A reflecting symmetry q → −q of a Hamiltonian system does not leave the symplectic structure dq ∧ d p invariant and is therefore usually associated with a reversible Hamiltonian system. However, if q → −q leads to H → −H, then the equations of motion are invariant under the reflection. Such a symmetry imposes strong restrictions on equilibria with q = 0. We study the possible bifurcations triggered by a zero eigenvalue and describe the simplest bifurcation triggered by non-zero eigenvalues on the imaginary axis.
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