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

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REFERENCES 319<br />

force can be foreseen for certa<strong>in</strong> systems when, effectively, the charged<br />

particles (of one <strong>and</strong> the same sign of charge) would experience a mutual<br />

“attraction”.<br />

Acknowledgments<br />

The author is much <strong>in</strong><strong>de</strong>bted to Bryce S. DeWitt for many friendly<br />

discussions; <strong>in</strong> particular, Bryce stressed (<strong>in</strong> May, 1992) the impossibility<br />

for systems of particles possess<strong>in</strong>g electric charges of one <strong>and</strong> the<br />

same sign, to create the field yield<strong>in</strong>g zero Lorentz force act<strong>in</strong>g on these<br />

particles. Thus he did implicitly anticipate that vanish<strong>in</strong>g of the Lorentz<br />

force should be a result of a superposition of the field mentioned above<br />

<strong>and</strong> a source–free electromagnetic field whose presence is obscured by<br />

the nonl<strong>in</strong>ear nature of E<strong>in</strong>ste<strong>in</strong>’s equations. My thanks are due to<br />

Georgios Tsalakou for the great pleasure of scientific collaboration with<br />

him. I gratefully acknowledge both spoken <strong>and</strong> e-mail discussions with<br />

Jan Horský; these contacts always were <strong>and</strong> cont<strong>in</strong>ue to be friendly <strong>and</strong><br />

fruitful.<br />

This work, <strong>in</strong> its <strong>in</strong>itial stage, was partially supported by the CONA-<br />

CyT (Mexico) Grant 1626P.<br />

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