activity
19952014
most citedThe Riemannian geometry of orbit spaces. The metric, geodesics, and integrable systems

6 citations · 24 across the 6 of their papers we have counts for

collaborators

6 papers

math.DG2014★ 5 cited

Tanaka structures (non holonomic G-structures) and Cartan connections

Dmitri V. Alekseevsky, Liana David

Let \gh = \gh_{-k}\oplus \cdots \oplus \gh_{l} (k >0, l \geq 0) be a finite dimensional real graded Lie algebra, with a Euclidian metric \langle \cdot , \cdot \rangle adapted to th…

math.DG2001★ 6 cited

The Riemannian geometry of orbit spaces. The metric, geodesics, and integrable systems

Dmitry Alekseevsky, Andreas Kriegl, Mark Losik +1

We investigate the rudiments of Riemannian geometry on orbit spaces for isometric proper actions of Lie groups on Riemannian manifolds. Minimal geodesic arcs are length minim…

math.DG2000

Compact homogeneous CR manifolds

Dmitry V. Alekseevsky, Andrea F. Spiro

We classify all compact simply connected homogeneous CR manifolds of codimension one and with non-degenerate Levi form up to CR equivalence. The classification is based on our…

math.SG1999★ 5 cited

Completely integrable systems: a generalization

Dmitry Alekseevsky, Janusz Grabowksi, Giuseppe Marmo +1

We present a slight generalization of the notion of completely integrable systems to get them being integrable by quadratures. We use this generalization to integrate dynamical sys…

math.DG1999★ 2 cited

Invariant CR Structures on Compact Homogeneous Manifolds

Dmitry V. Alekseevsky, Andrea F. Spiro

An explicit classification of simply connected compact homogeneous CR manifolds G/L of codimension one, with non-degenerate Levi form, is given. There are three classes of such man…

math.RT1995★ 6 cited

Classification of -(super)-extended Poincaré algebras and bilinear invariants of the spinor representation of

Dmitry V. Alekseevsky, Vicente Cortés

We classify extended Poincaré Lie super algebras and Lie algebras of any signature (p,q), that is Lie super algebras and Z_2-graded Lie algebras g = g_0 + g_1, where g_0 = so(V) +…