2008
DOI: 10.1088/0264-9381/25/14/145020
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General post-Minkowskian expansion of time transfer functions

Abstract: Abstract. Modeling most of the tests of general relativity requires to know the function relating light travel time to the coordinate time of reception and to the spatial coordinates of the emitter and the receiver. We call such a function the reception time transfer function. Of course, an emission time transfer function may as well be considered. We present here a recursive procedure enabling to expand each time transfer function into a perturbative series of ascending powers of the Newtonian gravitational c… Show more

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Cited by 100 publications
(184 citation statements)
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References 16 publications
(41 reference statements)
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“…Various concepts and techniques being useful to develop the 1-order RPS have been found in previous papers, among them, we may point out the definition and uses of the world function (Synge, 1931;Bahder, 2001;Bini et al, 2008;San Miguel, 2007) and the time transfer function, the form of this last function in the S-ST (Teyssandier and Le Poncin-Lafitte, 2008), and a method to find the user position coordinates by using the time transfer function (Čadež and Kostić, 2005;Čadež et al, 2010;Delva et al, 2011). Here, this last method is modified by using the analytical formula derived by Coll et al (2010) -instead of numerical iterations-to work with photons moving in M-ST The Earth's center is at rest in the asymptotic M-ST; hence, the S-ST may be considered as a perturbation of the asymptotic M-ST with a static metric g αβ = η αβ +s αβ , where η αβ is the Minkowski metric, and s αβ are perturbation terms depending on GM ⊕ /R, where R is the Schwarzschild radial coordinate.…”
Section: Relativistic Positioning In S-st: the 1-order Rpsmentioning
confidence: 99%
See 1 more Smart Citation
“…Various concepts and techniques being useful to develop the 1-order RPS have been found in previous papers, among them, we may point out the definition and uses of the world function (Synge, 1931;Bahder, 2001;Bini et al, 2008;San Miguel, 2007) and the time transfer function, the form of this last function in the S-ST (Teyssandier and Le Poncin-Lafitte, 2008), and a method to find the user position coordinates by using the time transfer function (Čadež and Kostić, 2005;Čadež et al, 2010;Delva et al, 2011). Here, this last method is modified by using the analytical formula derived by Coll et al (2010) -instead of numerical iterations-to work with photons moving in M-ST The Earth's center is at rest in the asymptotic M-ST; hence, the S-ST may be considered as a perturbation of the asymptotic M-ST with a static metric g αβ = η αβ +s αβ , where η αβ is the Minkowski metric, and s αβ are perturbation terms depending on GM ⊕ /R, where R is the Schwarzschild radial coordinate.…”
Section: Relativistic Positioning In S-st: the 1-order Rpsmentioning
confidence: 99%
“…It has been proved that T S may be expanded as follows [see Teyssandier and Le Poncin-Lafitte (2008) and references cited therein]:…”
Section: Relativistic Positioning In S-st: the 1-order Rpsmentioning
confidence: 99%
“…In this paper, we will revisit the role of the cosmological constant Λ in terms of the time transfer function recently proposed in [28,29], which is originally related to Synge's world function Ω(x A , x B ) and which enables us to circumvent the integration of the null geodesic equation. In Section 2, we will briefly summarize the time transfer function method.…”
Section: Introductionmentioning
confidence: 99%
“…This formulation has been proposed in [11] and it has been justified in the small impact parameter regime by much more theoretically rooted derivations in [5], [14] and [1]. Figure 4 shows that the order 2 correction is relevant for our experiment, especially when there is a superior conjunction with a small impact parameter of the radio wave path passing near the Sun.…”
Section: Shapiro Effectmentioning
confidence: 81%