Among all irreducible
symmetric spaces [Br57], we prove that there are not many candidates for irreducible
symmetric spaces G/H that admit standard compact Clifford Klein forms other than those listed in Theorem 1.7.
The transition from two-coordinate vectors in
symmetric coordinates to three-coordinate complex vectors in phase coordinates is carried out by multiplying on the matrix [F.sub.0] - [parallel][[bar.e].sub.+] [[bar.e].sub.-][parallel].
The presented cylindrically
symmetric spacetime (1) is conformally flat since the Weyl tensor vanishes, that is, [C.sub.[mu][nu][rho][sigma]] = 0, and static.
In this paper, we find homotheties of a class of the spherically
symmetric space-time (5) admitting [G.sub.3] = SO(3) as the maximal isometry group for x(t, r) =2 ln r, imposing no restriction on the stress-energy tensor.
Solution 4: The following is the fourth solution which has the maximum Noether symmetries for the plane
symmetric static conformal Minkowski spacetime
K., On pseudo cyclic Ricci
symmetric manifolds admitting semi-symmetric connection, Scientia, series A : Math.
Table 2 showed 67.2% (119 casts) had
symmetric canine relationship and 32.8% (58 casts) had asymmetric canine relationship.
3.1.1 The O(2)
symmetric positive solution branch by [lambda] continuation
It is well known (see [7-9]) that (1) over F has a
symmetric solution if and only if the equation AX = B has a solution and [AB.sup.T] = [BA.sup.T].
It follows from the previous lemma that one can find a Banach space X and a closed subspace H of X such that X is not weakly
symmetric with respect to H.