Abstract

We construct the Killing(-Yano) tensors for a large class of charged black holes in higher dimensions and study general properties of such tensors, in particular, their behavior under string dualities. Killing(-Yano) tensors encode the symmetries beyond isometries, which lead to insights into dynamics of particles and fields on a given geometry by providing a set of conserved quantities. By analyzing the eigenvalues of the Killing tensor, we provide a prescription for constructing several conserved quantities starting from a single object, and we demonstrate that Killing tensors in higher dimensions are always associated with ellipsoidal coordinates. We also determine the transformations of the Killing(-Yano) tensors under string dualities, and find the unique modification of the Killing-Yano equation consistent with these symmetries. These results are used to construct the explicit form of the Killing(-Yano) tensors for the Myers-Perry black hole in arbitrary number of dimensions and for its charged version.

Highlights

  • Introduction and summarySymmetries of dynamical equations have always played very important role in string theory

  • Since the mKYT equation is written in the string frame, S duality induces a conformal rescaling of such metric, so generically the modified Killing-Yano tensor is destroyed by such operation

  • We have demonstrated that nontrivial Killing tensors in arbitrary number of dimensions are always associated with ellipsoidal coordinates, and we used this observation to construct the Killing(-Yano) tensors for the Myers-Perry black hole ((3.20), (3.30), (3.31)), its charged version (5.3)–(5.4), and for several examples of F1-NS5 geometries ((5.15), (5.19)–(5.21))

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Summary

Introduction and summary

Symmetries of dynamical equations have always played very important role in string theory. Since at low energies strings behave as point particles, integrability must survive as a hidden symmetry of such objects, and this gives a very coarse necessary condition for integrability, which can be tested for large classes of backgrounds This condition was sufficient for ruling out integrability on all known supersymmetric geometries produced by D-branes, with an exception of AdSp×Sq and a couple of other examples [19]. Over the last four decades Killing(-Yano) tensors have been found for other geometries both in general relativity [40,41,42,43,44] and in string theory [45, 46], and in this article we will construct KYT for a large class geometries in arbitrary numbers of dimensions, which contains most of the known examples as special cases.

Killing tensors and Killing-Yano tensors
Killing tensors from the Hamilton-Jacobi equation
Separation of variables from Killing tensor
Killing-Yano tensors of various ranks
Example
Killing vectors and T duality
Killing vectors commuting with T duality direction
Killing vectors with z dependence
Conformal Killing Vectors and T duality
Killing tensors in the NS sector
Conditions on the B field from dimensional reduction
Conditions on the B field from separation of variables
T duality and the modified Killing-Yano equation
Examples of the modified KYT for F1-NS5 system
Charged Myers-Perry black hole
A N dxM dxN e2r e2y
F1-NS5 system from the five-dimensional black hole
Conformal Killing-Yano tensors
Discussion
A Conformal transformations of Killing tensors
Ellipsoidal coordinates from Killing tensors
Next we look at
Ellipsoidal coordinates in flat space
C Principal CKYT for the Myers-Perry black hole
Full Text
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