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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 299<br />

2.3. THE GENERAL STRUCTURE OF<br />

MODIFIED DISPERSION RELATIONS<br />

In both cases, that is <strong>in</strong> Eqs.(4) <strong>and</strong> (11), the general structure of<br />

dispersion relation for the propagation <strong>in</strong> one direction reads [10]<br />

where E is the energy of the photon. The parameter <strong>de</strong>pends on the<br />

un<strong>de</strong>rly<strong>in</strong>g theory <strong>and</strong> can be <strong>de</strong>rived to be for str<strong>in</strong>g theory [11]<br />

<strong>and</strong> ~ 4 for loop gravity [8]. The quantum gravity energy scale<br />

is, of course, of the or<strong>de</strong>r of the Planck energy From the above<br />

dispersion relation we <strong>de</strong>rive the velocity of light<br />

Therefore, the difference of the velocity of light for high energy photons<br />

<strong>and</strong> low energy photons, is given by<br />

<strong>Exact</strong>ly this quantity will be measured <strong>in</strong>, e.g., astrophysical observations,<br />

see below.<br />

3. TESTS OF MAXWELL’S EQUATIONS<br />

In or<strong>de</strong>r to make statements about the experimental status of Maxwell’s<br />

equations, one can just look experimentally for violations of predictions<br />

from Maxwell’s equations. A better strategy is first to build up a theoretical<br />

mo<strong>de</strong>l capable to <strong>de</strong>scribe as many <strong>de</strong>viations form the st<strong>and</strong>ard<br />

Maxwell theory as possible <strong>and</strong> afterwards to analyze the experimental<br />

results <strong>and</strong> astrophysical observations with this mo<strong>de</strong>l. Only <strong>in</strong> the latter<br />

case it is possible to make quantitative statements about the or<strong>de</strong>r of<br />

agreement of the Maxwell equations with experiments <strong>and</strong> observations.<br />

One theoretical frame which provi<strong>de</strong>s a complete <strong>de</strong>scription of all<br />

tests of Maxwell’s equations <strong>and</strong> which allows for a violation of all<br />

the dist<strong>in</strong>ctive features characteristic for the validity of the st<strong>and</strong>ard<br />

Maxwell equation, is given by the generalized Maxwell equations<br />

For the usual Maxwell equations we have <strong>and</strong><br />

where is the M<strong>in</strong>kowski metric. The homogeneous equations are not

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