J0737-3039A Psr 07 37 51.24669 -30 39 40.6895           ~ 317 1
4 PSR J1141-6545 Psr 11 41 07.00060 -65 45 19.0500     25.08 24.38   ~ 207 1
5 NAME Galactic Center reg 17 45 39.60213 -29 00 22.0000           ~ 16269 0
6 NGC 6544 GlC 18 07 20.58 -24 59 50.4   11.36 9.90     ~ 332 0
7 PSR J1807-2500B Psr 18 07 20.871209 -25 00 01.91500           ~ 64 0
8 NGC 6624 GlC 18 23 40.51 -30 21 39.7           ~ 939 1
9 PSR J1823-3021G Psr 18 23 40.7213 -30 21 35.630           ~ 13 0
10 PSR J1835-3259A Psr 18 35 44.856 -32 59 25.08           ~ 22 0
11 NGC 6652 GlC 18 35 45.63 -32 59 26.6           ~ 474 0
12 PSR J1915+1606 Psr 19 15 27.99999 +16 06 27.4034     22.5     ~ 1032 1
13 PSR B2127+11 Psr 21 29 58.24650 +12 10 01.2339           ~ 102 2
14 M 15 GlC 21 29 58.33 +12 10 01.2           ~ 3274 0
15 PSR J2129+1209C Psr 21 30 01.2030 +12 10 38.159           ~ 215 2
16 PSR J2222-0137 Psr 22 22 06.00015 -01 37 15.7827           ~ 78 0

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