On the structure equations of the induced linear connections.
On the structure function of a -structure
On the structure of complete Kähler manifolds with nonnegative curvature near infinity.
On the structure of complete Kähler manifolds with nonnegative curvature near infinity (Erratum).
On the structure of convex sets with applications to the moduli of spherical minimal immersions.
On the Structure of Cut Loci in Compact Riemannian Symmetrie Spaces.
On the Structure of Manifolds with positive Scalar Curvature.
On the structure of Riemannian manifolds of almost nonnegative Ricci curvature.
On the structure vector field of a real hypersurface in complex two-plane Grassmannians
Considering the notion of Jacobi type vector fields for a real hypersurface in a complex two-plane Grassmannian, we prove that if a structure vector field is of Jacobi type it is Killing. As a consequence we classify real hypersurfaces whose structure vector field is of Jacobi type.
On the Structures of Positively Curved Manifolds with Certain Diameter.
On the subanalyticity of Carnot–Caratheodory distances
On the Sum of the Hermitian Scalar Curvatures of a Compact Hermitian Manifold.
On the Symplectic Structure of Coadjoint Orbits of (Solvable) Lie Groups and Applications. I.
On the tangency of sets in generalized metric spaces
On the tangency of sets in generalized metric spaces for certain functions of the class
On the tangent space to the universal Teichmüller space.
On the tangential velocity arising in a crystalline approximation of evolving plane curves
In a crystalline algorithm, a tangential velocity is used implicitly. In this short note, it is specified for the case of evolving plane curves, and is characterized by using the intrinsic heat equation.
On the three-dimensional CR-submanifolds of the six-dimensional sphere.
On the topological charge conservation in the three-dimensional -model.
A field of three-component unit vectors on the dimensional spacetime is considered. Two field configurations with different values of the topological charge cannot be connected by the path of field configurations with a finite Euclidean action. Therefore there is no transition between them. The initial and final configurations are assumed to be continuous at infinity. The asymptotic behaviour of intermediate configurations may be arbitrary. The proof is based on the properties of the degree of...
On the topological invariance of the basic cohomology.