REVIEW
The Confrontation between General Relativity and Experiment
General Relativity and Quantum Cosmology · Submitted 16 Oct 2005 · 299 references
Pith's verdict: The field's reference document on experimental gravity, careful and candid in the body; the only real soft spot is that the abstract's 'half a percent' is tighter than the error budget actually supports.
Why Pith says this
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Referee report
The paper
The paper claims
The paper argues that general relativity agrees with every precision test of gravity performed to date, from laboratory equivalence-principle experiments to solar-system light deflection and binary-pulsar orbital decay.
The reading
What carries the argument
The bookkeeping device is the parametrized post-Newtonian formalism: ten coefficients, including $gamma$, $beta$, $xi$, $alpha_1$, $alpha_2$, and $alpha_3$, multiply the metric potentials that can appear at post-Newtonian order, so that each experiment becomes a bound on a combination of those coefficients. The argument also leans on the Einstein equivalence principle, which says local non-gravitational physics is independent of velocity and location, and on the strong equivalence principle, which extends that blindness to self-gravitating bodies. In binary pulsars, the machinery is the post-Keplerian timing model: the periastron advance, the redshift/time-dilation parameter, and the orbital-period derivative are expressed in general relativity as functions of the two masses, so three measured post-Keplerian parameters overdetermine the two masses and test the theory.
Extended reading notes
Core claim
The central claim is that general relativity has passed every precision test to date, and that the parametrized post-Newtonian framework organizes those tests into a coherent set of constraints on alternative metric theories. The paper reports $gamma-1=(2.1pm 2.3)times 10^{-5}$ from Cassini Doppler tracking, $gamma-1=(-1.7pm 4.5)times 10^{-4}$ from VLBI light deflection, a Nordtvedt parameter $eta_N=(4.4pm 4.5)times 10^{-4}$ from lunar laser ranging, and a corrected orbital-period derivative ratio $dot P_b^{rm CORR}/dot P_b^{rm GR}=1.0013pm 0.0021$ for the Hulse-Taylor pulsar. It also reports laboratory equivalence-principle bounds on the Eotvos ratio at the $3times 10^{-13}$ level and local-Lorentz-invariance bounds on $delta=1/c^2-1$ far below earlier optical experiments. Read together, these results leave no viable long-range scalar, vector, or preferred-frame alternative at the quoted sensitivity, and they extend the strong equivalence principle to neutron-star binaries.
Load-bearing premise
The conclusion that general relativity passes rests on the post-Newtonian framework being a complete parametrization of the deviations that matter, even though the paper restricts that framework to Poisson-like potentials and explicitly sets aside scalar fields with solar-system-scale Compton wavelengths and quantum-gravity-inspired $R^2$ terms.
Editorial extensions
If this is right
- Scalar-tensor gravity is pushed to coupling $omega>40000$ by the Cassini bound, so any long-range scalar partner of the metric must be very weakly coupled to matter.
- Preferred-frame parameters such as $alpha_1$ and $alpha_2$ are constrained below $10^{-4}$ and $10^{-7}$ respectively, leaving little room for theories with dynamical vector or prior-geometric fields.
- General relativity predicts only the two transverse quadrupolar gravitational-wave polarizations, so a detected breathing or longitudinal mode in a gravitational-wave network would contradict the theory.
- Direct observation of inspiralling compact binaries would test radiation reaction and the gravitational waveform at higher post-Newtonian order than the binary pulsar can reach.
Reading between the lines
- The review's null results are bounds on a specific family of metric theories, not on every conceivable deviation; a scalar field with a Compton wavelength comparable to solar-system scales, or a quantum-gravity dispersion effect, would not appear in the PPN table at all.
- The binary-pulsar agreement tests the radiative sector only at orbital velocities around $10^{-3}$, so direct inspiral waveforms probe a different regime and could reveal post-Newtonian terms that pulsar timing cannot constrain.
- The same equivalence-principle experiments that bound fifth forces can be read as bounds on any new long-range field coupled to mass-energy, including dark-sector fields whose macroscopic range is not yet excluded.
