This section lists the experiments which are used to test gravity theories carried out on the earth.

The test of gravity theories can be viewed as test of the fundations of gravity theories and the the theories themselves, say test of equivalent principle and general relativity or f(R) gravity theory. Thus we should break down general relativity theory into several stages. Here, we use the following table to do so.

**Physical Fundations: Hyperthesis**:

Theory | Mach | WEP | EEP | SEP | GC | Notes |
---|---|---|---|---|---|---|

GR | Partial | Y | Y | Y | Y |

**Mathematical Description**:

Theory | Topoplogy | Manifold | Connection | Metric |
---|---|---|---|---|

GR | No torsion | Non-metricity tensor vanishes |

**Theoretical Implifications**:

Theory | Gravitational Waves | Newtonian Limit | GR Limit | Notes |
---|---|---|---|---|

GR | Y | Y |

Most items in mathematics are the same in different theories.

**WEP**: weak equivalence principle**EEP**: Einstein equivalence principle**SEP**: strong equivalence principle**GC**, General Covariance**Mach Principle**: gravity coupled to matter

- General covirance
- Linear approximation should be compatible with Newton’s thoery/Weak field and slow motion limit is Newton’s thoery of gravity
- In theory regarding the metric, no higher than second derivative is envolved and the terms of second derivative is linear.

The first point is for the invariance of frames/coordinates. The second point is for the success of Newtonian’s theory on our earth.

Why do we believe the third point? The answer is that we don’t have to. Here we propose it is because the simplicity of such quasilinear equations, i.e.,

\[F(\phi, \partial \phi) \partial^2\phi + G(\phi, \partial\phi) = 0\]

We have a bunch of theorems on this system, including its existance of solutions, Couchy problem, wave propagation etc.

We can use both 1&2 and 1&3 to derive Einstein’s equation. That is 2 and 3 are identical when 1 is considered.

This is an application of stationary principal and Hilbert action or Hilbert action plus a \(\Lambda\).

**The only possible second-order Euler-Lagrange expression obtainable in
a four dimensional space from a scalar density of the form**
\(\scr L = \scr L(g_{\mu\nu})\) **is**

\[E^{\mu\nu} = \alpha \sqrt{-g} [ R^{\mu\nu} - \frac{1}{2} g^{\mu\nu}R ] +\lambda \sqrt{-g} g^{\mu\nu}\]

Thus modification could be

- Metric tensor not a fundamental tensor
- Higher than second order derivatives of the metric in the field equations
- Not a four dimension space
- Not rank (2,0) tensor field equations, non-symmetry of field equations under exchange of indices, or divergence field equations
- non-locality

**All spherically symmetric solutions of Einstein’s equations in vacuum
must be static and asymptotically flat, without** \(\Lambda\).

Actually, this can be extended to a \(\Lambda\) space only keeping the static result.

**The generic final state of gravitational collapse is a Kerr-Newman
black hole, fully specified by its mass, angular momentum and charge**

Also, “in the context of General Relativity with a cosmological constant all expanding universe solutions should evolve towards de Sitter space.” [1] This is only valid in some situation.

[1] | R. M. Wald. Asymptotic behavior of homogeneous cosmological models in the presence of a positive cosmological constant. Phys. Rev. D, 28(8):2118–2120, Oct 1983. |

The vacuum Einstein equation

\[R^{\mu\nu} - \frac{1}{2} g^{\mu\nu} R = 0,\]

which indicates that all constant metrics are solutions to vacuum Einstein equation.

Physically this doesn’t make any sense, unless we impose that our universe is Minkowski like. From this point of view, vacuum Einstein equation is more general than our universe.

Gauge freedom is the freedom of choosing a coordinate system. Fixing a gauge means choosing a particular coordinate system.

Gauge tranformation is Lie derivative along some arbitary vector here.

Line element

\[\begin{split}\tilde g _ {00} &=& -a^2(1+2 A Y) \\
\tilde g _ {0j} &=& -a^2 B Y _ j \\
\tilde g _ {ij} &=& a^2(\gamma _ {ij} +2 H _ L Y \gamma _ {ij} +2 H _ T Y _ {ij} )\end{split}\]

Energy momentum tensor is

\[\begin{split}\tilde T^0 _ {\phantom{0}0} = -\rho (1+\delta Y) \\
\tilde T^0 _ {\phantom{0} j} = (\rho + p)(v - B) Y \\
\tilde T^j _ {\phantom{j}0 } = -(\rho + p)v Y^{j}\end{split}\]

For a infinitesimal gauge transformation along some vector (\(X = T \partial_t + L^i \partial_i\)), gauge variables are

Symbol | Physics | Gauge Transformation | Note |
---|---|---|---|

\(\tilde A\) |

Through that we can find out gauge invariant variables.

