dongo
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Suppose you are given a Killing field [itex]\xi[/itex] on a manifold [itex](M, g)[/itex]. We can associate to this vector field a 1-form via the metric. Denote this 1-form by [itex]\eta[/itex]. Show that the codifferential of the 1-form vanishes, i.e., [itex]\delta\eta = 0.[/itex]
As far as I know, a Killing field is a vector field on a manifold whose local flow consists of local isometries. The more pragmatic to check wether [itex]\eta[/itex] is Killing or not is to calculate the Live derivate of the metric of the manifold with respect to the vector field in question. It has to be zero, i.e. [itex]L_{\eta}(g) = 0[/itex]. The codifferential of the usual differential operator is defined as the formally adjoint operator to the differential, where one can explicitly calculate it to be [itex]\delta = (-1)^{nk}\ast d \ast = -\sum_{i=1}^{n}\iota_{e_{i}}\nabla_{e_i}[/itex]. Here, [itex]n = dim(M)[/itex] and the [itex]e_{i}[/itex] form an orthonormal basis with respect to the metric [itex]g[/itex]. The codifferential acts on the space of k + 1 -forms and sends them to k - forms (on M), i.e., [itex]\delta : \Omega^{k+1} \rightarrow \Omega^{k}.[/itex][itex] <br /> <br /> <br /> <b>Since the question arose in a book on Kähler geometry, more precisely in asection where holomorphic vector field on Kähler-Einstein manifolds, I assume, it suffices to treat this case. However, in the general case, we know that the 1-form, associated to a real holomorphic vector field, can be (some sort of) hodge decomposed in three parts, namely [itex]/ix = dh + d^{c}f + /ix^{H}[/itex] where the first term on the right-hand side involves the usual differential. the second is the twisted differential, i.e., [itex]d^{c}=[itex]\sum_{i=1}^{n}Je_{i}\wedge \nable_{e_{i}}[/itex], and the last component is the harmonic part. Since we deal with a Kähler manifolds, and we know, that Killing fields are (real) holomorphic, we can use that the Laplace-operator on M is equal to: [itex]\Delta = 2\Delta^{\bar{\partial}}[/itex]. Note that this is only the case on Kähler-manifolds. And this is basically the point from which on I ahve no clue any longer. I'd appreciate hints rather solutions as I would ultimately like to come (with a little help of course) to a solution on my own.[/itex]</b>[itex] <br /> By the way, this is my first post, so if you have any recommendations concerning typesetting etc. you're welcome to utter them. Especially TEX help would be valuable because I have almost no experinece when it comes to that.<br /> <br /> <br /> dongo[/itex][/itex]
As far as I know, a Killing field is a vector field on a manifold whose local flow consists of local isometries. The more pragmatic to check wether [itex]\eta[/itex] is Killing or not is to calculate the Live derivate of the metric of the manifold with respect to the vector field in question. It has to be zero, i.e. [itex]L_{\eta}(g) = 0[/itex]. The codifferential of the usual differential operator is defined as the formally adjoint operator to the differential, where one can explicitly calculate it to be [itex]\delta = (-1)^{nk}\ast d \ast = -\sum_{i=1}^{n}\iota_{e_{i}}\nabla_{e_i}[/itex]. Here, [itex]n = dim(M)[/itex] and the [itex]e_{i}[/itex] form an orthonormal basis with respect to the metric [itex]g[/itex]. The codifferential acts on the space of k + 1 -forms and sends them to k - forms (on M), i.e., [itex]\delta : \Omega^{k+1} \rightarrow \Omega^{k}.[/itex][itex] <br /> <br /> <br /> <b>Since the question arose in a book on Kähler geometry, more precisely in asection where holomorphic vector field on Kähler-Einstein manifolds, I assume, it suffices to treat this case. However, in the general case, we know that the 1-form, associated to a real holomorphic vector field, can be (some sort of) hodge decomposed in three parts, namely [itex]/ix = dh + d^{c}f + /ix^{H}[/itex] where the first term on the right-hand side involves the usual differential. the second is the twisted differential, i.e., [itex]d^{c}=[itex]\sum_{i=1}^{n}Je_{i}\wedge \nable_{e_{i}}[/itex], and the last component is the harmonic part. Since we deal with a Kähler manifolds, and we know, that Killing fields are (real) holomorphic, we can use that the Laplace-operator on M is equal to: [itex]\Delta = 2\Delta^{\bar{\partial}}[/itex]. Note that this is only the case on Kähler-manifolds. And this is basically the point from which on I ahve no clue any longer. I'd appreciate hints rather solutions as I would ultimately like to come (with a little help of course) to a solution on my own.[/itex]</b>[itex] <br /> By the way, this is my first post, so if you have any recommendations concerning typesetting etc. you're welcome to utter them. Especially TEX help would be valuable because I have almost no experinece when it comes to that.<br /> <br /> <br /> dongo[/itex][/itex]