11 research outputs found
Four-dimensional Riemannian manifolds with two circulant structures
We consider a class (M, g, q) of four-dimensional Riemannian manifolds M,
where besides the metric g there is an additional structure q, whose fourth
power is the unit matrix. We use the existence of a local coordinate system
such that there the coordinates of g and q are circulant matrices. In this
system q has constant coordinates and q is an isometry with respect to g. By
the special identity for the curvature tensor R generated by the Riemannian
connection of g we define a subclass of (M, g, q). For any (M, g, q) in this
subclass we get some assertions for the sectional curvatures of two-planes. We
get the necessary and sufficient condition for g such that q is parallel with
respect to the Riemannian connection of g
Almost Conformal Transformation in a Class of Riemannian Manifolds
We consider a 3-dimensional Riemannian manifold V with a
metric g and an aΒ±nor structure q. The local coordinates of these tensors are
circulant matrices. In V we define an almost conformal transformation. Using
that definition we construct an infinite series of circulant metrics which are
successively almost conformaly related. In this case we get some properties
SPHERES AND CIRCLES WITH RESPECT TO AN INDEFINITE METRIC ON A RIEMANNIAN MANIFOLD WITH A SKEW-CIRCULANT STRUCTURE
We study hyper-spheres, spheres and circles, with respect to an indefinite metric, in a single tangent space on a 4-dimensional differentiable manifold. The manifold is equipped with a positive definite metric and an additional tensor structure of type (1, 1). The fourth power of the additional structure is minus identity and its components form a skew-circulant matrix in some local coordinate system. The both structures are compatible and they determine an associated indefinite metric on the manifold
ΠΡΡΡ Ρ Π°ΡΠΈΠ½Π½ΠΈ ΡΠ²ΡΡΠ·Π°Π½ΠΎΡΡΠΈ Π² ΡΠΈΠΌΠ°Π½ΠΎΠ²ΠΎ ΠΌΠ½ΠΎΠ³ΠΎΠΎΠ±ΡΠ°Π·ΠΈΠ΅ Ρ ΡΠΈΡΠΊΡΠ»Π°Π½ΡΠ½Π° ΠΌΠ΅ΡΡΠΈΠΊΠ° ΠΈ Π΄Π²Π΅ ΡΠΈΡΠΊΡΠ»Π°Π½ΡΠ½ΠΈ Π°ΡΠΈΠ½ΠΎΡΠ½ΠΈ ΡΡΡΡΠΊΡΡΡΠΈ
ΠΠ²Π° Π . ΠΠΎΠΊΡΠ·ΠΎΠ²Π°, ΠΠΈΠΌΠΈΡΡΡ Π . Π Π°Π·ΠΏΠΎΠΏΠΎΠ² - Π Π½Π°ΡΡΠΎΡΡΠ°ΡΠ° ΡΡΠ°ΡΠΈΡ Π΅ ΡΠ°Π·Π³Π»Π΅Π΄Π°Π½ ΠΊΠ»Π°Ρ V ΠΎΡΡΡΠΈΠΌΠ΅ΡΠ½ΠΈ ΡΠΈΠΌΠ°Π½ΠΎΠ²ΠΈ ΠΌΠ½ΠΎΠ³ΠΎΠΎΠ±ΡΠ°Π·ΠΈΡ M Ρ ΠΌΠ΅ΡΡΠΈΠΊΠ° g ΠΈ Π΄Π²Π° Π°ΡΠΈΠ½ΠΎΡΠ½ΠΈ ΡΠ΅Π½Π·ΠΎΡΠ° q ΠΈ S. ΠΠ΅ΡΠΈΠ½ΠΈΡΠ°Π½Π° Π΅ ΠΈ Π΄ΡΡΠ³Π° ΠΌΠ΅ΡΡΠΈΠΊΠ° Β―g
Π² M. ΠΠΎΠΊΠ°Π»Π½ΠΈΡΠ΅ ΠΊΠΎΠΎΡΠ΄ΠΈΠ½Π°ΡΠΈ Π½Π° Π²ΡΠΈΡΠΊΠΈ ΡΠ΅Π·ΠΈ ΡΠ΅Π½Π·ΠΎΡΠΈ ΡΠ° ΡΠΈΡΠΊΡΠ»Π°Π½ΡΠ½ΠΈ ΠΌΠ°ΡΡΠΈΡΠΈ.
ΠΠ°ΠΌΠ΅ΡΠ΅Π½ΠΈ ΡΠ°: 1) Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡ ΠΌΠ΅ΠΆΠ΄Ρ ΡΠ΅Π½Π·ΠΎΡΠ° Π½Π° ΠΊΡΠΈΠ²ΠΈΠ½Π° R ΠΏΠΎΡΠΎΠ΄Π΅Π½ ΠΎΡ g ΠΈ ΡΠ΅Π½Π·ΠΎΡΠ°
Π½Π° ΠΊΡΠΈΠ²ΠΈΠ½Π° Β―R ΠΏΠΎΡΠΎΠ΄Π΅Π½ ΠΎΡ Β―g; 2) ΡΡΠΆΠ΄Π΅ΡΡΠ²ΠΎ Π·Π° ΡΠ΅Π½Π·ΠΎΡΠ° Π½Π° ΠΊΡΠΈΠ²ΠΈΠ½Π° R Π² ΡΠ»ΡΡΠ°Ρ,
ΠΊΠΎΠ³Π°ΡΠΎ ΡΠ΅Π½Π·ΠΎΡΡΡ Π½Π° ΠΊΡΠΈΠ²ΠΈΠ½Π° Β―R ΡΠ΅ Π°Π½ΡΠ»ΠΈΡΠ°; 3) Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡ ΠΌΠ΅ΠΆΠ΄Ρ ΡΠ΅ΠΊΡΠΈΠΎΠ½Π½Π°ΡΠ°
ΠΊΡΠΈΠ²ΠΈΠ½Π° Π½Π° ΠΏΡΠΎΠ·Π²ΠΎΠ»Π½Π° Π΄Π²ΡΠΌΠ΅ΡΠ½Π° q-ΠΏΠ»ΠΎΡΠ°Π΄ΠΊΠ° {x, qx} ΠΈ ΡΠΊΠ°Π»Π°ΡΠ½Π°ΡΠ° ΠΊΡΠΈΠ²ΠΈΠ½Π° Π½Π° M.In the present paper it is considered a class V of 3-dimensional Riemannian manifolds
M with a metric g and two affinor tensors q and S. It is defined another metric Β―g in
M. The local coordinates of all these tensors are circulant matrices. It is found: 1)
a relation between curvature tensors R and Β―R of g and Β―g, respectively; 2) an identity
of the curvature tensor R of g in the case when the curvature tensor Β―R vanishes; 3)
a relation between the sectional curvature of a 2-section of the type {x, qx} and the
scalar curvature of M. *2000 Mathematics Subject Classification: 53C15, 53B20.This work is partially supported by project RS09 - FMI - 003 of the Scientific Research Fund, Paisii
Hilendarski University of Plovdiv, Bulgaria