Original abstract
The status of experimental tests of general relativity and of theoretical frameworks for analysing them is reviewed. Einstein's equivalence principle (EEP) is well supported by experiments such as the Eotvos experiment, tests of special relativity, and the gravitational redshift experiment. Future tests of EEP and of the inverse square law are searching for new interactions arising from unification or quantum gravity. Tests of general relativity at the post-Newtonian level have reached high precision, including the light deflection, the Shapiro time delay, the perihelion advance of Mercury, and the Nordtvedt effect in lunar motion. Gravitational-wave damping has been detected in an amount that agrees with general relativity to better than half a percent using the Hulse-Taylor binary pulsar, and other binary pulsar systems have yielded other tests, especially of strong-field effects. When direct observation of gravitational radiation from astrophysical sources begins, new tests of general relativity will be possible.
The compiled record
The paper's own sentences, arranged, kept beside the review and separate from it. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
The abstract, sentence by sentence
The status of experimental tests of general relativity and of theoretical frameworks for analysing them is reviewed. Einstein's equivalence principle (EEP) is well supported by experiments such as the Eotvos experiment, tests of special relativity, and the gravitational redshift experiment. Future tests of EEP and of the inverse square law are searching for new interactions arising from unification or quantum gravity. Tests of general relativity at the post-Newtonian level have reached high precision, including the light deflection, the Shapiro time delay, the perihelion advance of Mercury, and the Nordtvedt effect in lunar motion. Gravitational-wave damping has been detected in an amount that agrees with general relativity to better than half a percent using the Hulse-Taylor binary pulsar, and other binary pulsar systems have yielded other tests, especially of strong-field effects. When direct observation of gravitational radiation from astrophysical sources begins, new tests of general relativity will be possible.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | The status of experimental tests of general relativity and of theoretical frameworks for analysing them is reviewed. | contribution 0.74 | 0.14 | 0.06 | asserted 0.55 |
| s1 | Einstein's equivalence principle (EEP) is well supported by experiments such as the Eotvos experiment, tests of special relativity, and the gravitational redshift experiment. | background 0.79 | 0.04 | 0.07 | asserted 1.00 |
| s2 | Future tests of EEP and of the inverse square law are searching for new interactions arising from unification or quantum gravity. | future work 0.94 | 0.06 | 0.05 | asserted 0.85 |
| s3 | Tests of general relativity at the post-Newtonian level have reached high precision, including the light deflection, the Shapiro time delay, the perihelion advance of Mercury, and the Nordtvedt effect in lunar motion. | background 0.51 | 0.07 | 0.06 | asserted 1.00 |
| s4 | Gravitational-wave damping has been detected in an amount that agrees with general relativity to better than half a percent using the Hulse-Taylor binary pulsar, and other binary pulsar systems have yielded other tests, especially of strong-field effects. | result 0.60 | 0.08 | 0.08 | asserted 1.00 |
| s5 | When direct observation of gravitational radiation from astrophysical sources begins, new tests of general relativity will be possible. | future work 0.99 | 0.05 | 0.11 | hedged possibility 0.92 |
What was examined, and what was not
- arXiv listing abstract v2
- full text
- figures and tables
- references and citing sentences
- relations to other papers
- P abstract
- S sections
- T body sentences
- C citations
- R cross-paper relations
Figures
Figures reproduced from arXiv:gr-qc/0510072 by the authors.
References
How later papers used it
372 later papers cite it
17 later papers by other authors are listed below: 13 used its data or values, 1 compared its own results with it and 3 cited it as support.
Uses its data or values 13 of 50 papers with this label
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Used this paper's tightest constraint on γ, |γ-1| < 2.3 × 10^-5, in its own work.
Solar system and equivalence principle constraints on f(R) gravity by chameleon approach (2007) · 0.99 · paraphrased: the licence does not allow quoting
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Used this paper's observational constraints on the PPN parameters β and γ in its own work.
On the parameters of the spherically symmetric parametrized Rezzolla-Zhidenko spacetime through solar system tests, orbit of S2 star about Sgr A$^\star$, and quasiperiodic oscillations (2023) · 0.99 · paraphrased: the licence does not allow quoting
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Used this paper's Solar system constraint |γ-1| < 2.3 × 10^-5 to find a bound on the thin shell parameter.
