Abstract

We analytically calculate some orbital effects induced by the Lorentz-invariance/momentum-conservation PPN parameter $\alpha_3$ in a gravitationally bound binary system made of a compact primary orbited by a test particle. We neither restrict ourselves to any particular orbital configuration nor to specific orientations of the primary's spin axis $\boldsymbol{\hat{\psi}}$. We use our results to put preliminary upper bounds on $\alpha_3$ in the weak-field regime by using the latest data from Solar System's planetary dynamics. By linearly combining the supplementary perihelion precessions $\Delta\dot\varpi$ of the Earth, Mars and Saturn, determined with the EPM2011 ephemerides, we infer $|\alpha_3|\lesssim 6\times 10^{-10}$. Our result is about 3 orders of magnitude better than the previous weak-field constraints existing in the literature, and of the same order of magnitude of the bound expected from the future BepiColombo mission to Mercury. It is, by construction, independent of the other preferred-frame PPN parameters $\alpha_1,\alpha_2$, both preliminarily constrained down to a $\approx 10^{-6}$ level. The wide pulsar-white dwarf binary PSR J0407+1607 yields a preliminary upper bound on the strong-field version $\hat{\alpha}_3$ of the Lorentz-invariance/momentum-conservation PPN parameter of the order of $3\times 10^{-17}$. It relies upon certain assumptions on the unknown values of the pulsar's spin axis orientation $\boldsymbol{\hat{\psi}}$, the orbital node $\Omega$ and the inclination $I$. Neither the pulsar's proper motion, still undetected, nor a possible value of the pulsar's mass $m_{\rm p}$ up to two solar masses substantially affect our result.

Highlights

  • Looking at the equations of motion of massive objects within the framework of the parameterized post-Newtonian (PPN) formalism [1,2,3,4], it turns out that, in general, the parameter α3 [4,5,6] enters both preferred-frame accelerations (see Equation (6.34) of [4]) and terms depending on the body’s internal structure, which, represent “self-accelerations” of the body’s center of mass (see Equation (6.32)of [4])

  • We focused on the Lorentz invariance/momentum-conservation PPN parameter α3 and on some of its orbital effects

  • We used the latest results in the field of the planetary ephemerides of the Solar System to preliminarily infer new weak-field bounds on α3

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Summary

Introduction

The latter ones arise from violations of the total momentum conservation, since they generally depend on the PPN conservation-law parameters α3 , ζ1 , ζ2 , ζ3 , ζ4 , which are zero in any semiconservative theory, such as general relativity. It turns out [4] that, for both spherically symmetric bodies and binary systems in circular motions, almost all of the self-accelerations vanish independently of the theory of gravity adopted. As a by-product of the use of the latest data from the Solar System’s dynamics, we will able to bound the other preferred-frame PPN parameters α1 , α2 , as well

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