文摘
We characterize the circular periodic solutions of the generalized Lennard-Jones Hamiltonian system with two particles in \(\mathbb {R}^n\), and we analyze what of these periodic solutions can be continued to periodic solutions of the anisotropic generalized Lennard-Jones Hamiltonian system. We also characterize the periods of antiperiodic solutions of the generalized Lennard-Jones Hamiltonian system on \(\mathbb {R}^{2n}\), and prove the existences of \(0<\tau ^{*}\le \tau ^{**}\) such that this system possesses no \(\tau /2\)-antiperiodic solution for all \(\tau \in (0,\tau ^{*})\), at least one \(\tau /2\)-antiperiodic solution when \(\tau =\tau ^{*}\), precisely \(2^n\) families of \(\tau /2\)-antiperiodic circular solutions when \(\tau =\tau ^{**}\), and precisely \(2^{n+1}\) families of \(\tau /2\)-antiperiodic circular solutions when \(\tau >\tau ^{**}\). Each of these circular solution families is of dimension \(n-1\) module the \(S^1\)-action. Keywords Lennard-Jones potential Circular periodic solutions Anisotropic Lennard-Jones potential