1983
DOI: 10.1038/305508a0
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The Sun's quadrupole moment and perihelion precession of Mercury

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Cited by 32 publications
(14 citation statements)
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“…J 2 is an un‐normalized coefficient, which has different values in different papers owing to the different measuring technologies and theoretical models used (e.g. Campbell et al 1983; Kuhn et al 1998; Rozelot et al 2004; Kuhn et al 2009; Rozelot et al 2011). J 2 values are, for example, 0 ∼ 1.08 × 10 −5 (Kislik 1983), 1.46 × 10 −7 (Fivian et al 2008), 2 × 10 −7 (Pireaux & Rozelot 2003; Pitjeva 2005) and 2.3 × 10 −7 (Shapiro 1999).…”
Section: Disturbing Function Of Solar Oblateness and Disturbed Equamentioning
confidence: 99%
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“…J 2 is an un‐normalized coefficient, which has different values in different papers owing to the different measuring technologies and theoretical models used (e.g. Campbell et al 1983; Kuhn et al 1998; Rozelot et al 2004; Kuhn et al 2009; Rozelot et al 2011). J 2 values are, for example, 0 ∼ 1.08 × 10 −5 (Kislik 1983), 1.46 × 10 −7 (Fivian et al 2008), 2 × 10 −7 (Pireaux & Rozelot 2003; Pitjeva 2005) and 2.3 × 10 −7 (Shapiro 1999).…”
Section: Disturbing Function Of Solar Oblateness and Disturbed Equamentioning
confidence: 99%
“…However, the problem of how much of the perihelion advance results from solar oblateness remains and has been studied by numerous scientists during the past century (e.g. Gilvarry & Sturrock 1967; Sturrock & Gilvarry 1967; Boehme 1970; Dicke 1970; Campbell & Moffat 1983; Campbell et al 1983; Dicke, Kuhn & Libbrecht 1987; Kuhn et al 1998; Godier & Rozelot 1999; Shapiro 1999; Godier & Rozelot 2000; Milani et al 2001; Rozelot, Godier & Lefebvre 2001; Pireaux & Rozelot 2003; Rozelot et al 2004; Pireaux, Barriot & Rosenblatt 2006; Fivian et al 2008, 2009; Kuhn, Emilio & Bush 2009; Wayte 2010). The theoretical value of Mercury's perihelion precession was estimated from the disturbed equation so far and restricted to secular effects, without the disturbing problem exactly solved.…”
Section: Introductionmentioning
confidence: 99%
“…A conserved U(1) current is also introduced that couples to the metric without violating the equivalence principle; this current is interpreted to be a conserved number current (or fermion current) (28). In general, these constraints are quite weak (18)(19)(20)(21)(22)(23)(24)(25)(26)(27)(28)31). For example, the static, spherically symmetric solution is (39,40) The parameter l2 in [15] is the "charge" related to the aforementioned conserved particle number current in the usual way.…”
Section: Interpretation and Phenomenologymentioning
confidence: 99%
“…; however, the strong-field behaviour in general can be quite different because of the presence of torsion in N.G.T. (27,28).…”
Section: Introductionmentioning
confidence: 99%
“…an account of the perihelion advance of Mercury's orbit within the traditional Newtonian theory of gravity versus the modern account of Einstein's theory (Hall 1894;Campbell 1983); dark matter, dark energy and other proposals to account for the difference between what Einstein's theory of gravity predicts and some of the presently observed motions of galaxies and the rate of expansion of the universe itself (see van den Bergh 1999& Caldwell 2004 for a summary); and, finally, the many hidden variable theories which attempt to save the classical deterministic paradigm in the face of anomalous sub-atomic observations (see section 1.3.4 for references).…”
mentioning
confidence: 99%