Synge once said, use space and time, and define them.

This post is aimed to make clear what frame are we in.

In general relativity, we often transform coordinates. Here is an example.

**The general form of metric with spherical space component is**

(1)¶\[\mathrm ds^2 = - \gamma(r,t)c^2\mathrm dt^2 + \beta(r,t)c\mathrm dr\mathrm dt + \alpha(r,t)[\mathrm dr^2 + r^2 (\mathrm d\theta^2 + \sin^2\theta \mathrm d\phi^2)]\]

With a transformation \(\alpha(r,t)r^2 = r'^2\),

\[\mathrm ds^2 = - \gamma'(r',t)c^2\mathrm dt^2 + \beta'(r',t)c\mathrm dr\mathrm dt + \alpha(r,t)[\mathrm dr^2 + r^2 (\mathrm d\theta^2 + \sin^2\theta \mathrm d\phi^2)]\]

Then compose the integral multiplier

\[c\mathrm dt'= \eta(r',t) [ - \gamma'(r',t) c \mathrm dt + \frac{1}{2} \beta'(r',t)\mathrm dr']\]

And finally,

\[\mathrm ds^2 = -\eta^{-2}(r',t) \gamma'^{-1}(r',t)c^2\mathrm dt'^2 + [\alpha'(r',t) + \frac{\beta'^2(r',t)}{4r'} ]\mathrm dr'^2 + r'^2(\mathrm d\theta^2 + \sin^2\theta\mathrm d\phi^2)\]

In general

(2)¶\[\mathrm ds^2 = -b(r,t)c^2\mathrm dt^2 + a(r,t)\mathrm dr^2 + r^2(\mathrm d\theta^2 + \sin^2\theta\mathrm d\phi^2)\]

Then what? The two forms of metric demonstrate different properties. Take Birkhoff theorem as an example. The results could be very different startting from the form (1) and (2).

It is obviously very important to show what the coordinate transformation means and what frame are the observers in indicated by the coordinates.

- Inertial mass \(m_I\)
- Gravitational mass \(m_G\)

In Newtonian system, the acceleration of an object will be

\[\vec a \propto \frac{\vec F}{m_I}.\]

In a static and uniform gravitation field, the gravity force is

\[G = - g m_G \hat r\]

Thus the acceleration in this case should be

\[\vec a\propto -\hat r g \frac{m_G}{m_I}\]

When \(m_G/m_I\) is constant, the falling accerelation are the same for different objects with same mass. However, if \(m_G/m_I\) is not a constant, say \(m_G\ne m_I\), different objects would fall at different acceleration.

Now if we put two ball with different mass on the Eotvos torsion balance, the balance would rotate and we can measure it.

Detection of \(R^k_{0l0}=(1/c^2)\partial^2\Phi/\partial x^k\partial x^l \sim 10^{-32} \text{cm}^{-2}\).

Anisotropy of gravitation/electromagnetism is not proved in our galaxy.

Similar to Eddington and Dyson’s bending light observation, radio signals serve as a more precise experiment to test Einstein’s theory. And these experiments are against scalar tensor theories because scalar tensor theories give a smaller bending angle (1.66 second of arc less than the observations).

Tables constructed according to arXiv:1106.2476v3.

Test of fundamental principles

- WEP： 1. Eotvos torsion balance： \(\eta = (0.3 \pm 1.8) \times 10^{-13}\), More precise in space exp.[1a]_ [1b] [1c] 2. Gravitational redshift of light [2]
- EEP: 1. Hughes-Drever Experiment: \(n \le 10^{-27}\), references [3a] [3b]

Test of GR:

