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Exact Solutions and Scalar Fields in Gravity - Instituto Avanzado de ...

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On the experimental foundation of Maxwell’s equations 297<br />

effective equations govern<strong>in</strong>g the dynamics of the electromagnetic field<br />

is proposed [8, 9]. Despite that fact that all physical laws should be experimentally<br />

verified with <strong>in</strong>creas<strong>in</strong>g accuracy, the new quantum gravity<br />

<strong>in</strong>duced modifications of the Maxwell equations give additional motivation<br />

for test<strong>in</strong>g Maxwell’s equations. Moreover, s<strong>in</strong>ce Maxwell’s equations<br />

are so <strong>in</strong>timately connected with the special <strong>and</strong> general relativistic<br />

structure of structure of space–time, all tests of Special <strong>and</strong> General Relativity<br />

are <strong>in</strong> most cases at the same time also tests of the structure of<br />

Maxwell’s equations.<br />

2.1. LOOP GRAVITY INDUCED<br />

CORRECTIONS<br />

In loop gravity, averag<strong>in</strong>g over some quasiclassical quantum state, a<br />

so–called “weave”–state, which <strong>in</strong>clu<strong>de</strong>s the state of the geometry as well<br />

as of the electromagnetic field, gives the effective Maxwell equations [8]<br />

The correspond<strong>in</strong>g wave equation is<br />

The two helicity states lead to different<br />

dispersion relations<br />

There are two po<strong>in</strong>ts which need to be discussed: First, with (2) also a<br />

homogeneous Maxwell equation is modified <strong>and</strong>, second, the appearance<br />

of higher or<strong>de</strong>r <strong>de</strong>rivatives means that there are photons which propagate<br />

with <strong>in</strong>f<strong>in</strong>ite velocity.<br />

1 The <strong>de</strong>viation from the homogeneous Maxwell equations has the<br />

important consequence that the unique <strong>de</strong>scription of charged particle<br />

<strong>in</strong>terference is no longer true. If quantum mechanical equations<br />

are m<strong>in</strong>imally coupled to the electromagnetic potential, that<br />

is by the replacement then the phase shift <strong>in</strong> charged<br />

particle <strong>in</strong>terferometry is for a closed path C. If one<br />

applies Stokes’ law <strong>in</strong> the case of a trivial space–time topology <strong>in</strong><br />

that region, then this is equivalent to with<br />

where <strong>in</strong>tegration is over some 2–dimensional surface boun<strong>de</strong>d by<br />

the closed path C. The fact that the result should not <strong>de</strong>pend on

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