“…Since the onedimensional distribution span{∇f } is totally geodesic one has that (M, g) decomposes locally as a twisted product of the form I × ϕ N (see [24]). Moreover ρ(e 1 , e i ) = 0 (i = 2, 3, 4) shows that the twisted product reduces to a warped product [19]. Finally, since I × ϕ N is self-dual, it is necessarily locally conformally flat and the fiber N is of constant sectional curvature (see [6]).…”
Section: Basic Formulas and Self-dual Gradient Ricci Solitonsmentioning
confidence: 98%
“…Now, a straightforward calculation shows that the only possibly nonzero components of the Ricci tensor of g D,Φ are given by (19) ρ…”
“…On the other hand, since f is the potential function of a gradient Ricci soliton (i.e., Hes f +ρ = λg D,Φ ), it follows immediately from the expressions of the metric and the Ricci tensor in (18) and (19) that Hes f (∂ x i ′ , ∂ x j ′ ) = 0 for all i, j = 1, 2. Hence the function f expresses as…”
Abstract. We describe the local structure of self-dual gradient Ricci solitons in neutral signature. If the Ricci soliton is non-isotropic then it is locally conformally flat and locally isometric to a warped product of the form I ×ϕ N (c), where N (c) is a space of constant curvature. If the Ricci soliton is isotropic, then it is locally isometric to the cotangent bundle of an affine surface equipped with the Riemannian extension of the connection, and the Ricci soliton is described by the underlying affine structure. This provides examples of self-dual gradient Ricci solitons which are not locally conformally flat.
“…Since the onedimensional distribution span{∇f } is totally geodesic one has that (M, g) decomposes locally as a twisted product of the form I × ϕ N (see [24]). Moreover ρ(e 1 , e i ) = 0 (i = 2, 3, 4) shows that the twisted product reduces to a warped product [19]. Finally, since I × ϕ N is self-dual, it is necessarily locally conformally flat and the fiber N is of constant sectional curvature (see [6]).…”
Section: Basic Formulas and Self-dual Gradient Ricci Solitonsmentioning
confidence: 98%
“…Now, a straightforward calculation shows that the only possibly nonzero components of the Ricci tensor of g D,Φ are given by (19) ρ…”
“…On the other hand, since f is the potential function of a gradient Ricci soliton (i.e., Hes f +ρ = λg D,Φ ), it follows immediately from the expressions of the metric and the Ricci tensor in (18) and (19) that Hes f (∂ x i ′ , ∂ x j ′ ) = 0 for all i, j = 1, 2. Hence the function f expresses as…”
Abstract. We describe the local structure of self-dual gradient Ricci solitons in neutral signature. If the Ricci soliton is non-isotropic then it is locally conformally flat and locally isometric to a warped product of the form I ×ϕ N (c), where N (c) is a space of constant curvature. If the Ricci soliton is isotropic, then it is locally isometric to the cotangent bundle of an affine surface equipped with the Riemannian extension of the connection, and the Ricci soliton is described by the underlying affine structure. This provides examples of self-dual gradient Ricci solitons which are not locally conformally flat.
“…Twisted products were the object of recent investigations [2,4,5,6,11,15]. The reduced L q,p -cohomology of warped cylinders [a, b) × h N , i.e., of product manifolds [a, b) × N endowed with a warped product metric…”
Abstract. Vanishing results for reduced Lp,q-cohomology are established in the case of twisted products, which are a generalization of warped products. Only the case q ≤ p is considered. This is an extension of some results by Gol ′ dshtein, Kuz ′ minov and Shvedov about the Lp-cohomology of warped cylinders. One of the main observations is the vanishing of the "middledimensional" cohomology for a large class of manifolds.Mathematics Subject Classification. 58A10, 58A12.
“…There are also different generalizations of warped products such as warped products with more than one fiber manifold, called multiply warped products (see [35]) or warped products with two warping functions acting symmetrically on the fiber and base manifolds, called doubly warped products (see [34]). Finally, a warped product is said to be a twisted product if the warping function defined on the product of the base and fiber manifolds (see [16]). Basically, a standard static space-time can be considered as a Lorentzian warped product where the warping function is defined on a Riemannian manifold and acting on the negative definite metric on an open interval of real numbers.…”
Essentially, some conditions for the Riemannian factor and the warping function of a standard static space-time are obtained in order to guarantee that no nontrivial warping function on the Riemannian factor can make the standard static space-time Einstein.
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