arXiv subjects
Publications and source records attributed to Stanislav Hronek.
We study properties of pseudo-Riemannian metrics corresponding to Monge-Ampère structures on four-dimensional $T^*M$. We describe a family of Ricci flat solutions, which are parametrized by six coefficients satisfying the Plücker embedding equation. We also focus on pullbacks of the pseudo-metrics on two-dimensional $M$ and describe the corresponding Hessian structures.
It is known that the order $α'$ correction to the tree-level effective action for the bosonic and heterotic string can be described in the framework of Double Field Theory (DFT). Here we determine the DFT action and transformations at order $α'^2$ by a direct calculation. The result is vastly simpler than previous proposals. We show that this correction reproduces the known $α'^2$ correction to the heterotic string effective action. The relation of our action to an (implicit) all order proposal coming from the so-called generalized Bergshoeff-de Roo identification is also discussed.
It has been shown by Marques and Nunez that the first $α'$-correction to the bosonic and heterotic string can be captured in the $O(D,D)$ covariant formalism of Double Field Theory via a certain two-parameter deformation of the double Lorentz transformations. This deformation in turn leads to an infinite tower of $α'$-corrections and it has been suggested that they can be captured by a generalization of the Bergshoeff-de Roo identification between Lorentz and gauge degrees of freedom in an extended DFT formalism. Here we provide strong evidence that this indeed gives the correct $α'^2$-corrections to the bosonic and heterotic string by showing that it leads to a cubic Riemann term for the former but not for the latter, in agreement with the known structure of these corrections including the coefficient of Riemann cubed.
Double Field Theory (DFT) is an attempt to make the O(d,d) T-duality symmetry of string theory manifest, already before reducing on a d-torus. It is known that supergravity can be formulated in an O(D,D) covariant way, and remarkably this remains true to the first order in $α'$. We set up a systematic way to analyze O(D,D) invariants, working order by order in fields, which we carry out up to order $α'^3$. At order $α'$ we recover the known Riemann squared invariant, while at order $α'^2$ we find no independent invariant. This is compatible with the $α'$ expansion in string theory. However, at order $α'^3$ we show that there is again no O(D,D) invariant, in contradiction to the fact that all string theories have a quartic Riemann invariant with coefficient proportional to $ζ(3)$. We conclude that DFT and similar frameworks cannot capture the full $α'$ expansion in string theory.
We consider so-called Yang-Baxter deformations of bosonic string sigma-models, based on an $R$-matrix solving the (modified) classical Yang-Baxter equation. It is known that a unimodularity condition on $R$ is sufficient for Weyl invariance at least to two loops (first order in $α'$). Here we ask what the necessary condition is. We find that in cases where the matrix $(G+B)_{mn}$, constructed from the metric and $B$-field of the undeformed background, is degenerate the unimodularity condition arising at one loop can be replaced by weaker conditions. We further show that for non-unimodular deformations satisfying the one-loop conditions the Weyl invariance extends at least to two loops (first order in $α'$). The calculations are simplified by working in an $O(D,D)$-covariant doubled formulation.
In this paper, we study the relation between geodesic and harmonic mappings. Harmonic mappings are defined between Riemannian manifolds as critical points of the energy functional, on the other hand, geodesic mappings are defined in a more general setting (manifolds with affine connections). Using the well-established formalism of calculus of variations on fibred manifolds we solve the weak inverse problem for the equation of geodesic mappings and get a variational equation which is a consequence of the geodesic mappings equation. For the connection on the target manifold we get the expected result, that it is a metric connection. However, we find that the connection on the source manifold need not be metric. The interesting result is that the metric which induces the connection on the target manifold can change between fibres and these changes are related to the connection on the source manifold. These results hint onto a possibility for a more general structure on the fibred manifold, than usually assumed.