Abstract:
Solutions, parametrized by arbitrary functions, of the two-dimensional Einstein equations
are constructed by making a special choice of the determinant of the metric and using
solutions of the attxiliary $O(2,1)$$\sigma$ model. These solutions generalize ones considered
earlier [1]. The construction is also applied to the Einstein–Maxwell equations and to the
case when matter with equation of state $\varepsilon=p$ is present.