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

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Higgs–Field <strong>and</strong> <strong>Gravity</strong> 107<br />

From the field equation (29) it follows for the non-trivial Higgs–field<br />

ground–state, c.f. (10) <strong>and</strong> (11)<br />

for which the Higgs–potential (26) is m<strong>in</strong>imized simultaneously; its correspond<strong>in</strong>g<br />

ground–state value is zero <strong>and</strong> herewith the field equations<br />

(28) for the metric are fulfilled i<strong>de</strong>ntically with the M<strong>in</strong>kowski–metric as<br />

the metrical ground–state. Insertion of (35) <strong>in</strong>to the Dirac equation (30)<br />

<strong>and</strong> <strong>in</strong>to the Higgs–field gauge current (32) of the Yang–Mills equation<br />

(31 yields the fermionic mass–matrix (19 <strong>and</strong> the matrix of the mass<br />

square of the gauge–bosons (20). In the unitary gauge the Higgs–field<br />

takes the form (15).<br />

Insertion of (14) <strong>and</strong> (15) <strong>in</strong>to (28) gives the field equation of gravitation:<br />

with the trace<br />

<strong>and</strong> the equation of motion<br />

Accord<strong>in</strong>g to (38) the excited Higgs–field generates a gravitation like<br />

potential force act<strong>in</strong>g on the massive particles as <strong>in</strong> section 1.<br />

Obviously the Newtonian gravitational constant is <strong>de</strong>f<strong>in</strong>ed as <strong>in</strong> (23)<br />

only after symmetry break<strong>in</strong>g by the ground–state value Simultaneously<br />

there exists a variability of the gravitational constant <strong>de</strong>scribed by

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