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A nonlinear tensor field and the second metric tensor
Authors:L Sh Grigorian  S Gottlöber
Institution:(1) Institute for Applied Physics Problems, Armenia;(2) Erevan State University, USSR;(3) Astrophysics Institute, Potsdam, Germany
Abstract:In our preceding paper {see L. Sh. Grigorian and S. Gottlöber, Astrofizika (in press)]} we investigated a self-gravitating system consisting of a scalar field and a linear tensor field ohgrik= ohgrki with minimal coupling and with allowance for the action of vacuum polarization effects. In the present paper we investigate the case of a nonlinear tensor field ohgrik. The action S psgr (epsiv) of the field ohgrik is determined by the difference RikRcaronik, where Rik is the space-time Ricci tensor and Rik is the analogous quantity constructed using the metric gammaik=gik+epsiohgrik induced by ohgrik (epsi is a free parameter). Here 
$$\mathop {lim}\limits_{\varepsilon  \to 0} $$
S psgr (epsiv) coincides with the previously known expression for the action of a linear field ohgrik. Equations of motion are derived for ohgrik in curved space-time. The energy-momentum metric tensor, determining the contribution of ohgrik to the gravitational field equations, is calculated.Translated from Astrofizika, Vol. 39, No. 1, pp. 135–144, January-March, 1996.
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