Modified gravity with disappearing cosmological constant (2020) · 0.99 · paraphrased: the licence does not allow quoting
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Used this paper's current tightest constraint |γ-1| < 2.3 × 10^-5 from Solar system tests of the post-Newtonian parameter γ to derive a bound on the thin shell parameter.
$\Lambda$CDM without cosmological constant (2020) · 0.99 · paraphrased: the licence does not allow quoting
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Used this paper's current Solar system limits on the PPN parameters in its own work.
Models of non-relativistic quantum gravity: the good, the bad and the healthy (2010) · 0.99 · paraphrased: the licence does not allow quoting
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Used this paper's Cassini tracking constraint |γ-1| < 2.3 × 10^-5 on the post-Newtonian parameter γ.
Phantom crossing, equation-of-state singularities, and local gravity constraints in f(R) models (2007) · 0.98 · paraphrased: the licence does not allow quoting
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Used this paper's Solar system constraints on the PPN parameters, |γ̃-1| < 2.3 × 10^-5 from Cassini tracking and |β̃-1| < 2.3 × 10^-4 from lunar laser ranging.
Semi-Analytic Stellar Structure in Scalar-Tensor Gravity (2010) · 0.98 · paraphrased: the licence does not allow quoting
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Used this paper's bound on the parameter γ in its own work.
Parameterized post Newtonian approximation in a teleparallel model of dark energy with a boundary term (2016) · 0.97 · paraphrased: the licence does not allow quoting
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Used this paper's light bending constraint δ = 1.0000 ± 0.0001.
Gravity Modification with Yukawa-type Potential: Dark Matter and Mirror Gravity (2009) · 0.96 · paraphrased: the licence does not allow quoting
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Used this paper's bound β < 10^-4 from experiments on the deviation parameter β.
On Non-commutative Geodesic Motion (2013) · 0.96 · paraphrased: the licence does not allow quoting
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Used this paper's bound from PPN data today, 1/2 ω(Ψ_now)+3 < 7 × 10^-4.
Scalar-tensor cosmologies with dust matter in the general relativity limit (2011) · 0.96 · paraphrased: the licence does not allow quoting
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Used this paper's current constraints α_1 < 10^-4 and α_2 < 4 × 10^-7.
Tests of Lorentz invariance: a 2013 update (2013) · 0.96 · paraphrased: the licence does not allow quoting
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Used this paper's experimental tests of the post-Newtonian parameters in the solar system in its own work.
Solar-System Constraints on f(R) Chameleon Gravity (2011) · 0.93 · paraphrased: the licence does not allow quoting
Compares with it 1 of 6 papers with this label
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We constrain the parameters of these three models and compare these constraints with the solar system constrains [ref] .
Gravitational radiation from binary systems in $f(R)$ gravity: A semi-classical approach (2022) · Constraints from observations · 0.98
Cites it as support 3 of 7 papers with this label
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Used this paper's statement that general relativity agrees with observations better than the percent as support for taking the standard description of neutron star orbital motion.
Gravitomagnetism in superconductors and compact stars (2007) · 0.98 · paraphrased: the licence does not allow quoting
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In fact, entire classes of modified gravity theories have been effectively ruled out (or at the very least stringently constrained) by Solar System observations alone [ref] , as we discuss below.
Gravitational-Wave Tests of General Relativity with Ground-Based Detectors and Pulsar-Timing Arrays (2024) · The importance of testing · 0.95
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Used this paper's compatibility with the weak equivalence principle, local Lorentz invariance and local position invariance as evidence that the Machian model reproduces general relativity's predictions.
Machian Origin of the Entropic Gravity and Cosmic Acceleration (2010) · 0.95 · paraphrased: the licence does not allow quoting
How the literature uses it
318 arXiv papers cite this in 498 sentences
Papers whose main result relates to this one's
States the same result 1 paper
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The status of experimental tests of general relativity and of theoretical frameworks for analysing them are reviewed.
The Confrontation between General Relativity and Experiment · 0.99
Papers citing it · 290 sentences without a confident label
Uses its method or tool 1 paper
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Second, by going to into the parameterized post-Newtonian (PPN) approach [ref] thereby, the asymptotic form of spacetime, reads as [equation] where $β$ and $γ$ denote the dimensionless PPN parameters.