- Null geodesics test: 1. photon trajectory, spatial deflection: \(\theta = (0.99992\pm 0.00023)\times 1.75''\), where 1.75 is the theoretical value; Achieved through observing star position, etc [4] 2. Shapiro time-delay effect: \(\Delta t = (1.00001\pm 0.00001)\Delta t_{GR}\), references [5a] [5b]
- Time like geodesics: 1. Anomalous perihelion precession: Just use the PPN formalism [6a] [6b] [6c] 2. Nordtvedt effect: \(\eta = (-1.0 \pm 1.4) \times 10^{-*13}\), references [7a] [7b] 3. Spinning objects obiting [8a] [8b]
- Small-range: 1. Potential probing [9a] [9b]
- Radiation 1. Speed of gravitational waves 2. Polarity of gravitational radiation 3. Dynamics of source objects

[1a] | arXiv:0712.0607 |

[1b] | Eotvos experiment: using torsion balance to test the equality of gravitational mass and inertial mass. Wikipedia has a photo of how this works. |

[1c] | \(\eta=2\frac{ABS(a1-a2)}{ABS(a1+a2)}\). \(a1\) and \(a2\) are the accelerations of the two bodies in Eotvos torsion balance. Thus \(\eta\) is the accleration difference of the two objects. |

[2] | To be added |

[3a] | References: R. W. P. Drever. A search for anisotropy of inertial mass using a free precession technique. Philosophical Magazin, 6:683-687, May 1961. ; V. W. Hughes, H. G. Robinson, and V. Beltran-Lopez. Upper Limit for the Anisotropy of Inertial Mass from Nuclear Resonance Experiments. Physical Review Letters, 4:342-344, Apr. 1960. ; S. K. Lamoreaux, J. P. Jacobs, B. R. Heckel, F. J. Raab, and E. N. Fortson. New limits on spatial anisotropy from optically-pumped 201 Hg and 199 Hg. Physical Review Letters, 57:3125–3128, Dec. 1986. ; T. E. Chupp, R. J. Hoare, R. A. Loveman, E. R. Oteiza, J. M. Richardson, M. E. Wagshul, and A. K. Thompson. Results of a new test of local Lorentz invariance: A search for mass anisotropy in 21 Ne. Physical Review Letters, 63:1541–1545, Oct. 1989. |

[3b] | Hughes-Drever Experiment: test the isotropy of mass and space through the NMR spectrum, or the mono-metric spacetime. |

[3c] | n: four momentum of the test particle is \(p_\mu = \frac{m g_{\mu\nu}u^\nu}{\sqrt{-g_{\alpha\beta}u^\alpha u^\beta}} + \frac{ n h_{\mu\nu}u^\nu }{ -h_{\alpha\beta} u^\alpha u^\beta }\). Thus \(n\) is the effect of another metric. |

[4] | S. S. Shapiro, J. L. Davis, D. E. Lebach, and J. S. Gregory. Measurement of the Solar Gravitational Deflection of Radio Waves using Geodetic Very-Long-Baseline Interferometry Data, 1979 1999. Physical Review Letters, 92(12):121101, Mar. 2004. |

[5a] | References, I. I. Shapiro. Fourth Test of General Relativity. Physical Review Letters, 13:789–791, Dec. 1964. ; B. Bertotti, L. Iess, and P. Tortora. A test of general relativity using radio links with the Cassini spacecraft. Nature, 425:374–376, Sept. 2003. |

[5b] | Shapiro time-delay effect: time delay when light travels through a massive object. |

[6a] | Observational data for the value of perihelion precession of Mercury are summarized in E. V. Pitjeva. Modern Numerical Ephemerides of Planets and the Importance of Ranging Observations for Their Creation. Celestial Mechanics and Dynamical Astronomy, 80:249–271, July 2001. |

[6b] | PPN formalism is the lowest order of GR. |

[6c] | Anomalous precession: |

[7a] | K. Nordtvedt. Equivalence Principle for Massive Bodies. I. Phenomenology. Physical Review, 169:1014–1016, May 1968. ; J. G. Williams, S. G. Turyshev, and D. H. Boggs. Progress in Lunar Laser Ranging Tests of Relativistic Gravity. Physical Review Letters, 93(26):261101, Dec. 2004, arXiv:gr-qc/0411113. |

[7b] | Nordtvedt effect: massive objects in Eotvos torsion balance experiments. We can use the whole Earth-Moon system to test this effect. |

[8a] | To be added |

[8b] | There is a Lense Thirring effect here. GPB has done this. |

[9a] | GR can be reduced to Newtonian potential at small range. |

[9b] | Currently, most of the modification has a Yukawa potential form. |

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