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From aptm@kharkov.ua Tue Jan 25 15:15:00 2000
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Message-ID: <001901bf672a$829d56a0$03032cc2@kharkov.ua>
From: "O.B.Zaslavskii"
To:
Subject: black holes
Date: Mon, 24 Jan 2000 22:54:32 +0200
Organization: The Tarielle Station
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Please find enclosed the attached file with the abstract of my talk which I
suggest for the colloquium on black holes (3 March). It is based on my two
recent papers hep-th/9911077 (Phys. Rev. D, in press) and hep-th/ 0001090
(accepted in Phys. Lett. B).
I would greatly appreciate you for financial support including travel since
in our situation any support (and even salary) are now absent in our Kharkov
University, so such a support is the only chance for me to participate in
the meeting.
Sincerely,
Oleg Zaslavskii,
Department of Physics, Kharkov Karazin's National university, Svoboda Square
4, Kharkov 61077, Ukraine

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\begin{document}
\draft
\author{O. B. Zaslavskii}
\address{Department of Physics, Kharkov Karazin's National University, =
Svoboda Sq.4,\\
Kharkov\\
61077, Ukraine\\
E-mail: aptm@kharkov.ua}
\title{Dilaton gravity and black holes with finite curvature at the =
horizon away
from the Hawking temperature}
\maketitle

\begin{abstract}
% insert abstract here
\end{abstract}

\pacs{}

%\date{\today}

It is shown that static solutions with a finite curvature at the horizon =
may
exist in dilaton gravity at temperatures $T\neq T_{H}$ (including =
$T=3D0$)
where $T_{H}\,$is the Hawking temperature. Hawking radiation is absent =
and
the state of a system represents thermal excitation over the Boulware
vacuum. The horizon remains unattainable for an observer because of the
thermal divergences in the stress-energy of quantum fields there. =
However,
the curvature at the horizon is finite, when measured from outside, =
since
these divergences are compensated by those in the gradients of the =
dilaton
field. The Spacetimes under consideration are geodesically incomplete =
and
the coupling between the dilaton and gravity diverges at the horizon, so =
we
have a ''singularity without singularity''.

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\end{document}

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