No-Hair Theorem in the Wake of Event Horizon Telescope · A framework suitable for strong field testing of NHT · 0.93
Uses its data or values 45 papers
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The strongest constraint comes from $α_2$, which is constrained to satisfy $|α_2|<4×10^-7$ [ref] from limits on the Sun's spin precession, implying $|| < 4 ×10^-7$ (we will discuss this constraint in Section [ref]).
Solar System Constraints on Disformal Gravity Theories · A concrete model · 0.93
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While the inferred size of the shadow from the recently obtained horizon-scale images of the supermassive compact object in M87 galaxy by the EHT collaboration [ref] was found to be consistent to within 17% for a 68% confidence interval of the size predicted from GR for a Schwarzschild black hole using the a priori known estimates for the mass and distance of M87* based on stellar dynamics [ref] , this measurement admits other possibilities, as do various weak-field tests [ref] .
Constraints on black-hole charges with the 2017 EHT observations of M87* · Introduction · 0.92
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The present tightest constraint on $γ$ is $|γ-1| <2.3 ×10^-5$ [ref] , which translates into
Solar system and equivalence principle constraints on f(R) gravity by chameleon approach · Introduction · 0.99
Compares with it 6 papers
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Comparing them to those generated by the $α_1$-term in the PPN formalism [ref] (while the terms corresponding to $α_2$ and $α_3$ vanish in the present model [ref] ), we find that their ratio is $8 r^3/(r_s α_1√(2k)) ≈(r/10^4 AU)^3/α_1$, giving thus scalar effects similar to those of an $α_1 ≈2×10^-12$ at the orbit of Mars.
Improving relativistic MOND with Galileon k-mouflage · Introduction · 0.85
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For the Earth $M_⊕=5.97·10^24 Kg; R_⊕=6.37·10^6 m.$ so that [ref] [equation] that is similar to a bound recently obtained [ref] , which gives $ω>3·10^5$.
Precision Gravity Tests and the Einstein Equivalence Principle · Application to the Brans-Dicke metric · 0.94
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We constrain the parameters of these three models and compare these constraints with the solar system constrains [ref] .
Gravitational radiation from binary systems in $f(R)$ gravity: A semi-classical approach · Constraints from observations · 0.98
Cites it as support 4 papers
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Moreover, laboratory experiments support the idea that only the gravitomagnetic fields of coherent quantum systems are anomalous, whereas the gravitoelectric ones seem to be standard at a high level of accuracy [ref] , so we can reasonably take the standard description of neutron star orbital motion and discuss possible anomalous contributions, bearing in mind that the theory of general relativity is in agreement with observations better than the percent [ref] .
Gravitomagnetism in superconductors and compact stars · Astrophysical Observations · 0.98
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Will, the only theories of gravity that can embody EEP in the above constructive formulation of the Principle are those that satisfy the postulates of metric theories of gravity [ref] , which are: * Spacetime is endowed with a symmetric metric. * The trajectories of freely falling spherical test bodies are geodesics of that metric. * In local freely-falling and non-rotating reference frames the non-gravitational laws of physics are those written in the language of Special Relativity (SRT).
Is torsion needed in a theory of gravity? A reappraisal · Experimental evidence for torsion · 0.96
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The latter indeed changes its sign for antimatter, but the results for tests of the equivalence principle and GR in general indeed rule out this option [ref] .
A constraint on antigravity of antimatter from precision spectroscopy of simple atoms · Introduction · 0.99
Cites it as background 119 papers
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Solar system experiments constrain these parameters either directly or in combinations (see [ref] for a review) and so one can constrain a wide class of theories using the same experimental data.
Solar System Constraints on Disformal Gravity Theories · Introduction · 0.80
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In general, theories of gravity that depend on Riemann manifolds can host a maximum of six polarizations which are related to the metric tensor form, namely two tensor polarization modes (plus and cross), two vector modes (vector $x$ and vector $y$), and two scalar modes (breathing and longitudinal) [ref] .
Gravitational Wave Propagation and Polarizations in the Teleparallel analog of Horndeski Gravity · Introduction · 0.83
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Let us next discuss constraints from fifth force experiments that are carried out in a vacuum [ref] .
Solar system and equivalence principle constraints on f(R) gravity by chameleon approach · Introduction · 0.97
Discussion
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