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We study the backreaction of quantum fields in the Boulware vacuum state on the Schwarzschild geometry, using the Riegert–Mottola–Vaulin renormalized stress-energy tensor derived from the conformal anomaly. An order-reduction procedure is applied to the first order, paying special attention to the conservation of the resulting stress-energy tensor. The results obtained in these different situations are compared between them, and also to recent works in the literature using other approximations for the renormalized stress-energy tensor.

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