sigma07-094. 338KB Jun 04 2011 12:10:07 AM
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![Fig. 1], or just look at the exponents of (−1) in the formula). At fixed x, orbits n and −(n + 1)do not have the same length, but when integrated over x those two sets of orbits collectively](https://thumb-ap.123doks.com/thumbv2/123dok/1159612.899670/12.612.118.460.415.556/exponents-formula-fixed-orbits-length-integrated-orbits-collectively.webp)
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(Note that in this case, as long as all the integer initial data are non-zero, then the coefficient J which appears in (2.25) is uniquely determined, and J ∈ Q .) This can be seen as
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In theoretical physics Gauss–Bonnet curvatures are known as a Lagrangian of pure Lovelock gravity, Gauss–Bonnet gravity or Lanczos gravity. the integer part of one half the
We briefly review the concepts of generalized zero curvature conditions and inte- grability in higher dimensions, where integrability in this context is related to the existence
